The CS110 ELECTRIC FIELD METER (CS110) is warranted by CAMPBELL
SCIENTIFIC, LTD. to be free from defects in materials and workmanship under
normal use and service for twelve (12) months from date of shipment unless
specified otherwise. Batteries have no warranty. CAMPBELL SCIENTIFIC
LTD’S obligation under this warranty is limited to repairing or replacing (at
CAMPBELL SCIENTIFIC LTD’S option) defective products. The customer shall
assume all costs of removing, reinstalling, and shipping defective products to
CAMPBELL SCIENTIFIC, LTD. CAMPBELL SCIENTIFIC, LTD. will return
such products by surface carrier prepaid. This warranty shall not apply to any
CAMPBELL SCIENTIFIC, LTD. products which have been subjected to
modification, misuse, neglect, accidents of nature, lack of maintenance or shipping
damage. This warranty is in lieu of all other warranties, expressed or implied,
including warranties of merchantability or fitness for a particular purpose.
CAMPBELL SCIENTIFIC, LTD. is not liable for special, indirect, incidental or
consequential damages from the use, failure or malfunction of the CS110. In no
event will CAMPBELL SCIENTIFIC, LTD. have liability in excess of the
purchase price for the CS110. CAMPBELL SCIENTIFIC, LTD. does not warrant
that the CS110 will meet customer’s requirements or that its operation will be
uninterrupted or error-free. Atmospheric or local electric field conditions or
different site characteristics may cause false information, late data, or otherwise
incomplete or inaccurate data. The CS110 only measures conditions that make
lightning more likely. Just as with weather forecasts, the CS110 measurements
only help assess the probability of lightning. Lightning can occur causing personal
injury, even death, or damage to property without any warning from the CS110.
Please inform us before returning equipment and obtain a Repair Reference
Number whether the repair is under guarantee or not. Please state the faults as
clearly as possible, and if the product is out of the guarantee period it should be
accompanied by a purchase order. Quotations for repairs can be given on request.
When returning equipment, the Repair Reference Number must be clearly marked
on the outside of the package.
Note that goods sent air freight are subject to Customs clearance fees which
Campbell Scientific will charge to customers. In many cases, these charges are
greater than the cost of the repair.
Campbell Scientific Ltd,
Campbell Park, 80 Hathern Road,
Shepshed, Loughborough, LE12 9GX, UK
Tel: +44 (0) 1509 601141
Fax: +44 (0) 1509 601091
Email: support@campbellsci.co.uk
www.campbellsci.co.uk
PLEASE READ FIRST
About this manual
Please note that this manual was originally produced by Campbell Scientific Inc. primarily for the
North American market. Some spellings, weights and measures may reflect this origin.
Some useful conversion factors:
2
Area: 1 in
Length: 1 in. (inch) = 25.4 mm
1 ft (foot) = 304.8 mm
1 yard = 0.914 m
1 mile = 1.609 km
In addition, while most of the information in the manual is correct for all countries, certain information
is specific to the North American market and so may not be applicable to European users.
Differences include the U.S standard external power supply det ails where some information (for
example the AC transformer input voltage) will not be applicable for British/European use. Please
note, however, that when a power supply adapter is ordered it will be suitable for use in your country.
Reference to some radio transmitters, digital cell phones and aerials may also not be applicabl e
according to your locality.
(square inch) = 645 mm2
Mass: 1 oz. (ounce) = 28.35 g 1 lb (pound weight) = 0.454 kg
Pressure: 1 psi (lb/in
Volume: 1 UK pint = 568.3 ml
1 UK gallon = 4.546 litres
1 US gallon = 3.785 litres
2
) = 68.95 mb
Some brackets, shields and enclosure options, including wiring, are not sold as standard items in the
European market; in some cases alter n a tiv es are offered. Details of the alt ernatives will be covered in
separate manuals.
Part numbers prefixed with a “#” symbol are special order parts for use with non-EU variants or for
special installations. Please quote the full part number with the # when ordering.
Recycling information
At the end of this product’s life it should not be put in commercial or domestic refuse
but sent for recycling. Any batteries contai ned within the product or used during the
products life should be removed from the product and also be sent to an appropriate
recycling facility.
Campbell Scientific Ltd can advise on the recycling of the equipment and in some cases
arrange collection and the correct disposal of it, although charges may apply for some
items or territories.
For further advice or support, please contact Campbell Scientific Ltd, or your local agent.
Campbell Scientific Ltd, Campbell Park, 80 Hathern Road, Shepshed, Loughborough, LE12 9GX, UK
Tel: +44 (0) 1509 601141 Fax: +44 (0) 1509 601091
Email: support@campbellsci.co.uk
www.campbellsci.co.uk
Contents
PDF viewers note: These page numbers refer to the printed version of this document. Use
the Adobe Acrobat® bookmarks tab for links to specific sections.
1. General Description .................................................... 1
G-4. Determination of Csite ...................................................................... G-5
H-1. Tripod CS110 and StrikeGuard ......................................................... H-1
H-2. CS110 and StrikeGuard on Tripod Mast ........................................... H-2
H-3. Grounding the CS110 Grounding Strap ............................................ H-3
H-4. Grounding the Tripod and Battery .................................................... H-4
H-5. Connections for Combined System ................................................... H-5
H-6. Determination of Csite ...................................................................... H-6
iii
This is a blank page.
iv
CS110 Electric Field Meter
1. General Description
1.1 CS110 Introduction
Atmospheric electric fields have been measured for decades by electric field
meters nicknamed “field mills”. Traditional field mills employ a spinning metal
rotor (vane) electrically connected to Earth ground, placed between the external
field and stationary metal sense electrodes. The grounded spinning rotor
alternately shields and exposes the sense electrodes from the electric field to be
measured, resulting in a modulation of the induced charge on the sense electrodes.
Typically, a pair of charge amplifiers converts the modulated charge into AC
voltages that are synchronously rectified and filtered to form a low-frequency
voltage proportional to the low-frequency (≤10 Hz) electric field.
Ground Strap
Case Lid
Reciprocating Shutter
Figure 1. CS110 Electric Field Meter
Unlike traditional rotating vane field mills, the CS110 uses a reciprocating shutter.
A stepper motor opens and then closes the reciprocating shutter by 45° during
measurements. The reciprocating shutter is electrically connected to ground
potential by a flexible stainless-steel strap operated below its fatigue limit,
resulting in an ultra-reliable electrical ground connection. The CS110 offers
improved dc error performance, as compared with traditional rotating vane field
Sealed Connectors
Stator
1
CS110 Electric Field Meter
1.2 CR1000 Datalogger
1.3 Meteorological Inputs
1.4 Communication and Data Storage
mills, by utilizing a zero field (closed shutter) reference for each measurement.
Power consumption is also reduced (< 1 Watt for 1 measurement per second) in
the CS110 by de-energizing the motor coils in between measurements.
The CS110 contains an embedded CR1000 datalogger, which provides
measurement and control functions, data processing and storage, a user interface
language (CRBasic™), and flexible communications options. LoggerNet™ PC
software (purchased separately) provides versatile networking and data collection
capabilities. For more details on the CR1000 datalogger see the CR1000
Measurement and Control System Operator’s Manual.
The CS110 interfaces to various meteorological sensors resulting in an automated
weather station that includes atmospheric electric field. Wind speed and direction,
air temperature and relative humidity, rainfall, solar radiation or barometric
pressure sensors interface directly to the CS110. Measurement details of the
various sensors are given in section 7.
The circular RS-232 connector on the underside of the CS110 can be used to
interface directly to RS-232 devices (DTE or DCE), utilizing the CS110
RS-232 cable (CS110CBL1).
The circular CS I/O connector on the underside of the CS110 can be used to
interface directly to various Campbell Scientific peripherals, utilizing the CS110
CS I/O cable (CS110CBL2). Examples of CS I/O peripherals include the CR1000
Keyboard Display and the COM220 phone modem.
The DB9 end of CS110 RS-232 cable and CS110 CS I/O cable won’t fit through the
conduit used on some enclosures, whereas the smaller circular end that connects to
the CS110 will.
The embedded CR1000 will have either 2 MB (PN: 006740) or 4 MB (PN:
006741) of battery-backed SRAM and 16K Flash EEPROM. The operating
system and user programs are stored in Flash EEPROM. Memory not used by the
operating system and user program is available for data storage. The size of
available memory can be seen in the Status Table discussed in Appendix A of the
CR1000 manual.
2
1.5 Digital I/O
Three general purpose 0 to 5 V digital I/O lines are available on the CS110 Power
cable (CS110CBL3) that attaches to the circular power connector on the underside
of the CS110. The blue, yellow, and green wires connect to control ports C1, C2,
and C3 respectively. Using CRBasic, these digital I/O lines can be used to
conditionally turn on alarms, provide an interrupt or pulsed signal to be measured
by the CS110, or as a serial communication port.
1.6 Self-Check Features
The CS110 has been designed to provide reliable electric field measurements and
to minimize and simplify maintenance. The CS110 incorporates extensive selfchecking for each measurement in an effort to identify measurement problems and
reduce or eliminate scheduled maintenance. The status code returned from each
electric field measurement reports on instrument health along with any
measurement problems as described in Appendix A.
For example, insulator leakage current is measured during each electric field
measurement, indicating the cleanliness of electrode insulators. A leakage current
compensation circuit for the charge amplifier input is incorporated in the CS110 to
minimize the effects of insulator leakage current on measured results (Patent
pending). A status code indicating excessive leakage current is returned if the
measured input leakage current exceeds the compensation range due to insulator
cleanliness problems.
Instruction Manual
A relative humidity sensor is included inside the CS110 case to provide
information on when case desiccant should be changed. The CS110 also provides
measurement of the battery input voltage in order to monitor the input power to
the instrument. Section 7 discusses CS110 electric field measurement details.
CS110 maintenance details are discussed in Section 10.
3
CS110 Electric Field Meter
2. CS110 Specifications
Electric Field Measurement Performance:
Accuracy
Parallel-Plate Configuration
±1% of reading + 60 V m
-1
offset
1
Measurement
3
Range
(V m-1)
Resolution
(V m-1)
Sensitivity
(µV/V m-1)
Noise
(V m-1
RMS)
±(0 to 21,000) 3 12 4.0
±(21,000 to 212,000) 30 118 18.0
2 m CM10 Tripod Configuration2
-1
1
offset
Noise
(V m-1
RMS)
Accuracy
Measurement
3
(V m-1)
Range
±5% of reading + 8 V m
Resolution
(V m-1)
Sensitivity
(µV/V m-1)
±(0 to 2,200) 0.32 1.2 0.42
±(2,200 to 22,300) 3.2 13 1.9
1
Typical offset for clean electrodes is ≤ |30 V m-1| for the
parallel-plate configuration, which is reduced by the field
enhancement factor for typical inverted and elevated mounting
configurations.
2
Field enhancement due to typical inverted and elevated
mounting requires additional site correction, estimated at ±5%
accuracy when done in appropriate high field conditions.
Practical outdoor CS110 electric field measurement accuracy is
estimated at ±5% of reading + 8 V m
-1
for the CS110 2 metre
CM10 Tripod Site.
4
3
The CS110 incorporates automatic gain ranging between two
input ranges. The measurement is first tried on the lowest input
range. If the signal is too large for the lowest range, the larger
range is used.
Standard Mounting: 2 m height on a CM10 tripod mast
Site Correction: Site correction factors available for several standard mounting
configurations
Sample (Measurement) Rate: Programmable sample rate up to 5 samples per
second, variable sample rates possible. Variable example: sample every 10
seconds until field exceeds threshold then sample once a second until field
returns to normal.
Instruction Manual
Power Requirements: 11 to 16 Vdc; peak-current demand is 750 mA during
motor operation.
7 mA @ 12 V = 0.08 W average power consumption at 1 sample
per 10 seconds
60 mA @ 12 V = 0.7 W average power consumption at 1 sample
per second
120 mA @ 12 V = 1.4 W average power consumption at 2 samples
per second
300 mA @ 12 V = 3.6 W average power consumption at 5 samples
per second
Communication: 1 RS-232 port; 1 CS I/O port used to interface with our
peripherals such as a COM320 Voice Modem; digital control ports 1, 2, and
3 for alarm, SDI-12 communications, or asynchronous communications
Baud Rates: Selectable from 300 to 115,200 bps
ASCII Protocol: one start bit, one stop bit, eight data bits, no parity
Lightning Protection: Multi-stage transient protection on all external interfaces
CE Compliance: Standards to which conformity is declared—BS EN61326:2002
data processing and storage options and setting output ports based on alarm
conditions. LoggerNet
programming allows the selection of sample rate,
TM
includes the CRBasic editor and compiler.
Rugged Construction: Ultra-reliable metallic ground connection to reciprocating
shutter (no wiping contact), brushless stepper motor, powder-coated
aluminium case, Teflon insulators, and electro-polished 316L stainless steel
used for corrosion protection of critical exposed metallic parts
Easy Maintenance: The stator is easily removed for cleaning (proper cleaning
does not invalidate calibration). Instrument self-checking allows maintenance
to be performed on an as needed basis. The self-checking also monitors
internal humidity, insulator cleanliness, and power supply voltage, and
verifies that CS110 components such as the charge amplifier and shutter
open/close are functioning properly.
