TheCS547 CONDUCTIVITY AND TEMPERATURE PROBE AND A547
INTERFACE are warranted by CAMPBELL SCIENTIFIC, INC. to be free
from defects in materials and workmanship under normal use and service for
twelve (12) months from date of shipment unless sp ecified otherwise. Batteries
have no warranty. CAMPBELL SCIENTI F IC, INC.'s obligation under this
warranty is limited to repairing or replacing (at CAMPBELL SCIENTIFIC,
INC.'s option) defective products. The customer shall assume all costs of
removing, reinstalling, and shipping defective products to CAMPBELL
SCIENTIFIC, INC. CAMPBELL SCIENTIFIC, INC. will return such
products by surface carrier prepaid. This warranty shall not apply to any
CAMPBELL SCIENTIFIC, INC. products which have been subjected to
modification, misuse, neglect, accidents of nature, 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, INC. is not liable for special, indirect, incidental, or
consequential damages.
Products may not be returned without prior authorization. The following
contact information is for US and International customers residing in countries
served by Campbell Scientific, Inc. directly. Affiliate companies handle repairs
for customers within their territories. Please visit www.campbellsci.com to
determine which Campbell Scientific company serves your country. To obtain
a Returned Materials Authorization (RMA), contact CAMPBELL
SCIENTIFIC, INC., phone (435) 753-2342. After an applications engineer
determines the nature of the problem, an RMA number will be issued. Please
write this number clearly on the outside of the shipping container.
CAMPBELL SCIENTIFIC's shipping address is:
CAMPBELL SCIENTIFIC, INC.
RMA#_____
815 West 1800 North
Logan, Utah 84321-1784
CAMPBELL SCIENTIFIC, INC. does not accept collect calls.
CS547 Probe and A547 Interface
Table of Contents
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CS547 Conductivity and Temperature
Probe and A547 Interface
1. Overview
The CS547 conductivity and temperature probe, and A547 interface are designed
for measuring the electrical conductivity, dissolved solids, and temperature of
fresh water with Campbell Scientific dataloggers. They require the use of AC
excitation, so they can be used with the CR10(X), 21X, and CR7 dataloggers but
not with the BDR301 or BDR320. Use with multiplexers is possible.
Electrical conductivity (EC) of a solution is a simple physical property, but
measurements can be difficult to interpret. This manual instructs the user how to
make EC measurements with the CS547. Accuracy specifications apply to
measurements of EC in water containing KCl, Na
which are typical calibration compounds, and to EC not yet compensated for
temperature