Operating Temperature Range: -25° to 50°C standard, -40° to +85°C optional
RH Range: 0 to 100% RH
Dimensions: 15.2 x 15.2 x 43.2 cm (6" x 6" x 17")
Weight: 4 kg (9 lbs)
Mounting: Vertical pipe 1.91 to 6.35 cm (0.75” to 2.5”) OD
5
CS110 Electric Field Meter
Warranty: The CS110 has a one year warranty against defects in materials and
workmanship. A three year warranty is provided for the embedded CR1000
Measurement and Control Module.
3. CS110 Measurement Details
The charge amplifier circuitry of the reciprocating electric field meter is depicted
in Figure 2. Induced charge on the sense electrode results in the operational
amplifier placing charge on the feedback capacitor C in order to restore the sense
electrode to virtual ground.
Figure 2. Charge Amplifier Circuitry of Reciprocating Electric Field Meter
The charge amplifier output during a measurement cycle of the reciprocating
electric field meter is illustrated in Figure 3.
6
Instruction Manual
Figure 3. Charge Amplifier Output During an Electric Field Measurement Cycle
160
Offset voltages V
off1
and V
are zero field reference measurements made when the
off2
shutter is closed, and utilized to accurately estimate voltage ΔV when the shutter is
completely open. Electronic offset voltages, surface potentials between various
metallic parts and leakage currents on the charge amplifier input result in non-zero
values of V
off1
and V
prior to the measure of V
. An electronic reset of the charge amplifier is performed
off2
to keep the charge amplifier output near zero volts when
off1
the shutter closed. The measured electric field E, as determined from the charge
amplifier output is as follows:
E = k⋅ΔV = k⋅[V
open
– (V
off1
+ V
)/2] (eq. 1)
off2
Where k is a constant determined by electrode geometry and electronic gain.
The resulting algorithm effectively eliminates measurement error sources that vary
slowly with respect to the time between zero field reference measurements, which is
approximately 140 ms. Measurement noise due to 50 or 60 Hz AC power can be
suppressed by utilizing the 50 Hz or 60 Hz noise rejection measurement capability of
the datalogger.
Current source I
in Figure 2 represents leakage currents across the Teflon
leak
insulators supporting the sense electrode, along with the input bias current of the
operational amplifier. Deleterious effects of I
are compensated for in the
leak
determination of ΔV as given in (eq. 1). However, it is desirable to minimize the
difference between V
magnitude V
voltages. Hence a leakage-current compensation circuit is utilized to
open
generate the current Icomp, illustrated in Figure 2, such that I
current compensation algorithm determines I
from the previous measurement, which is determined as follows:
on I
leak
off1
and V
in order to preserve dynamic range for large
off2
= I
comp
for the present measurement based
comp
leak
. The leakage-
I
Where C
is the value of feedback capacitor used in the charge amplifier, and I
f
= Cf·(V
leak
off1
– V
off2)
/ΔT + I
(eq. 2)
comp
the leakage current compensation value implemented during the measurement.
comp
is
7
CS110 Electric Field Meter
This charge amplifier input leakage current increases with degradation of insulation
of the sense electrode insulators due to moisture or other surface contamination.
Consequently, the measurement and reporting of I
when insulators should be cleaned.
The reciprocating motion of the CS110 electric field meter is limited to
approximately 5 Hz, which is adequate for lightning hazard warning, where 1 minute
averaged data is often used. For applications desiring > 5 Hz, the CS110
reciprocating electric field meter can be configured as a slow antenna (MacGorman
and Rust 1998). The shutter would typically be left open indefinitely in slow
antenna mode and resistor R3, depicted in Figure 2, is switched in parallel with Cf
providing a 66 ms decay time constant for the charge amplifier. In the slow
antenna mode, the charge amplifier has a high-pass filter frequency response with
the lower cutoff frequency defined as f
instrument is a field change meter and the charge amplifier output can be sampled
by the datalogger as fast as every 20 ms (50 Hz), using 250 μs integration
durations for the analogue integrator. Voltage measurements using the 250 μs
integration duration for an analogue integrator, result in an upper 3 dB bandwidth
of 1.8 kHz. Detailed information regarding the slow antenna mode of the CS110
is given in Appendix E and Section 8.3.
= (2⋅π⋅R⋅C)-1 = 2.4 Hz. In this mode the
3dB
is useful in determining if or
leak
4. Site Requirements and Recommendations
4.1 Power Requirements
Field mills typically consume many watts of power because their motors are
operated continuously. In the reciprocating approach, the stepper motor is
powered off much of the time, resulting in low power consumption. The current
required by the CS110 powered from 12 V DC is shown in Figure 4. As depicted
in the figure, the average electric field meter current is a function of the desired
measurement rate, which is user-controlled by means of the datalogger program,
making economical remote solar power feasible. Variable sample rates based on
measured results can also be implemented to conserve power in solar powered
applications. For example, the datalogger can be programmed to measure electric
field at a 10-second rate during fair weather conditions, and then automatically
switch to 1-second measurements during threatening conditions. An example
variable sample rate program is given in Appendix F. Figure 4 does not include
the current required for peripheral devices necessary to communicate with the
CS110 site. Like the stepper motor, communication devices that are turned off
when not needed, can offer low average power consumption.
8
Instruction Manual
1000
100
10
Average Current (mA) @ 12 V
1
0.1110100
Measurement Interval (Seconds)
Figure 4. CS110 Average Current Consumption versus Measurement Interval
The CS110 requires 11 V to 16 Vdc with a peak current demand of 750 mA
during motor operation. The CS110 Power Cable (PN 010350) is used to connect
the dc power supply to the CS110. The recommended max imum len gth on the CS110 Power Cable (CS110CBL3) is 15 metres. The CS110 is protected
against accidental reversal of the positive and ground leads from the dc power
supply. Transient protection is also included on the power supply inputs. DC
input voltages in excess of 18 V may damage the CS110.
4.2 Campbell Scientific Ltd Power Supplies
The PS100E provides a 12 Vdc, 7.0 Ahr rechargeable power supply for the CS110
and peripherals. Larger capacity battery packs are also available such as the
PS17E-LA. The rechargeable battery can be trickle-charged from an ac power
wall charger. Charging power can also come from a 17 – 28 VDC input such as a
solar panel. Depending on power requirements, 10 watt or 20 watt solar panels
are available.
4.3 Communication Options
The circular RS-232 connector on the underside of the CS110 can be used to
interface directly to RS-232 devices (DB-9), utilizing the CS110 RS-232 cable
(CS110CBL1).
The circular CS I/O connector on the underside of the CS110 can be used to
interface directly to various Campbell Scientific, Ltd. peripherals, utilizing the
CS110 CS I/O cable (CS110CBL2). Examples of CS I/O peripherals include the
CR1000 Keyboard Display and the COM220 phone modem.
The CS110 also offers SDI-12 communication or SDM (Synchronous Device for
Measurement) control capability utilizing the CR1000 control ports available
through the CS110 POWER CABLE (CS110CBL3).
9
CS110 Electric Field Meter
4.4 Site Recommendations
Many factors can distort and/or change the electric field at a given sight. For
example, vegetation growth can reduce the effective height of an elevated
instrument above the ground and can created unwanted space-charge due to
corona discharge. Gravel rings or concrete pads around a given site are
recommended to prevent changes in effective instrument height due to vegetation
growth. Electric field meters used for lightning warning at Kennedy Space Centre
use a 25-foot radius gravel ring around each electric field meter [LPLWS].
Animals and people within the vicinity of an electric field meter can significantly
alter the measurements. Fencing off a given site may be best for some
applications. However, installing a small metal fence around an electric field
meter site may result in corruption of measurements at large electric fields because
of corona discharge from sharp metal points on the fence.
Aerosols, dust, and automobile exhaust should be considered when selecting an
electric field meter site, as they can affect the local electric field.
In theory, the effects of tall nearby objects can be accounted for in site correction.
Yet, because of possible corona current along with general field distortion, it is
recommended that electric field meter sites should not be located near tall objects.
Kennedy Space Centre site requirements stipulate having no objects protruding
higher than 18° above the horizon, as seen from the ground at the electric field
meter location [LPLWS]. Roof mounted electric field measurements are practical
if a site correction can be done to account for field distortions.
Also a good Earth ground connection to the CS110 and associated mounting
hardware is necessary to make a given site appear as a vertical extension of the
Earth ground. It is recommended that the integrity of this Earth Ground
connection be checked periodically by verifying that the resistance of the stator to
Earth Ground rod is <1 Ω.
Although the list of factors that can impair electric field measurements is long,
experience has shown that useful electric field measurements can be made by
paying careful attention to the above mentioned details.
5. Factory Calibration and Site Correction
5.1 Factory Calibration
Electric field meters are typically factory calibrated using a parallel plate method,
where a uniform electric field is developed by applying a known voltage between
parallel conductive plates. The large hexagonal parallel plate electric field
calibrator illustrated in Figure 5 is used for factory calibration of the CS110
Electric Field Meter. The large physical size was incorporated to minimize nonideal fringing effects. Sharp corners were avoided in order to prevent corona
discharge. All metal parts of the calibrator are manufactured from stainless steel,
and the inside surfaces are polished to reduce the surface charges in order to
provide a stable zero electric field. All outer surfaces are electrically connected
and tied to Earth ground while the insulated inner plate is driven by a high voltage
amplifier. The high-voltage amplifier is calibrated out-of-house yearly against a
reference that is traceable to the National Institute of Standards and Technology
(NIST).
10
Instruction Manual
Figure 5. Parallel-Plate Electric Field Meter Calibration Chamber.
Each CS110 is factory calibrated in the parallel plate calibration fixture depicted
in Figure 5. A linear fit of the calibration data results in a calibration equation in
slope-intercept form expressed as
E = M
The multiplier M
parallel_plate
is a function of the CS110 electrode dimensions and the
parallel_plate
⋅V + O
parallel_plate
(eq. 3).
feedback capacitor in the charge amplifier. The offset term O
unwanted surface charges residing on non-conductive deposits on the electrodes.
The electric field offset of an instrument varies over time because of variations in
surface cleanliness along with charging and discharging processes. Polished 316L stainless-steel is used for critical electrode surfaces on the CS110 to minimize
unwanted surface charges. CS110s with clean electrodes have been found to
display electric field offsets <⏐30 V/m⏐, which has negligible effect on the
determination of M
parallel_plate
during factory calibration. Neglecting O
because of the ±15 kV/m range of electric fields used
parallel_plate
results in the simplified parallel-
plate calibration equation
E = M
parallel_plate
The estimated measurement accuracy of M
⋅V (eq. 4).
parallel_plate
for the CS110 calibrated in
the parallel plate electric field calibrator illustrated in Figure 5 is ± 1 %. The
electric field offset of the CS110 can be measured by covering the stator with a
clean Zero Electric Field Cover (PN: 010346). If the resulting zero field reading
parallel_plate
is due to
11
CS110 Electric Field Meter
with the zero field cover exceeds an absolute value of 60 V/m then cleaning of
electrodes in the CS110 is suggested. The factory calibration data for a typical
CS110 factory calibration and resulting determination of M
parallel_plate
= 84.32
V/m⋅mV (Volts/metre⋅millivolt) is illustrated in Figure 6.
20000
y = 84.324x + 26.258
2
= 1
15000
10000
5000
R
-200-150-100-50050100150200250
Applied Electric Field (V/m)
0
-5000
-10000
-15000
-20000
Charge Amplifier Output Voltage (mV)
Figure 6. Factory Calibration Data for CS110 SN: 1026
12
Instruction Manual
NOTE
Careful removal and replacement of the stator on the CS110 does
not invalidate the factory derived M
However, switching stators with another unit or accidentally
bending the stator, shutter or sense electrodes invalidates the factory
parallel-plate calibration because of possible electrode dimensional
changes.
5.2 Site Correction
As previously mentioned, each CS110 is factory calibrated in a parallel plate
calibration fixture resulting in calibration equation 4. However, when monitoring
the Earth’s electric field, equation 4 is valid only if the instrument aperture is
mounted flush with the Earth’s surface and upward-facing. Yet for permanent
outdoor measurements of electric field, a flush-mounted and upward-facing
orientation is problematic because of dirt, bird droppings, rain, etc., collecting on
the sense electrodes and fouling the measurement. Consequently, a downward
facing and elevated configuration as illustrated in Figure 8 is recommended for
long-term field applications.
Figure 7. NIST Calibration Certificate
parallel_plate
of a given unit.
13
CS110 Electric Field Meter
Figure 8. CS110 2 Metre CM10 Tripod Site.
Inverting the CS110 reduces the effective gain while elevating it’s height above
ground enhances the gain, with respect to an ideal upward-facing flush-mounted
geometry. It should be mentioned that this gain enhancement reduces the effect of
unwanted electrical field offsets. A site correction factor C
correct M
parallel_plate
The corrected multiplier M
M
In equation 5, M
site, whereas C
CS110 used at the site. C
for non flush-mounted configurations [McGorman and Rust].
becomes as follows:
corrected
= C
corrected
parallel_plate
site
is unique for each CS110, yet independent of a given
is unique for each given site, yet independent of the particular
is typically determined by using a flush-mounted
site
site⋅Mparallel_plate
is necessary to
site
(Eq. 5).
upward-facing unit in the vicinity of the site needing correction. Campbell
Scientific, Ltd. developed the site correction facility illustrated in Figure 9 to
determine C
for various site configurations.
site
14
Instruction Manual
Figure 9. Campbell Scientific, Ltd. Electric Field Meter Site Correction Facility
An upward-facing calibration kit (PN: 01034) was developed to hold the CS110 in
a flush-mounted upward-facing position, as illustrated in Figure 10.
Figure 10. CS110 Attached to Upward-Facing Flush-Mounted Plate for Site Correction
15
CS110 Electric Field Meter
NOTE
Both the upward-facing and the inverted and elevated unit need to
be electrically connected to Earth potential. This can best be
accomplished by a grounding rod and wire connected to ground lugs
provided on both the upward-facing plate and on the mounting
bracket on the standard CS110.
Ideally, site correction should be done in the absence of precipitation, and during
the presence of slowly varying electric fields of bipolar polarity and magnitudes
large enough to make instrument offset errors negligible. These conditions may
be infrequent in practice, making site correction using a flush-mounted upwardfacing unit somewhat challenging. Falling precipitation along with blowing dirt
can result in questionable measurements by an exposed, upward-facing unit.
Cleaning of the electrodes of an upward-facing unit is recommended after it has
been exposed to blowing dust and/or falling precipitation. The measurement of
meteorological parameters such as rainfall, along with the averaging and data
storage capability of the CS110 can be utilized to autonomously measure, process
and store data to aid in site correction.
Campbell Scientific, Ltd. has performed a site correction on the CS110 2 Metre
CM10 Tripod Site described in Appendix G. The collected data between the
upward-facing unit and a downward facing CS110 2 Metre CM10 Tripod site is
illustrated in Fig 11. A best-fit line computed from the data resulted in C
site
=
0.105 ± 4%, which is valid for users at other sites who use the same site
dimensions on level terrain clear of vegetation. Dimensional details of the 2 metre
standard meteorological site are described in Appendix F.
10/02/05 Site Correction of CS110 2 Meter CM10 Tripod Site
-80000-60000-40000-20000020000400006000080000
Mparallel_plate = 87.6 volt/meter*millivolt
10/02/05 Site Correction ofCS110 2 Meter CM10 Tripod Site
Results indicate C
Results indicate Csite = 0.105.
8000
6000
4000
2000
-2000
-4000
-6000
0
= 0.105.
site
y = 0.1051x - 35.664
2
R
= 0.9996
Mparallel_plate = 87.6 volt/meter*millivolt
Electric Field (volt/meter for Upward Facing CS110 SN:1022
Electric Field (volt/meter) for Upward Facing CS110 SN:1022
Uncorrected (C
Uncorrected (Csite = 1) Electric Field (volt/meter)for 2 Meter Mounted CS110 on CM10
Figure 11. Site Correction Data for CS110 2 Metre CM10 Tripod Site
16
The user is responsible for determining if a CS110 site is representative of the
CS110 2 Metre CM10 Tripod Site, and if not, for determining the
appropriate site correction.
The atmospheric electric field at the Earth’s surface during fair weather conditions
is on the order of –100 V/m; the negative sign indicating that the electrostatic
force on a positive charge is directed downward to the Earth’s surface
[McGorman and Rust],[Rakov and Uman]. Ballpark site corrections are sometimes
computed in fair weather conditions by assuming a -100 V/m fair weather field. The
accuracy of a fair weather site correction is questionable because local conditions
may result in a fair weather field significantly different (>100%) from –100 V/m.
Also, the unknown electric field offset may be significant when calibrating at –100
V/m. This offset can be measured by covering the stator with a clean Zero Electric
Field Cover (PN: 010346. Fair weather field site correction is not recommended for
lightning warning applications because of the relatively poor accuracy in determining
.
C
site
6. Lightning Warning
Lightning warning devices fall into two classes: lightning detectors and electric
field monitors. Stand-alone lightning detectors provide warning based on nearby
discharges, but give no warning until a detectable discharge occurs. Electric field
monitors measure the atmospheric electric field, indicating the presence of nearby
electrified clouds capable of producing lightning discharges. Consequently,
electric field monitors can give warning at the beginning of storms prior to
hazardous discharges. Both lightning detectors and electric field monitors are
employed in high-risk applications.
Instruction Manual
Lightning safety guidelines based on human obse rvati on s exist and shou ld
not be ignored simply because of the presence of sensitive electronic
instrumentation. The NOAA 30/30 rule suggests seeking shelter if thunder is
heard within 30 seconds of a lightning flash (approximately 6 miles), and
remaining in a sheltered area for 30 minutes after the last lightning or thunder
before resuming outdoor activities [NOAA].
It should be noted that no method of lightning warning completely eliminates the risks associated with lightning. As mentioned, lightning detectors give no
warning until a detectable discharge has occurred. Atmospheric electric field
yields warning prior to the “first strike” for storms developing overhead, along
with some indication of the end of a thunderstorm. Yet there are occurrences of
cloud-to-ground lightning discharges striking the ground several miles away from
the electrified cloud where the discharge initiated [NOAA]. Electric field
monitors may give no practical warning in these instances because the electric
field in the vicinity of the strike point may not indicate hazardous levels until
milliseconds before the strike. Consequently, while lightning warning systems
can greatly reduce the probability of death or injury from lightnin g
discharges, they cannot reduce this probability to zer o.
Figure 12. Electric Field Measured with CS110 during Local Thunderstorm
August 2, 2005 Thunderstorm at Logan, Utah
Mountain Standard Time (1 sample per second)
Figure 12 illustrates the atmospheric electric field monitored by a CS110 during a
local thunderstorm. As illustrated in Figure 11, the atmospheric electric field
changes dramatically from fair weather conditions (≈ -100 V/m) during the course
of this thunderstorm. The abrupt electric field change observed at approximately
6:12 am was due to a hazardous cloud-to-ground lightning discharge. A lightning
hazard warning algorithm would ideally issue an alarm, or perhaps various
caution/alarm levels, during the critical front-end portion of the storm illustrated in
Figure 11, as the electric field is seen to deviate from a typical fair weather field
and approach levels capable of producing hazardous lightning discharges. There
is no universal hazard alarm level based on atmospheric electric field, although
two levels that have been used are ≥ ⏐1000 V/m⏐ [LPLWS] and ≥ ⏐2000⏐ V/m
[NAVSEA]. Obviously the lower the level used the more risk reduction available,
at the expense of increased down time for operations suspended for lightning
hazard warning. Campbell Scientific is not liable for the reliability and
performance of the warning algorithms implemented by users of our
equipment. While lightning warning systems can greatly reduce the
probability of death or injury from ligh tning discharges, they cannot reduce
this probability to zero.
As previously mentioned, both lightning detection and electric field
monitoring are used for lightning warning systems in high-risk applications.
Lightning detectors with serial digital output s can be interfaced to the CS110
resulting in both lightning detection and electric field monitoring for a given
site. The CS I/O port, along with the three general purpose 0 to 5 V d igital
I/O ports (C1 - blue, C2 - yellow and C3 - gre en) available on the CS110
Power cable (CS110CBL3) can be used for a serial digital interface. Control
ports C1, C2 and C3 can also be used to conditionally control warning and
alarm indicators.
18
A network or array of electric field meters improves lightning warning
because of a wider area of coverage a lon g with measurement redundancy.
The PackBus
TM
communication protocol capability of the CR1000 datalogger
embedded in the CS110 provides for extensive n et wor kin g capabil ity.
7. CRBasic Programming
The CR1000 uses a programming language that has similarities to structured
BASIC, hence the name CRBasic. Within CRBasic there are special instructions
for making various measurements and for defining tables of output data.
Measured results are assigned variable names. Mathematical operations are
written out much as they would be algebraically. Conditional statements based on
measured results provide users with extensive capability for measurement and
control applications. See Section 8 for details on individual instructions.
Appendix F contains some example CRBasic programs for the CS110. A simple
example CRBasic program illustrating some of the general concepts follows:
'Comments can be inserted in CRBasic utilizing a single quote (').
'Simple CS110 program that measures panel (case) temperature, internal case
'relative humidity, battery voltage and electric field.(CS110_Simple.cr1).
'Updated last by Jody Swenson on 7/12/04.
const Mult = 85 'Define constant to be used in the program.
Public panel_temp 'Define variables to be used in the program.
Public internal_RH
Public battery_volt
Public E_field
Public leakage_cur
Public status
DataTable(Tab1,1,500) 'User defined table called Tab1 of size 500 records.
DataInterval(0,60,sec,10) 'Output data to the table processed every 60 seconds.
Average (1,panel_temp,ieee4,0) 'Average panel temperature over interval.
Average (1,internal_RH,ieee4,0) 'Average internal case RH.
Average (1,battery_volt,ieee4,0) 'Use 4 byte ieee4 format for wide dynamic range.
Average(1,E_field,ieee4,0)
StdDev (1,E_field,ieee4,0)
Average (1,leakage_cur,ieee4,0)
Maximum (1,status,ieee4,0,False)
EndTable
BeginProg
Scan(1,sec,0,0) 'Scan loop occurring every second.
PanelTemp (panel_temp,250) 'Measure temperature on CS110 panel board.
VoltDiff (internal_RH,1,mV2500,5,True ,0,250,0.1,0)
Battery (battery_volt) 'Measure CS110 battery voltage.
CS110(E_field,leakage_cur,status,_60Hz,Mult,0) 'CS110 electric field measurement.
CallTable Tab1 'Call data table Tab1 every scan.
NextScan
EndProg
Public variables are defined and available for viewing in the Public table, which is
a data table automatically set up by the CR1000. The Public table keeps only the
current value of each of the defined variables.
Instruction Manual
In the example program, the DataTable instruction is used to define the data table
Tab1. A record in a table consists of the data from all output processing
instructions, along with a record number and time stamp data. Using -1 for last
parameter in DataTable results in the automatic allocation of all available table
storage area. The DataInterval instruction following the DataTable instruction
defines the interval at which new values are determined and written into the table,
which is every 60 seconds in the above example. Once a table is full the CR1000
writes new values over the top of old values starting with the oldest data in the
19
CS110 Electric Field Meter
'CS110 efield and weather station program.(CS1 10_W S tat ion. cr 1).
'Measures rainfall, wind speed and direction, solar radiat ion,
'relative humidity and air temperature and electric field.
'Updated last by Jody Swenson on 11/15/05 for Error_Count.
const Mparallel_plate = 85
const C
site
= 0.10
const Mcorrected = Mparallel_plate*C
Public E_field
Units E_field=volts/m
Public battery_volt
Public leakage_cur
Units leakage_cur=nA
Public status
Public panel_temp
Units panel_temp=DegC
Public rain_fall
Units rain_fall=inch
Public wind_speed
Units wind_speed=mph
Public wind_dir
Units wind_dir=deg
Public solar_rad
Units solar_rad=W/m2
Public air_temp
Units air_temp=DegF
Public RH
Units RH=%
Public internal_RH
Units internal_RH=%
Public E_status(16) 'E_field status array.
Public k 'Index for E_status array.
Public meas_error 'Disable variable for slow table.
Public Error_Count 'Keep track of total errors measurements.
DataTable(Tabslow,1,-1) '-1 to auto-allocate all available memory.
DataInterval(0,60,sec,10) 'Averaged 60 second output data.
table. Data can be collected manually or automatically on a scheduled collection
interval by means of LoggerNet PC software.
The Sample output processing instruction simply outputs the current variable
value at the appropriate time to the data table. The Average and StdDev output
processing instructions accumulate all measured values over the associated data
interval and then compute the average and standard deviation, respectively, at the
appropriate time. Several other processing instructions exist for the CR1000 as
described in the CR1000 Measurement and Control System Operator’s Manual.
The Scan and NextScan instructions set up a loop based on the scan interval.
PanelTemp, VoltDiff, Battery, and CS110 are measurement instructions that
return the temperature inside the CS110 case, relative humidity inside the CS110
case, the voltage being provided to the CS110 to power the instrument and the
measured electric field, respectively. These and other measurement instructions
are discussed more fully in Section 7 on CS110 Measurement Instructions. The
CallTable instruction sends data to the output processing instructions associated
with a given table.
A more involved program that incorporates site correction multiplier, rainfall,
wind speed and direction, solar radiation, relative humidity and air temperature,
along with electric field follows:
'Mcorrected is what goes into CS110 instruction.
site
20
Instruction Manual
Average(1,E_field,ieee4,meas_error)
Sample (1,status,FP2) 'Use 2-byte floating point for non-critica l numbers.
Sample (1,Error_Count,FP2)
Totalize (16,E_status,FP2,0) 'Look at Efield status array over interval.
Average (1,leakage_cur,FP2,0)
Average(1,panel_temp,FP2,0)
Totalize (1,rain_fall,FP2,0)
WindVector (1,wind_speed,wind_dir,FP2,False,0,0,0)
Average (1,solar_rad,FP2,0)
Average(1,air_temp,FP2,0)
Average (1,RH,FP2,0)
Average (1,battery_volt,FP2,0)
Average (1,internal_RH,FP2,0)
EndTable
DataTable(Tabfast,1,-1) '-1 to auto-allocate all availa ble memory.
Sample(1,E_field,ieee4)
Sample (1,status,FP2)
Sample (1,leakage_cur,FP2)
Sample (1,rain_fall,FP2)
Sample (1,wind_speed,FP2)
Sample (1,wind_dir,FP2)
Sample (1,solar_rad,FP2)
Sample (1,air_temp,FP2)
Sample (1,RH,FP2)
Sample (1,battery_volt,FP2)
EndTable
BeginProg
Error_Count = Tabslow.Error_Count(1,1) 'Retrieve ErrorCount from Tab60sec in case of watchdog.
if (Error_Count = NAN) Then
Error_Count = 0
EndIf
Scan(1,sec,0,0)
for k = 1 to 16 'Initialize status array.
E_status(k) = 0
next
PanelTemp (panel_temp,250)
Battery (battery_volt)
VoltDiff (internal_RH,1,mV2500,5,True ,0,250,0.1,0)
PulseCount (rain_fall,1,2,2,0,0.01,0) 'TE525 tipping bucket 0.01 inches per tip
PulseCount (wind_speed,1,1 ,1,1,0.2192,0) 'Mult for 05103 Wind Monitor.
BrHalf (wind_dir,1,mV2500,4,Vx2,1,2500,False,450,250,355,0) 'Mult. for 05103 Wind Monitor.
VoltDiff (solar_rad,1,mV7_5,3,True,450,250,200,0)
meas_error = 0 'Initialize dis able va riable for E field ave rage in s low table .
SW12 (1 ) 'Apply 12 V to warm-up Temp and RH probe at least 150 ms.
CS110(E_field,leakage_cur,status,_60Hz,Mcorrected,0)
VoltSe (RH,1,mV2500,1,1,0,250,0.1,0)
VoltSe (air_temp,1,mV2500,2,1,0,250,.18,-40)
SW12 (0) 'Turn off power to Temp and RH probe.
if RH > 100 and RH < 108 then
RH = 100
EndIf
If E_field = NAN Then 'Not-A-Number because of measurement problem.
meas_error = 1 'Disable output to slow table if efield = NAN.
EndIf
E_status(status) = 1 'Set appropriate element in status array.
If status > 6 Then
Error_Count = Error_Count + 1 'Increment Error_Count.
EndIf
CallTable Tabfast
21
CS110 Electric Field Meter
CallTable Tabslow
NextScan
EndProg
This program incorporates two different user-defined data tables, Tabfast and
Tabslow. Tabfast contains 1 second measurements, while Tabslow contains 1
minute averaged data. Under certain error conditions the CS110 returns NAN
(Not-A-Number) for measured electric field rather than a questionable electric
field measurement. For example, the CS110 will detect if the shutter cannot be
properly closed at the completion of a measurement due to an obstruction. If the
shutter cannot properly close then the CS110 will return NAN for the electric field
measurement along with a status value indicating that the motor could not
properly close the shutter. The various CS110 status codes are described in
Appendix A.
The above program utilizes the array E_status(16) to store the various status codes
returned from a given measurement. The Totalize instruction in Tabslow
computes the total number of occurrences for each array value during the output
interval. Consequently, the array E_status returns the total number of occurrences
of each status code during the associated 1 minute output interval. As given in
Appendix A, status codes 1, 2, and 3 are associated with good electric field
measurements, whereas each of the higher codes indicates a concerning condition
such as low-battery voltage or too much leakage current on the electrode
insulators.
There are times when it is desirable to exclude a measured result from an output
processing instruction such as Average. This can be conveniently accomplished
using a disable variable (DisableVar) associated with appropriate output
processing instructions. The last parameter of the Average instruction is the
DisableVar and will exclude the current measured value when DisableVar is not
equal to zero. In order to prevent a single NAN electric field result from
corrupting measurements over the entire output interval, the variable meas_error is
used to disable writing NAN results to the Average(1,E_field,ieee4,meas_error)
instruction in TabSlow.
It is also sometimes desirable to keep a count of total measurement errors, which
is accomplished in the above program by the variable Error_Count. The last
stored value of Error_Count is retrieved from final storage at the beginning of the
program and Error_Count is incremented once during a scan each time status >6
from the CS110 instruction. The Error_Count can be zeroed by means of
LoggerNet by accessing the Public variable Error_Count in the Numeric display
available in the Connect Screen.
Appendix F contains more example CS110 programs that users may find
beneficial in various applications. A more detailed description of CRBasic is
contained in the CR1000 Measurement and Control System Operator’s Manual.
8. CS110 Measurement Instructions
8.1 CR1000 Measurement Overview
22
The CR1000 datalogger can perform many different measurement tasks as defined
by measurement instructions in CRBasic. A brief explanation of CS110
measurement instructions is given followed by some specific examples. Further
measurement instructions and measurement details are provided in the CR1000
Measurement and Control System Operator’s Manual.
Instruction Manual
The CR1000 differential voltage measurement (VoltDiff) instruction is given as
where Dest is the destination variable of the result. Reps is the number of times to
repeat a given measurement on successive channels, Range is one of ±5000 mV,
±2500 mV, ±250 mV, ±25 m, ±7.5 mV, or ±2.5 mV input voltage ranges available
on the CR1000. DiffChan is the appropriate differential input channel (1 – 8).
RevDiff is a true or false parameter to determine whether or not to perform two
successive differential measurements with reversed input polarity, in order to
reduce low-frequency measurement errors. Settling Time is a parameter allowing
extra input settling time for “slow” settling sensors. Integ is a parameter
indicating the length of time to perform an analogue integration during the
measurement, with options of 250 μs, _50Hz and _60Hz. Integration times for
_50Hz and _60Hz are 20 ms and 16.67 ms, respectively for cancellation of
unwanted 50 Hz and 60 Hz noise. Mult provides for scaling within the
measurement instruction, while Offset provides for the incorporation of offsets.
Single-ended voltage measurements are referenced to ground, rather than the low
side of a differential input. The VoltSE single-ended measurement instruction is
quite similar to the VoltDiff instruction and is given as follows:
An internal ground reference is utilized in single-ended measurements. Singleended offset errors are reduced in single-ended measurements by measuring the
voltage on the internal ground reference. The MeasOff parameter in the VoltSe
instruction determines if this internal ground reference is measured at the
beginning of every VoltSe instruction (MeasOff = True) or whether a single-
ended offset voltage measure is performed as part of an on-going instrument self-
calibration routine occurring in background (MeasOff = False).
Another general purpose voltage measurement instruction is the BrHalf
instruction, which provides voltage excitation for a simple resistive divider (half
of a 4-element Wheatstone bridge), and then measures the resulting voltage.
Most parameters of the BrHalf instruction are common to the VoltDiff and
VoltSE instructions, and so only the differences will be discussed. The ExChan
parameter determines which one of the three CR1000 voltage excitation outputs
are used to excite the half-bridge. MeasPEx determines how many successive
channels are excited by the same excitation channel in successive Reps. ExmV
determines the excitation voltage which can range from –2500 mV to +2500 mV.
RevEx is a true/false parameter and if true then the polarity of the excitation is
reversed during the measurement and a second measurement taken. Like input
reversal on differential measurements, excitation reversal is an error cancelling
technique for reducing low-frequency measurement errors such as offset voltages.
The Battery instruction is used to measure the input voltage of the power supply
to the CS110 and follows:
Battery (Dest)
The PanelTemp instruction is used to measure the temperature of a thermistor
located within the CS110 case and follows:
23
CS110 Electric Field Meter
8.2 Measuring Electric Field
PanelTemp (Dest,Integ)
The PulseCount instruction is used to count the pulses generated from sensors,
such as an anemometer or switch closures from a tipping bucket rain gauge, and
has the following parameters.
PChan is the number pulse channel (1 or 2) used for the measurement. PConfig is
a code (0-2) for three different types of pulse-count inputs; High-frequency = 0,
low-level AC = 1, and switch closure = 2. POption is a code to determine if
results are returned as counts for a given interval (POption = 0), or as frequency =
counts/(scan interval in seconds) (POption = 1).
The CS110 instruction is used to perform the electric field measurement of the
CS110 and follows:
CS110(Dest,Leakage,Status,Integ,Mult,Offset)
Leakage is a variable containing the measured leakage current in nano amps (nA)
on the charge amplifier input during the CS110 electric field measurement. A
perfect unit is 0 nA. Actual units deviate from perfection such that some have
small (<< 1 nA) positive leakage current and some have small negative leakage
current. Status is a variable containing numeric codes indicating various status
conditions occurring during the measurement, as defined in Appendix A. Integ is
a parameter indicating the length of time to perform an analogue integration
during the measurement, with options of 250 μs, _50Hz and _60Hz. Integration
times for _50Hz and _60Hz are 20 ms and 16.67 ms, respectively for cancellation
of unwanted 50 Hz and 60 Hz noise. Mult provides for convenient scaling within
the measurement instruction, and Offset provides for convenient incorporation of
offsets. The CS110 instruction measures the electric field utilizing the ±250 mV
range. If the result is NAN, the instruction re-measures utilizing the ±2500 mV
input voltage range.
24
8.3 Measuring Electric Field Change
CS110Shutter(Status,Move)
Status is a variable containing the following subset of measurement status codes
given in Appendix A: status codes 1, 4, 7, 8, 9, 10, 11, 14, 15, and 16.
Move is a variable set to 1 to open the shutter and set to 0 for the CS110Shutter
instruction to close the shutter.
The CS110Shutter instruction can be utilized along with a Delay instruction to
visually verify the fully opened and fully closed positioning of the CS110 shutter,
as described in Appendix D on Servicing the CS110. The CS110Shutter
instruction can also be used to implement a Slow Antenna electric field
measurement as described in Appendix E. The CS110 panel board contains
circuitry to switch in a parallel 200 MΩ resistor with the 330 pf feedback
capacitor in the charge amplifier during execution of an open shutter
CS110Shutter instruction. This results in a charge amplifier with a 66 ms time
constant implemented as a slow antenna that can be utilized to measure changes in
electric field at rates much faster than the 5 Hz maximum rate of the CS110
electric field measurement instruction. In the slow antenna mode the CS110
becomes a field-change meter, meaning that the useful data becomes the
Instruction Manual
differences between the VoltDiff measurements rather than the absolute value of
each VoltDiff measurement.
8.4 Measuring Solar Radiation or Barometric Pressure
Circular connector labelled SOLAR RADIATION on the CS110 can be used to
connect up an LI200X solar radiation sensor. Alternately, a special cable, the
CS110 BAROMETRIC PRESSURE SENSOR CABLE (17460), can be purchased
and connected to the SOLAR RADIATION connector to interface to either the
CS100 or the CS106 barometric pressure sensor. Examples of instructions to
measure the LI200X solar radiation sensor or the barometric pressure sensors are
given below.
8.5 Measuring Air Temperature and Relative Humidity
Circular connector labelled TEMP/RH can be used to connect up an HC2S3
temperature and relative humidity sensor. Example CRBasic instructions to
measure the HC2S3 Temperature and RH are given below.
SW12 (1 ) ‘Apply switched 12 V power to the probe.
Delay (0,150,mSec) ‘Warm up probe before measurements.
VoltSe (air_temp,1,mV2500,2,1,0,250,.18,-40) ‘Single-ended air temp. measure.
VoltSe (RH,1,mV2500,1,1,0,250,0.1,0) ‘Single-ended relative humidity.
SW12 (0) ‘Turn off power to the probe.
if RH > 100 and RH < 108 then
RH = 100
Endif
8.6 Measuring Wind Speed and Direction
Circular connector labelled WIND can be used to connect up various wind
sensors, including the 05103 Wind Monitor, 034 Met One Wind Sensor, and
03001 Wind Sentry. Example CRBasic instructions to measure the 05103 Wind
Monitor are given below.
PulseCount(rain_fall,1,2,2,0,0.01,0) 'TE525 tipping bucket 0.01 inches per tip
8.8 Measuring Internal Case Humidity
9. PC Software
Circular connector labelled RAIN can be used to connect up a rain gauge using a
switch closure such as the CS700 or the TE525MM tipping bucket rain gauges.
Example CRBasic instruction to measure the TE525 is given below.
In order to determine when to change desiccant within a CS110 case, a relative
humidity sensor is contained inside the case. The following CRBasic instruction
provides internal humidity data to the variable Internal_RH, which can then be
monitored in real-time and/or included in an output table.
Changing of CS110 desiccant is recommended for internal relative humidity
values ≥ 80%.
9.1 Quick Start
Campbell Scientific offers two datalogger support software packages for PC
computers that can be used with the CS110 and its embedded CR1000 datalogger.
The PC400 package is less expensive than the full featured LoggerNet package
but PC400 does not support combined communication options (e.g., phone-toRF), PakBus routing, or scheduled data collection. LoggerNet software is
recommended for applications that require these capabilities.
The CS110’s embedded CR1000 datalogger is only supported in LoggerNet
version 3.0 and higher or PC400 version 1.0 and higher. Upgrades to earlier
versions of LoggerNet or PC208W are available for approximately half the list
price.
The following overview describes connecting a PC running LoggerNet to the
CS110 and viewing electric field data. The full capabilities of LoggerNet and
PC400 are covered in their respective manuals.
Connect the CS110’s RS232 port to the PC, and apply 12 Vdc power to the
CS110. Due to a factory installed CR1000 program the shutter should begin to
open/close about 30 seconds after power is turned on.
The CR1000 uses a Campbell Scientific communication protocol called PakBus.
Each CR1000 datalogger in a network connecting to the LoggerNet PC should
have a unique PakBus address. Each CS110 is shipped with a PakBus address
of 1.
26
The following three screen captures show the settings for each of the three links in
the path from COM Port 1 on the PC to the CS110 with the factory default PakBus
address of 1. Use LoggerNet Tool Bar’s “Setup” button or “EZ Setup” button to
create the PC to CS110 communication path shown below:
Instruction Manual
27
CS110 Electric Field Meter
Remember to click on the “Apply” button to cause the settings to take effect. The
“Apply” button is greyed out once it has been executed.
Once this is done, switch to the “Connect” button on the LoggerNet Tool Bar,
select the CS110, and select “Connect”.
28
If the connection is made and the stations time shows up in the window, you can
then select the “Numeric:” button and add the desired public variables to see
electric field readings updated every measurement interval.
Instruction Manual
If you have changed the CR1000’s PakBus address and subsequently forgotten it,
you can download from http://www.campbellsci.com/downloads at no cost, a
software package named Device Configuration Utility that will discover the
PakBus address. Run the software and set it up with device type set to CR1000,
specify the correct COM port, and select “Connect” and the software will discover
the PakBus address for you.
If necessary, this software is also used to send a new operating system (OS) to the
CR1000.
The following screen captures show the Device Configuration software.
29
CS110 Electric Field Meter
10. Maintenance
10.1 Checking Site Ground Integrity
10.2 Corrosion and Rust Inhibitors
The CS110 electric field meter needs to be electrically connected to Earth ground
for valid measurements. It is recommended that the integrity of this Earth Ground
connection be checked periodically by verifying that the resistance of the stator to
Earth Ground rod is <1 Ω.
In corrosive environments, metal friction points (set screws, bolts, etc.) and
electrical connections to earth ground can be protected with the use of a rust
inhibitor. Sanchem makes such an inhibitor and some information on their
products may be found at http://www.sanchem.com/ox.html. Following is an
excerpt from their web site:
“NO-OX-ID A-SPECIAL is a soft, wax based rust preventive and lubricant that
contains an active rust inhibitor and small amount of solvent for ease of
application. This corrosion resistant coating can be applied by spray or brush
application. NO-OX-ID A-SPECIAL controls corrosion by leaving a thick, semitransparent, non-drying barrier coating that retains its anti-rust properties
indefinitely.
30
NO-OX-ID A-SPECIAL is the electrical contact grease of choice in new electrical
installations and maintenance because of its excellent performance in keeping
metals free from corrosion. This rust preventative has been used for over 50 years
to prevent corrosion in electrical connectors from low micro-power electronics to
high voltage switchgear. NO-OX-ID A-SPECIAL prevents the formation of
oxides, sulfides and other corrosion deposits on copper surfaces and conductors
can be prevented with its use.”
Instruction Manual
Loctite also makes a similar product and some information on their products may
be found at http://content.loctite.com/sticks/silver-as.html. Following is an excerpt
from their web site:
Heavy-duty, temperature-resistant up to 1600°F, petroleum-based lubricant
fortified with graphite and metallic flake.
Features & Benefits
• Protects metal parts in high heat environments up to 1600°F
• Prevents rust, corrosion, seizing and eases disassembly
• Reduces friction and wear to critical parts
• Buttery texture ideal for both coarse and fine threads
• Exceptional lubrication properties
Typical Applications
•For use with copper, brass, cast iron and all alloys including stainless steel, all
The CS110 has been designed to provide reliable electric field measurements and
to simplify and minimize maintenance. Scheduled maintenance may not be
required, as the CS110 incorporates extensive self-checking, and provides status
information about each measurement. An example CS110 instruction follows.
Returned E_field values of NAN (Not-A-Number) indicate a measurement
problem that can be determined from the associated status value.
The status parameter returned from each electric field measurement reports of
measurement problems along with instrument health. The CS110 status values
are described in Appendix A.
The leakage parameter returns the measured charge amplifier input leakage
current. A perfect unit is 0 nA. Actual units deviate from perfection such that
some have small (<< 1 nA) positive leakage current and some have small negative
leakage current. Occasional leakage current values exceeding ±4.2 nA may occur
if insulators are wet. If leakage current values return to < ⎢1.0 nA⎟ upon drying
then no service is required. However, prolonged leakage current values near to
and exceeding ⎢4.2 nA⎟ are likely due to insulator contamination requiring
removal of the stator and cleaning.
10.4 Cleaning the CS110 Electrode Head
The CS110 motor assembly illustrating the 316-L stainless-steel stator, shutter,
and sense electrode is illustrated in Figure 13.
Base Plate
Shutter
Sense Electrode
Insulator
Stator
32
Figure 13. CS110 Stator, Shutter and Sense Electrode
Instruction Manual
Contamination of the polished stator, shutter, and sense electrode can result in
unwanted surface charges that induce electric field offset errors in the
measurement.
Three Teflon insulators are utilized to electrically insulate the high-impedance
sense electrode from the motor assembly base plate. Surface contamination of
these insulators can result in excessive leakage current. The CS110 includes a
circuit to compensate for input leakage current on the charge amplifier up to ±4.2 nA.
Leakage current values in excess of ±4.2 nA can cause measurement errors and
are indicated by status = 11.
Cleaning of the CS110 electrodes and/or insulators is recommended if any of
the following conditions occur:
• When insulators are dry, and leakage current exceeds ± 4.2 nA as indicated by
status = 11.
•Visual evidence of contamination (salt deposits, scaling, dust, spider webs
etc.) on or around electrode area.
• Zero field reading with Zero Electric Field Cover (PN: 010346) exceeds
± 60 V/m. Note: it is important that the inside of the zero field cover also be
clean for good zero field reading.
Electrode Cleaning Procedure:
1. Remove the stator by loosening the 2 Philips head screws on the motor
assembly base plate, allowing the stator to pivot and be removed.
2. Inspect the stator for any contaminant deposits and scrub such deposits off
with soap and hot water if available. Any residue may form non-conductive
layers that can hold unwanted surface charge. Using a brush that will fit
between the shutter and the sense electrode, carefully wash the shutter and
sense electrode, along with the three insulators attaching the sense electrode
to the main body of the CS110. One brush (CSI PN #17578) ships with each
CS110. Large offsets are likely due to electrical charges residing insulative
deposits on metallic surfaces, while large leakage currents are likely due to
contaminated insulators.
3. Rinse well, using de-ionized water if available, and blow dry with air. Note:
Rubbing and wiping tends to induce unwanted surface charging that will
eventually dissipate.
4. Reassemble the stator making sure it is positioned properly before tightening
the two Philips head stator screws. Try and avoid getting fingerprints, etc. on
clean electrodes as they can result in unwanted surface charge. (Clean cotton
gloves are helpful.)
5. Attach the zero field cover plate (PN: 010346) to the stator and verify that the
leakage current ≤ ⎢0.5 nA⎟ and that the zero field offset ≤ 60 V/m. Leakage
current > ⎢0.5 nA⎟ and/or zero field offsets > 60 V/m indicate problems with
cleanliness and/or unwanted surface charge.
10.5 Changing Desiccant
The CS110 is shipped with desiccant inside the sealed case to reduce humidity for
the sensitive electronics enclosed. A humidity sensor is also contained inside the
CS110 case to allow monitoring of the internal relative humidity. The following
33
CS110 Electric Field Meter
CRBasic instruction provides internal humidity data to the variable Internal_RH,
Changing of CS110 desiccant is recommended for internal relative humidity
values ≥80%.
NOTE
34
Figure 14. Inside of CS110 Case Illustrating Bracket
for Holding Desiccant.
Replacement intervals less than once every six months for the 4
Unit (PN: 005669 desiccant pack within the sealed CS110 case
indicate a problem with the CS110 case seal or with the desiccant
packs being used.
Procedure for Changing Desiccant:
1. Remove the CS110 case lid by unscrewing the captive screws that attach the
lid to the main body of the CS110.
2. Inspect the gasket on the CS110 lid making sure that a good seal is possible
when the lid is replaced.
3. Remove the old desiccant pack and replace with a new 4 unit desiccant pack
(PN: 005669) making sure the new pack is placed into the bracket that
prevents the desiccant from sliding into the motor assembly.
10.6 Checking Shutter/Encoder Alignment
Status codes 14, 15, and 16 indicate problems with the stepper motor correctly
opening and closing the shutter. A mechanical trim procedure is done at the
factory to set proper shutter/encoder alignment, as described in Appendix D.
Proper shutter/encoder alignment can be verified with the following procedure
utilizing the special CS110Shutter instruction which positions the shutter in the
fully closed or fully open positions. The following program combines the
CS110Shutter instruction with Delay instructions so that fully closed and fully
open shutter positions can be verified visually. Stator to shutter overlap exists in
the fully opened and fully closed positions so that slight shutter position variations
do not alter the exposed area to the sense electrode. A fully opened shutter will
display symmetrical stator to shutter overlap, within the 1.8° stepper motor step
size, on both edges of each of the 4 openings in the stator when viewed from a
perpendicular position to the direction of the shutter blades. No visible gaps
between the stator and shutter blades should be visible on a fully closed shutter
when viewed from a position perpendicular to the shutter blades.
'Program to open/close the CS110 shutter (CS110_Shutter1.cr1).
'Last updated by Jody Swenson on 9/26/05.
Battery(Batt)
CS110Shutter(stat(1),1) 'Fully open shutter.
Delay (0,3000,mSec)
CS110Shutter(stat(2),0) 'Fully close shutter.
CallTable Efield
NextScan
EndProg
10.7 Re-Calibration
Re-calibration of measurement instruments is commonly done in data critical
applications in order to combat component drift with time. Component drift is a
function of the environment experienced by the instrument. High humidity and/or
high temperature environments generally cause the most drift. For the CR1000
datalogger a two year re-calibration interval is recommended, with longer
intervals being sensible for users that find negligible instrument drift over a two
year period. The embedded CR1000 datalogger inside the CS110 case should
35
CS110 Electric Field Meter
experience a low-humidity environment, which helps minimize datalogger
measurement drift.
As mentioned in Section 5.1, each CS110 is factory calibrated in the parallel plate
calibrator illustrated in Figure 5 to determine individual instrument gain. The
CS110 electric field measurement instrument gain is a function of electrode
dimensions, along with the 1% feedback capacitor used in the charge amplifier.
While measurement drift of CR1000 is likely negligible with regard to the ±5% of
reading accuracy specification of electric field measurements, datalogger drift may
be a factor for the measurement of temperature by means of an external
temperature and RH probe.
A parallel-plate calibration is recommended whenever any electrodes are bent,
removed or replaced, with the exception of the removal and replacement of the
same stator during the process of insulator cleaning. For CS110 applications
requiring long-term electric field measurement accuracy better than ± 10%, a
parallel plate factory calibration is recommended every three years.
The expected lifetime of the CS110 is 5 to 10 years, again depending upon the
operational environment. Instruments operated in coastal environments will likely
suffer from external finish degradation and/or operational failure sooner than
instruments operated in dry inland environments.
11. References
“Lightning Physics and Effects” by Vladimir A. Rakov and Martin A. Uman,
Cambridge University Press, 2003.
“The Electrical Nature of Storms” by Donald R. MacGorman, and W. David Rust,
Oxford University Press, Inc., 1998.
“On some determinations of the sign and magnitude of electric discharges in
lightning flashes” by C.T.R. Wilson, Proceedings of the Royal Society, Series A,
Vol. 92, 555-574, 1916.
“Industrial Electrostatics – fundamentals and measurements” by D.M. Taylor and
P.E. Secker, John Wiley & Sons Inc. 1994, pg. 36-38.
(LPLWS) METEOROLOGICAL\CCAFS\81900\LAUNCH PAD LIGHTNING
WARNING SYSTEM
(http://www-sdd.fsl.noaa.gov/RSA/lplws/LPLWS-handbook.Apr03.pdf
note that the web site address is case sensitive.
NOAA (See www.lightningsafety.noaa.gov\outdoors.htm
NAVSEA OP 5, Vol 1, Seventh Rev. Para 6-2, pg 6-1 and 6-2, 2001.
.)
). Please
36
Instruction Manual
CS110 electric field measurement instrument gain is a function of electrode
dimensions, along with the 1% feedback capacitor used in the charge amplifier.
While measurement drift of CR1000 is likely negligible with regard to the ±5% of
reading accuracy specification of electric field measurements, datalogger drift may
be a factor for the measurement of temperature by means of an external
temperature and RH probe.
A parallel-plate calibration is recommended whenever any electrodes are bent,
removed or replaced, with the exception of the removal and replacement of the
same stator during the process of insulator cleaning. For CS110 applications
requiring long-term electric field measurement accuracy better than ± 10%, a
parallel plate factory calibration is recommended every three years.
The expected lifetime of the CS110 is 5 to 10 years, again depending upon the
operational environment. Instruments operated in coastal environments will likely
suffer from external finish degradation and/or operational failure sooner than
instruments operated in dry inland environments.
11. References
“Lightning Physics and Effects” by Vladimir A. Rakov and Martin A. Uman,
Cambridge University Press, 2003.
“The Electrical Nature of Storms” by Donald R. MacGorman, and W. David Rust,
Oxford University Press, Inc., 1998.
“On some determinations of the sign and magnitude of electric discharges in
lightning flashes” by C.T.R. Wilson, Proceedings of the Royal Society, Series A,
Vol. 92, 555-574, 1916.
“Industrial Electrostatics – fundamentals and measurements” by D.M. Taylor and
P.E. Secker, John Wiley & Sons Inc. 1994, pg. 36-38.
(LPLWS) METEOROLOGICAL\CCAFS\81900\LAUNCH PAD LIGHTNING
WARNING SYSTEM
(
NAVSEA OP 5, Vol 1, Seventh Rev. Para 6-2, pg 6-1 and 6-2, 2001.
37
Appendix A. CS110 Measurement Status
Codes
Status codes 1 through 3: Good Instrument Health.
status = 1, Good instrument health. ±250 mV measurement range only.
Return measured Efield value.
status = 2, Good instrument health. ±2500 mV measurement range used.
Return measured Efield value.
status = 3, Good instrument health. NAN returned for Efield because of
measurement over-range on the ±2500 mV measurement range.
No priority issues exist with status codes 1 through 3 since only 1 of these “Good
Instrument Health” codes can exist for a given measurement.
Status codes 4 through 6: Good measurement, after properly positioning the
shutter.
status = 4, Good instrument health. ±250 mV measurement range only. Had to
properly position shutter.
status = 5, Good instrument health. ±2500 mV measurement range used.
Had to properly position shutter.
status = 6, Good instrument health. NAN returned for Efield because of
measurement over-range on the ±2500 mV measurement range. Had to
properly position shutter.
Status code 4 through 6 indicate that the shutter was not properly positioned upon
commencing the measurement. The problem was recognized, corrected and a valid
measurement made. Status codes 4 through 6 are common upon power up, or if
the shutter has been touched or bumped since the last execution of the CS110
instruction. Persisting status codes 4 through 6 indicate a problem with parking the
shutter that should be investigated.
Status codes 7 through 10:
Datalogger warnings and errors.
status = 7, +5Vext low. Return measured Efield value.
status = 8, Datalogger skipped scan. Return measured Efield value.
status = 9, Input power < 9.6 V. Return measured Efield value.
status = 10, Datalogger watchdog reset. Return measured Efield value.
Status codes 7, through 10 increase in priority with 7 being the lowest and 10 the
highest of the warning and error codes. Status code 7 is a low priority error
message, as low +5Vext is a concern, but does not corrupt electric field
measurements. Status code 7 is overwritten by any other warning and error code
(i.e. status ≥ 7), including Leakage current exceeds compensation range.
Status codes 8 through 10 are the highest priority error messages returned by the
CS110, and will overwrite other lesser errors that occur simultaneously during the
CS110 instruction. Since only one status value can be returned from a CS110
instruction, status 10 is given the highest priority, status 9 the second highest, and
8 the third highest priority of CS110 status codes. Next in priority are codes 16,
15, 14, 13, 12, and 11 followed by 7, 6, 5, 4, 3, 2 and 1.
A-1
Appendix A. CS110 Measurement Status Codes
Status codes 11 through 16:
Measurement warnings and errors.
status = 11, Leakage current exceeds compensation range of ± 4.2 nA. Return
measured Efield value.
status = 12 Failed charge-amplifier self check. Return NAN instead of
measured Efield value.
status = 13, Large closed shutter offset voltage. Vos > ⏐1.00 V⏐. Return NAN
instead of measured Efield value.
status = 14, Motor move error. Incorrect number of motor steps to close shutter.
Return NAN instead of measured Efield value.
status = 15, Motor move error. Encoder UPCNTs < 24 or > 26. Encoder
DNCNTs < 24 or > 26, or don’t find home when closing. Return NAN
instead of measured Efield value.
status = 16, Can’t properly position shutter. Return NAN instead of measured
Efield value.
Status code 11 returns the measured Efield value because the electric field
computation algorithm compensates for leakage current, even if it exceeds ±4.2
nA, although maximum signal amplitude becomes limited. Consequently,
cleaning of the instrument is recommended if status code 11 persists for long
periods of time.
Status codes 12 through 16 all cause the measured electric field to be set to NAN
in order to prevent the use of possible erroneous measurements. The priority of
codes 11 through 16 increases with increasing values, although codes 8, 9 and 10
are higher priority.
A-2
Appendix B. CS110 Accessories
B.1 Zero Electric Field Cover
As previously mentioned, unwanted surface charges residing on non-conductive
deposits on electrodes result in a non-zero electric field, even when external
electric fields are zero. Polished 316-L stainless-steel is used for critical electrode
surfaces on the CS110 to minimize unwanted surface charges. CS110’s with clean
electrodes have been found to display electric field offsets less than 20 V/m in
absolute value. The CS110 Zero Electric Field Cover (PN: 010346) is used to
check the electric field offset voltage of the CS110. If the measured electric field
is ≥| 60 V/m| with the Zero Electric Field Cover on, then inspection and cleaning
of the electrode surfaces as discussed in Section 10.4 is recommended.
B.2 Upward-Facing Site Calibration Kit
As previously mentioned, the CS110 is calibrated in a parallel plate calibration
chamber, resulting in a valid calibration for a flush-mounted upward-facing
configuration. Yet, inverted and elevated CS110 mounting configurations are
recommended for long term installations. Upward-facing site calibration kit
(PN: 01034) has been designed to provide a flush-mounted upward-facing
configuration for the CS110 to aid in determining site correction factors.
B.3 CR1000 Keyboard Display
The CR1000 keyboard display (CR1000KD) is a convenient CR1000 user
interface that can be directly connected to the CS110. The CR1000 keyboard
display connects to the CS110 through the CS I/O port, requiring a CS110 CS I/O
Cable (CS110CBL2-L). The CR1000KD can be used to view data and programs,
and to make simple program modifications. Details on the CR1000KD can be
found in the CR1000 Measurement and Control System Operators Manual.
B.4 Miscellaneous Peripheral Modules
The CS110 is compatible with CSI SDM (Synchronous Device for Measurement)
peripherals. The C1, C2, and C3 control ports necessary for SDM are available
through the CS110 POWER CABLE (CS110CBL3-L). SDI-12 sensors can also
be read using C1 and/or C3.
B-1
Appendix B. CS110 Accessories
This is a blank page.
B-2
Appendix C. CS110 Connector Pinouts
The following information describes the connectors that mate with the builtin (bulkhead) connectors on the CS110. Connector pin numbering for the 6
and 9 pin connectors are shown below. The view is a view of the solder-cup
side of the cabled connector. The circular connectors are Mini-Con-X type
from Conxall. The CSI part numbers shown for the connectors include the
backshell. CSI fills the backshell with a relatively thick epoxy to seal and
provide strain relief.
1
6
2
3
POWER CONNECTOR
CS110CBL3-L CS110 Power Cable
Connector is female and is CSI PN 17654 (Conxall #6282-6SG-522 or
Switchcraft #EN3C6F). Pin 1 is indicated with a dot.
Pin Description Colour
1 C1 Control Port 1 Blue
2 +12 V Power Red
3 Gnd Digital Ground Drain (clear)
4 P_Gnd Power Ground Black
5 C3 Control Port 3 Green
6 C2 Control Port 2 Yellow
5
4
1
29
38
7
6
5
4
WIND CONNECTOR
Connector is male and is CSI PN 9889 (Conxall #6282-6PG-522 or
Switchcraft #EN3C6M). Pin 1 is indicated with a dot.
Pin Description
1 2LO Single-ended channel 4
1 1Mohm Pin 1 also connects to ground via a 1 Mohm 1% 50ppm
resistor
2 Gnd Panel Ground
3 EX2 Excitation channel 2
4 P1 Pulse channel 1
5 Gnd Power ground
6 Gnd Ground
C-1
Appendix C. CS110 Connector Pin-outs
RAIN CONNECTOR
Connector is male and is CSI PN 9889 (Conxall #6282-6PG-522 or
Switchcraft #EN3C6M). Pin 1 is indica ted w/ a dot
Pin Description
1 empty
2 empty
3 P2 Pulse channel 2
4 empty
5 Gnd Power ground
6 Gnd Power ground
CSIO CONNECTOR
CS110CBL2-L CS110 CS I/O Cable
Connector is 9 pin female and is CSI PN 17674 (Conxall #3082-9SG-330).
Pin 1 is indicated w/ a dot
Pin Description
1 +5V +5 Volt dc supply
2 Gnd Power ground
3 Ring Ring
4 RX Receive
5 ME Modem enable
6 SDE Synchronous device enable
7 CLKHS Clock hand shake
8 +12V +12 Volt dc supply
9 TX Transmit
RS-232 CONNECTOR
CS110CBL1-L CS110 RS-232 Cable
Connector is 9 pin male and is CS I PN 15880 (Conxall #3282-9PG-330).
Pin 1 is indicated w/ a dot
Pin Description
1 DTR Data terminal ready
2 TX Transmit
3 RX Receive
4 empty
5 Gnd Power ground
6 DTR Tied to pin 1
7 CTS Clear to send
8 RTS Request to send
9 Ring Ring
C-2
Appendix C. CS110 Connector Pin-outs
SOLAR RADIATION CONNECTOR
Connector is male and is CSI PN 9889 (Conxall #6282-6PG-522 or
Switchcraft #EN3C6M). Pin 1 is indicated w/ a dot
Pin Description
1 3HI Single-ended channel 5 or high side of differential channel
3
2 3LO Single-ended channel 6 or low side of differential channel
3
3 +12V +12 Volt dc supply
4 C4 Control port 4
5 C3 Control port 3
6 Gnd Power ground
TEMP/RH CONNECTOR
Connector is male and is CSI PN 9889 (Conxall #6282-6PG-522 or
Switchcraft #EN3C6M). Pin 1 is indicated w/ a dot
Pin Description
1 1HI Single-ended channel 1 or high side of differential channel
1
2 1LO Single-ended channel 2 or low side of differential channel
1
2 1Kohm Pin 2 also connects to ground via a 1 Kohm 0.1% 10 ppm/C
resistor
3 empty
4 +12Vsw Switched +12 volt dc supply
5 Gnd Ground
6 Gnd Power ground
C-3
Appendix C. CS110 Connector Pin-outs
This is a blank page.
C-4
Appendix D. Servicing the CS110
The CS110 has been designed to provide reliable electric fie ld measure me nts and
to simplify and minimize maintenance. An exploded view illustrat ing t he vari ous
major components of the CS110 is illustrated in Fig ure D-1.
Desiccant Holder Bracket
Interface Plate
CS110 Panel Board
CR1000 Datalogger
CS110 Case
Case Lid
Lid gasket
Motor Assem bl y
FIGURE D-1. Exploded View of CS110 Electric Field Meter
D.1 Lid Gasket
Whenever removing the CS110 case lid inspect the lid gasket for damage and
replace (PN: #17533) in order to form a good seal.
D.2 Changing Out the CR1000
The CR1000 datalogger is accessible in the CS110 by removing the case lid. The
CR1000 is secured to the CS110 via the desiccant holder bracket along with the
two thumb screws on the CR1000 module. Light prying on the CR1000 module
is required to unplug the three 40-pin con nectors that interface to the CS110 panel
board, after removing the two thumb screws on the CR1000 module.
When installing a CR1000 into the CS110 case, first check f or proper orien tat ion
of the three 40-pin connectors that interface to the CS110 panel board. Onc e
D-1
Appendix D. Servicing the CS110
proper connector orientation is verified, set the CR1000 into the CS11 0 case and
feel for proper positioning of the three 40-pin connectors. When the connector
shrouds are engaged, press down firmly on the CR1000 to mate the connector
pins, prior to engaging the two thumb screws on the CR1000 module. Replace
the desiccant holder bracket and desiccant after tighte nin g the thum b screw s.
D.3 Changing Out Motor Assembly
First remove the CR1000 by removing th e desiccant holder bracket along with the
two thumb screws on the CR1000 module. Next remove the black anodized
interface plate between the CR1000 and CS11 0 pane l boar d. Unplug the three
locking electrical connectors on the CS110 panel board from the motor assembly.
Remove the stator by loosening the 2 Philips head screws located on the
underside of the CS110. Next remove the four Philips head screws that attach the
motor assembly to the white powder-coated aluminium case. With the four
screws removed, carefully break it free from the bond to the gasket and allow it to
be removed through the bottom of the CS110 case. Be sure to check the integrity
of the motor assembly gasket on the CS110 case before replacing the motor
assembly.
NOTE
Replacement of the motor assembly invalidates the factory
calibration of a CS110 because of possible dimensional differences
between assemblies.
D.4 Changing Out the CS110 Panel Board Assembly
First remove the CR1000 by removing th e desiccant holder bracket along with the
two thumb screw on the CR1000 mod ule. Next remove the black anodized
interface plate between the CR1000 and CS11 0 pane l boar d.
Next remove the mounting posts that support the black anodized interface plate
followed by the two Phillips head screws by the motor assembly that attach the
CS110 panel board PCB to the CS110 case. Disconnect the three locking
electrical connectors that connect signals between the CS110 panel board and the
motor assembly. Next remove the plastic nuts from the circular connectors on the
outside of the CS110 case. The CS110 panel boar d should now be free and can
be manoeuvred out of the case.
Reverse the above procedure when install ing a CS 110 pane l board P CB. Make
sure that the circular connectors each have a functional o-ring before placing the
CS110 panel board inside the CS110 case. The plastic nuts on the circular
connectors should be tightened to a torque of 10-12 inch⋅lbs.
Readers are referred to Section 10 on Maintenance for instructions on how to
clean the CS110 electrodes and change desiccant in the sealed CS110 case.
D.5 Shutter/Encoder Alignment
D-2
A factory trim is done to align the position of the CS110 shutter with an Index
mark on the rotary position encoder. Re-trimming of the shutter/encoder
alignment becomes necessary after encoder disassembly. The procedure to trim
the shutter/encoder alignment uses a CS110 single-step trim instruction called
CS110Trim. This instruction allows a single shut ter step open (fla g 1) and
closed (flag 2) utilizing the flag capability in LoggerN e t. The fol low ing C S110
program listing (CS110_Index_Trim.cr1) is for trimming the Index mark to the
fully closed shutter position.
Appendix D. Servicing the CS110
'CS110 program to trim index to fully closed shutter position (CS110_Index_Trim.cr1).
' Index/shutter trim procedure fol lows:
' 1. Take at least 8 full-steps open via flag(1) in order to synchronize
' motor coils with motor controller phase state.
' 2. Open shutter to the fully opened position via flag(1) and flag(2).
' 3. Utilizing flag(3) drop into scan that fully closes shutter with 25 full steps.
' 4. Monitor index output on o-scope or vo ltmeter and trim encoder adjustment so that
' Index = 5 V in fully closed position.
' 5. Take a step open (flag(1)) and then closed (flag(2)) and verify park on Index.
' Updated last by Jody Swenson on 7/15/04.
Public Flag(3)
Public I
Public Battery
Public Panel_Temp
BeginProg
Scan(10,msec,0,0)
If Flag(1) Then
CS110Trim(1) 'Take a step open.
Flag(1) = 0 'Reset Flag 1.
EndIf
If Flag(2) Then
CS110Trim(-1) 'Take a step closed.
Flag(2) = 0 'Reset Flag 2.
EndIf
If Flag(3) Then 'Exit scan via Flag 3.
Flag(3) = 0
ExitScan
EndIf
NextScan
Scan(1000,msec,0,0)
For I = 1 To 25 'Loop to fully close a fully opened shutter.
CS110Trim(-1) 'Take a step closed.
Delay (0,10,mSec)
Next I
ExitScan
NextScan
Scan(10,msec,0,0)
If Flag(1) Then
CS110Trim(1) 'Take a step open.
Flag(1) = 0 'Reset Flag 1.
EndIf
If Flag(2) Then
CS110Trim(-1) 'Take a step closed.
Flag(2) = 0 'Reset Flag 2.
EndIf
NextScan
EndProg
The CS110_Index_Trim.cr1 program uses flags 1, 2 and 3 available in
LoggerNet, for user control. Flags 1 and 2 are used to single step the shutter one
step open and closed, respectively. These flags are used initially to position the
shutter into the fully opened position, as observed visually by stator to shutter
overlap.
D-3
Appendix D. Servicing the CS110
se
e
NOTE
At least 8 consecutive open (flag 1) initiated motor steps should
occur prior to arriving at the fully open position in order to
guarantee synchronization between the motor controller phase state
and the stepper-motor coils being energized.
Stator to shutter overlap exists in the full y opened and fully closed positions so
that slight shutter position variations do not alter the measured result. A fully
opened shutter will display symme trical stator to shutter overlap, within the 1.8°
stepper motor step size, on both edges of each of the 4 openings in the stator.
Once the shutter has been adjusted to the fully open position by means of flags 1
and 2, flag 3 is to be set high to execute a 25 closed step loop, which positions the
shutter in the fully closed position, which is the desired position for the Index
trim. No visible gaps between the sta tor and shutter blades should be visible in
the fully closed shutter position. Once in the fully closed position, hook an
oscilloscope or dc voltmeter to the Index test pin on the CS110 pa nel PC B. The
Ports and Flags button on the LoggerNet connect screen along with a graphical
display can also be used for trimming if the update interval is set to 50 ms.
Connector
Locking Plate
Motion of Encoder
Ba
Plat
D-4
Encoder Base
Plate
FIGURE D-2. CS110 Motor Assembly
Appendix D. Servicing the CS110
Referring to Figure D-2, loosen the 2 Philips head screws on the connector
locking plate on the top of the motor assembly. Slowly rotate the encoder base
plate until Index (Control Port # 8) always equals 5 V (5 V = True = Green in
LoggerNet). Tighten down the 2 P hilips head screws on the connector locking
plate and verify that Index still eq uals 5 V. Using flags 1 and 2, move the motor a
step away from and then back to the fully closed position and verify that Index
equals 5 V for the fully closed position.
The CS110Shutter instruction can be used to open, pause and then close the
CS110 shutter to allow visual inspection/ve rification of proper opened and closed
shutter positions. The following CS110 program can be used to verify pr oper
opening and closing of the shutter. Stator to shutter overlap exists in the fully
opened and fully closed positions so that slight shutter position variations do not
alter the exposed area to the sense elec trode. A fully opened shutter will display
symmetrical stator to shutter overlap, within the 1.8° stepper motor step size, on
both edges of each of the 4 openings in the stator. No visible gaps between the
stator and shutter blades should be visible on a fully closed shutter.
'Program to open/close the CS110 shutter (CS110_Shutter1.cr1).
'Last updated by Jody Swenson on 9/26/05.
Scan(5000,msec,0,0)
PanelTemp(PTemp,250)
Battery(Batt)
CS110Shutter(stat(1),1) 'Fully open shutter.
Delay (0,3000,mSec)
CS110Shutter(stat(2),0) 'Fully close shutter.
CallTable Efield
NextScan
EndProg
D-5
Appendix D. Servicing the CS110
D.6 Motor O-ring Seal
NOTE
A double-seal O-ring is located on the motor shaft underneath the CS110 shutter
to help seal the CS110 case. Use Allen head screwdriver to remove the 1
screw and loosen the second (primary) set screw in the shutter hub, in order to
access and replace the motor O-ring. The motor O-ring slides on a UHMW
washer for reduced friction and w ear.
Apply a thin layer of Parker Super O- lube silicone base grease (or equivalent) to
O-ring. Wipe off excess. Install O-ring on shaft. Clean excess grease off the shaft.
After replacing the motor O-ring, the CS110 shutter is installed to compress the
O-ring. When replacing the shutter, line u p the set screw hole so that it is
perpendicular to the flat surface on the motor shaft. The shutter should then be
compressed by applying a precise force. Campbell Scientific part number 010345
is used to apply the precise force. A second shutter hub set screw is used to
prevent the primary shutter hub set screw from working loose during operation.
Removal and replacement of the shutter from the motor shaft
necessitates a check and possibly re-trimming of the Index to the
fully closed position as described in Shutter/Encoder alignment.
Removal and replacement of the shutter also invalidates the factory
calibration because of possible dimensional differences when
reassembled.
st
set
D-6
Appendix E. CS110 as a Slow Antenna
As previously mentioned the CS110 can sample the external electric field at a
maximum rate of 5 Hz (200 ms) using the CS110 instruction. Faster sampling of
the rapid electric field changes associated with lightning discharges is desirable in
some applications, and can be accomplished with the CS110 electric field meter
configured as a Slow Antenna which is sometimes c alled a field change meter.
E.1 Response of the CS110 Slow Antenna in the
Frequency Domain
The CS110 as a Slow Antenna with the 25 0 µs integration responds to events as
shown in Figure E-1. The lower frequency limit is due to the measurement
circuitry and the upper frequency limit is a function of the integration time . Both
are explained below.
The CS110Shutter instruction can be used to fully open the shutter, indefinitel y
exposing the sense electrode to external fields. Execution of the CS110Shutter
instruction with the “open” command changes the CS1 10 panel boa rd cha rge
amplifier circuitry to a slow antenna by switching in a 200 MΩ resistor in parallel
with the 330 pF feedback capacitor, resulting in a (330pF)⋅(200MΩ) = 66 ms
decay time constant. In this slow ante nna configuration the charge amplifier has
a high-pass filter frequency response with the lower cut-off frequency defined by
the decay time constant such that f
events with frequencies higher than 2. 4 Hz (shorter than 417 ms) are “passed
through” while lower frequency events are “cut off” (search “cut-off frequency”
in Wikipedia). The -3dB point for voltage is:
= (2⋅π⋅R⋅C)-1 = 2.4 Hz. This means that
3dB
The CS110 can measure the slow antenna output at rates up to 50 Hz (100 Hz
may be possible but it has not been tested), using the fast integration (250 μs
integration) for the VoltDiff instruction. Voltage measurements using the 250 μs
integration duration for the analogue integrator, result in an upper 3 dB bandw idth
of 1.8 kHz (0.555 ms). Figure E-1 shows the combined effect of both filters.
− 10/3
103dB
trueof 0.708==−
E-1
Appendix E. CS110 as a Slow Antenna
Overall Frequency Response of CS110 Slow-Antenna Measurement with 250 us Integration
0.999
1
0.833
0.667
MagSys f()
Relative Magnitude
0
0.5
0.333
0.167
0
0.11101001103×1104×
f
Frequency (Hz)
Figure E-1. CS110 slow antenna frequency response.
100000.1
E-2
Appendix E. CS110 as a Slow Antenna
E.2 Response of the CS110 Slow Antenna in the Time
Domain
The following graphs shows one lightning strike measured at 50 Hz by both the
CS110 slow antenna and by one of Kennedy Space Centre’s (KSC) field mills. In
Figure E-3 the KSC electric field meter readings have been converted to efield
change per measurement.
Figure E-2. KSC electric field and CS110 slow antenna data.
E-3
Appendix E. CS110 as a Slow Antenna
Figure E-3. KSC electric field change and CS110 slow antenna data.
The KSC electric field mill and the CS110 were not precisely synced accounting
for some of the differences in the data shown in the above graph. Since that time,
the CS110 has been improved and now has the ability to sync to within ±10 µs of
the GPS signal’s PPS pulse. The resolution of accuracy f or the clock set is 10
microseconds if the internal CR1000 datalogger has a hardware revisio n number
greater than 007 (RevBoard field in the datalogger's Status table).
E-4
E.3 Programming
The following CRBasic program utilizes the slow antenna c apa bi lity of the
CS110.
'Program to use the CS110 in slow antenna mode (slowant1.cr1).
'Last updated by Jody Swenson on 9/30/05.
PipeLineMode
Const Mult = 85
Public Delta_E
Public Delta_E_mV2500
Public stat(2)
Public E_field
Public Leakage
BeginProg
CS110 (E_field,Leakage,stat(1),250,Mult,0) 'Measure E_field and leakage.
CS110Shutter(stat(2),1) 'Fully open shutter.
Scan(20,msec,0,0)
VoltDiff (Delta_E,1,mV250,8,False,0,250,Mult,0) 'no input reversal.
VoltDiff (Delta_E_mV2500,1,mV2500,8,False,0,250,Mult,0) 'no input reversal. If Delta_E = NAN Then
Delta_E = Delta_E_mV2500
EndIf
CallTable SlowAnt
NextScan
EndProg
Appendix E. CS110 as a Slow Antenna
In the above program the PipeLineMode instruction enables parallel task
processing necessary to complete a scan in 20 ms. The CS110 instruction
following the BeginProg statement provides a meas ure of the absol ute ele ctric
field along with a leakage current compensation value, and is only executed once.
The CS110Shutter instruction can fully open or fully close the shutter, based on
the whether the 2
are used on two different input voltage ranges to provide more dynamic range in
the charge amplifier output measurement.
The CS110 can be programmed to operate as a field meter and then switch to
operate as a slow antenna. For example, efield measurements may be desired
until they exceed an alarm threshold of ±1500 V/m after which slow antenna
(field change) measurements may be desired. The CR1000 operating system does
not allow the Sequential Mode command and the Pipeline Mode command used
in the above example to exist in the sam e program. For the CS110 to be able to
switch between measuring the e lectric field with the CS110 instruction and the
electric field change in the “slow antenna” mode, the slow antenna instructions
must be run in the Sequential Mode. One way to accomplish this would be to
program the CR1000 to monitor a 1 minute r unning average of the efield and
when it exceeds ±1500 v/m switch to the slow antenna mode for a fixed amount
of time and then return to the field me ter mode.
nd
parameter is a 1, or 0, respectively. Two VoltDiff instructions
E-5
Appendix E. CS110 as a Slow Antenna
E.4 Calibration
The factory calibration described in Section 5 applies to the maximum amplitude
of the step response of the CS110 when it is operating as a slow antenna.
Switching in the 200 MΩ resistor in the feedback path simply slows the decay of
the signal induced on the sense electrode resulting in a 66 millisecond decay time
constant
The CS110 operating as a slow antenna returns the change in the electric field
with units of volts per metre per scan. A 50 Hz scan interval would yield:
X volts * metre
-1
* 20 ms-1.
E-6
Appendix F. Example CRBasic
Programs
An example CS110 weather station program using a variable electric field
measurement rate in order to minimize current consumption in solar powered
applications follows.
'CS110 efield and weather station program with variable measurement
'rate for low-power consumption.(CS110_low_power.cr1).
'Measures rainfall, wind speed and direction, solar radiation,
'relative humidity, air temperature, and electric field.
'Updated last by Jody Swenson on 9/18/04 for Mparallel_plate and Csite.
const Mparallel_plate = 85
const Csite = 0.10 'Approximate value for weather station site.
const Mcorrected = Mparallel_plate* Csite 'Mcorrected is multiplier for CS110 instruction.
const SLOW_INTERVAL = 10
const FAST_INTERVAL = 1
Public E_field
Units E_field=volts/m
Public battery_volt
Public leakage_cur
Units leakage_cur=nA
Public status
Public panel_temp
Units panel_temp=DegF
Public rain_fall
Units rain_fall=inch
Public wind_speed
Units wind_speed=mph
Public wind_dir
Units wind_dir=deg
Public solar_rad
Units solar_rad=W/m2
Public air_temp
Units air_temp=DegF
Public RH
Units RH=%
Public internal_RH
Units internal_RH=%
Public count
Public E_field_int 'Interval to make efield measurement rate
Public run_avg10
Public abs_run_avg600
Public E_status(16) 'Efield status array.
Public k 'Index for E_stat array.
Public meas_error 'Disable va riable for slow table.
F-1
Appendix F. Example CRBasic Programs
DataTable(Tabslow,1,-1) '-1 to auto-allocate all available memory.
DataInterval(0,60,sec,10) 'Averaged 60 second output data.
Average(1,E_field,ieee4,meas_error)
Sample (1,run_Avg10,ieee4)
Totalize (16,E_status,FP2,0) 'Look at Efield status array for last 60 seconds.
Average (1,leakage_cur,FP2,0)
Average(1,panel_temp,FP2,0)
Totalize (1,rain_fall,FP2,0)
WindVector (1,wind_speed,wind_dir,FP2,False,0,0,0)
Average (1,solar_rad,FP2,0)
Average(1,air_temp,FP2,0)
Average (1,RH,FP2,0)
Average (1,battery_volt,FP2,0)
Average (1,internal_RH,FP2,0)
EndTable
DataTable(Tabfast,1,-1) '-1 to auto-allocate all available memory.
Sample(1,E_field,ieee4)
Sample (1,run_Avg10,ieee4)
Sample (1,status,FP2)
Sample (1,leakage_cur,FP2)
Sample (1,rain_fall,FP2)
Sample (1,wind_speed,FP2)
Sample (1,wind_dir,FP2)
Sample (1,solar_rad,FP2)
Sample (1,air_temp,FP2)
Sample (1,RH,FP2)
Sample (1,battery_volt,FP2)
EndTable
BeginProg
E_field_int = FAST_INTERVAL 'Initialize to fast interval.
Scan(1,sec,0,0)
for k = 1 to 16 'Initialize status array.
E_status(k) = 0
next
PanelTemp (panel_temp,250)
panel_temp = panel_temp*1.8 + 32 'Convert to Fahrenheit.
Battery (battery_volt)
VoltDiff (internal_RH,1,mV2500,5,True ,0,250,0.1,0)
PulseCount (rain_fall,1,2,2,0,0.01,0) 'TE525 tipping bucket 0.01 inches per tip.
PulseCount (wind_speed,1,1 ,1,1,0.2192,0) 'Mult for 05103 Wind Monitor.
BrHalf (wind_dir,1,mV2500,4,Vx2,1,2500,False,450,250,355,0) 'Mult. for 05103 Wind Monitor.
VoltDiff (solar_rad,1,mV7_5,3,True,450,250,200,0)
SW12 (1 ) 'Apply switched 12 V power to the probe.
Delay (0,150,mSec) 'Warm up probe before measurements.
VoltSe (RH,1,mV2500,1,1,0,250,0.1,0)
VoltSe (air_temp,1,mV2500,2,1,0,250,.18,-40)
SW12 (0) 'Turn off power to the probe.
if RH > 100 and RH < 108 then
RH = 100
Endif
count = count + 1
if (count >= E_field_int) then
count = 0 'reset the count for SLOW_INTERVAL
meas_error = 0 'Initialize disable variable for Efield average in slow table.
CS110(E_field,leakage_cur,status,_60Hz,Mcorrected,0)
If E_field = NAN Then
meas_error = 1 'Disable output to slow table if efield = NAN.
E_field_int = FAST_INTERVAL 'Go to fast interval if NAN.
F-2
Appendix F. Example CRBasic Programs
EndIf
E_status(status) = 1 'Set appropriate element in status array.
Endif
If E_field <> NAN Then
AvgRun (run_avg10,1,E_field,10) 'Used for average output in fast table.
AvgRun (abs_run_avg600,1,ABS(E_field),600) 'Used to stay longer at fast interval.
EndIf
if (E_field>100 or ABS(E_field)>=300 or abs_run_avg600>=300)and (battery_volt>11.0) then
E_field_int = FAST_INTERVAL
else
E_field_int = SLOW_INTERVAL
EndIf
If E_field_int = FAST_INTERVAL Then
CallTable Tabfast 'Only call fast table when fast efield active
EndIf
CallTable Tabslow 'Call slow every time at slow interval.
NextScan
EndProg
In the above program all measurements, except the electric field measurement, are
done once per second. The electric field measurement is done once every
SLOW_INTERVAL when measured electric field values are between -300 V/m
and +100 V/m as determined by an if statement. The -300 V/m and +100 V/m
values are somewhat arbitrary and can easily be changed to better suit a given
application. When measured electric field values fall outside of the -300 V/m and
+100 V/m range, the electric field measurement rate becomes the
FAST_INTERVAL. A running average instruction (AvgRun) is used to maintain
measurements at the FAST_INTERVAL for some time following elevated electric
fields, even after several near zero measurements.
F-3
Appendix F. Example CRBasic Programs
This is a blank page.
F-4
Appendix G. CS110 2 Metre CM10 Tripod
Site
FIGURE G-1. CS110 2 Metre CM10 Tripod Site
The Tripod_CS110 site consists of the CS110 mounted on the CM10 Tripod at a
height of 2 metres, and an ENC 12/14 enclosure.
The following may affect the site calibration factor, C
site
:
• CM10 Tripod
• CS110 Electric Field Meter
• ENC 12/14 Enclosure
If the above items are installed using the following set of instructions, the site is
level with a 762 cm (25 foot) radius of gravel around the tripod and there are no
obstructions higher than 18 degrees from the centre of a measurement site
2
then
the C
site
determined for this configuration should be valid.
G-1
Appendix G. CS110 2 Metre CM10 Tripod Site
Installation of the Tripod_CS110 Site:
Drive the ground rod into the ground where the centre of the tripod is to be placed.
Extend the tripod legs so the far end of the sliding clamp is 142 cm (56 inches)
from the mast end of the pipe. Extending the legs as described above puts the feet
on a circle with a radius of approximately 196 cm (77 inches) from the centre of
the tripod to the outside edge of the pivoting feet. The distance from the top of the
top collar to the ground will be approximately 102 cm (40 inches). Locate the
centre of the tripod above the ground rod with one leg of the tripod pointing
toward the equator. Level the tripod by removing or adding small amounts of
gravel under the feet as needed.
Apply Teflon tape to both ends of the 3.175 cm (1 ¼ inch) outside diameter mast.
Attach the cap to the top of the mast.
Attach the CS110 mounting bracket to the mast with the top of the bracket about
23.5 cm (9¼ inches) below the top of the cap on the mast but don’t tighten bolts
very tight as it will likely need to be rotated and either raised or lowered slightly.
Mount the completed mast on the tripod.
Adjust the CS110 mounting bracket so the top of the mounting bracket is
approximately 229 cm (90 inches) above the ground and between the two legs
opposite the equator still leaving the bolts not too tight yet. Mount the CS110 on
the mounting bracket. The field meter should now be facing away from the
equator with the face of the stator 200 cm or 78 ¾ inches above the ground.
Tighten the mounting bolts. See Figure G-2.
G-2
Appendix G. CS110 2 Meter CM10 Tripod Site
FIGURE G-2. CS110 on CM10 Tripod Mast
Mount the fibreglass enclosure to the top of the leg facing the equator with the top
bracket approximately 5 cm (2 inches) below the top of the leg. Be careful
opening the lid because in this almost horizontal position it is possible to pull the
hinge rivets out of the enclosure.
If there is a solar panel, install the solar panel on the leg facing the equator below
the enclosure. Tilt the solar panel at an angle less than horizontal that is equal to
the latitude plus 10 degrees (see solar panel manual).
Ground the CS110 Electric Field Meter (Figure G-2), the tripod, and the battery
(through the enclosure ground) with three separate ground wires as shown in
Figure G-3. Power and communication cables should be run down the equator
side of the mast and under the enclosure as shown. Wire-tie all cables into place
so they don’t move with the wind.
G-3
Appendix G. CS110 2 Metre CM10 Tripod Site
FIGURE G-3. Earth Grounding
Stake the tripod to the ground and/or weigh it down with sand bags.
Determination of C
site
Surface mounted upward facing CS110: SN1022 with M
parallel_plate
= 87.6
Tripod with CS110 only: SN1023 with M
parallel_plate
= 81.77
Each CS110 recorded one minute averages of 1 second measurements of electric field
data for the same 2200 to 2300 hour time period on October 2, 2005. The data from
both units is plotted in Figure G-4. A best-fit line was computed. The linear
regression yields a C
site
= 0.105 for the Tripod CS110 Only Site.
G-4
Appendix G. CS110 2 Meter CM10 Tripod Site
Site Correction for Tripod CS110 Only Site - October 2, 2005
1 minute average of 1 second data
Results indicate Csite = 0.105.
y = 0.1051x - 35.664
R
2
= 0.9996
-10000
-8000
-6000
-4000
-2000
0
2000
4000
6000
8000
-80000-60000-40000-20000020000400006000080000
Uncorrected (Csite = 1) Electric Field (volt/meter) for Tripod CS110 Only site
Tripod CS110 Only Uncorrected E_Field 1_Min_Avg volts/m
Linear (Tripod CS110 Only Uncorrected E_Field 1_Min_Avg
FIGURE G-4. Determination of C
site
G-5
Appendix G. CS110 2 Metre CM10 Tripod Site
This is a blank page.
G-6
Appendix H. Tripod CS110 and
StrikeGuard Site
H.1 Tripod CS110 and StrikeGuard
FIGURE H-1. Tripod CS110 and StrikeGuard
The Tripod CS110 and StrikeGuard Site includes the following that affect C
site
:
• CM10 Tripod
• StrikeGuard Lightning Detector
• CS110 Electric Field Meter
• ENC 12/14 Enclosure
If the above items are installed using the following set of instructions, the site is
level with a 25 foot radius of gravel around the tripod and there are no
obstructions higher than 18 degrees from the centre of a measurement site
2
then
the C
site
determined for this configuration should be valid.
H-1
Appendix H. Tripod CS110 and StrikeGuard Site
H.1.1 Installation of the Tripod CS110 and StrikeGuard Site
Drive the ground rod into the ground where the centre of the tripod is to be placed.
Extend the tripod legs so the far end of the sliding clamp is 142 cm (56 inches)
from the mast end of the pipe. Extending the legs as described above puts the feet
on a circle with a radius of approximately 196 cm (77 inches) from the centre of
the tripod to the outside edge of the pivoting feet. The distance from the top of the
top collar to the ground will be approximately 102 cm (40 inches). Locate the
centre of the tripod above the ground rod with one leg of the tripod pointing
toward the equator. Level the tripod by removing or adding small amounts of
gravel under the feet as needed.
Apply Teflon tape to both ends of the 3.175 cm (1 ¼ inch) outside diameter mast.
Attach the cap to the top end of the mast.
Attach the CS110 mounting bracket to the mast with the top of the bracket about
23.5 cm (9¼ inches) below the top of the cap on the mast but don’t tighten bolts
very tight as it will likely need to be rotated and either raised or lowered slightly.
Mount the completed mast and cross arm on the tripod.
Adjust the CS110 mounting bracket so the top of the mounting bracket is
approximately 229 cm (90 inches) above the ground and between the two legs
opposite the equator still leaving the bolts not too tight yet. Mount the CS110 on
the mounting bracket. The field meter should now be facing away from the
equator with the face of the stator 200 cm or 78 ¾ inches above the ground.
Tighten the mounting bolts. See Figure H-2.
Mount the StrikeGuard Lightning Detector to the top of the mast on the equator
side of the mast with the top of the mounting bracket butted up against the cap on
the top of the mast.
FIGURE H-2. CS110 and StrikeGuard on Tripod Mast
H-2
Appendix H. Tripod CS110 and StrikeGuard Site
Mount the fibreglass enclosure to the top of the leg facing the equator with the top
bracket approximately 5 cm (2 inches) below the top of the leg. Be careful
opening the lid because in this almost horizontal position it is possible to pull the
hinge rivets out of the enclosure.
If there is a solar panel, install the solar panel on the leg facing the equator below
the enclosure. Tilt the solar panel at an angle less than horizontal that is equal to
the latitude plus 10 degrees (see solar panel manual).
Ground the CS110 Electric Field Meter (Figure H-3), the tripod, and the battery
(through the enclosure ground) with three separate ground wires as shown in
Figure H-4.
FIGURE H-3. Grounding the CS110 Grounding Strap
H-3
Appendix H. Tripod CS110 and StrikeGuard Site
FIGURE H-4. Grounding the Tripod and Battery
Stake the tripod to the ground or weight it down with sand bags.
Connect power and communication cables as shown in Figure H-5.
H-4
Appendix H. Tripod CS110 and StrikeGuard Site
FIGURE H-5. Connections for Combined System
Power and communication cables should be run down the equator side of the mast
and under the enclosure as shown. Wire-tie all cables into place so they don’t
move with the wind.
H-5
Appendix H. Tripod CS110 and StrikeGuard Site
H.1.2 Determination of C
site
Surface mounted upward facing CS110: SN1022 with M
parallel_plate
= 88.31.
CM10 Tripod Mounted StrikeGuard and CS110: SN1023 with M
parallel_plate
= 81.77.
Each CS110 recorded one minute averages of 1 second measurements of electric field
data for the same one hour time period from 3 AM to 4 AM on August 11, 2005. The
data from both units is plotted in Figure H-6. A best-fit line was computed. The
linear regression yields a C
site
= 0.108 for the Tripod CS110 and StrikeGuard Site.
Site Correction for CS110/StrikeGuard on CM10 Tripod August 11, 2005
1 minute average of 1 second samples
Results indicate Csite = 0.108
y = 0.1079x - 64.062
R
2
= 0.9994
-4000
-2000
0
2000
4000
6000
8000
10000
-40000-20000020000400006000080000100000
Uncorrected Electric Field (volts/meter) for CM10 tripod mounted StrikeGuard & 2 Meter CS110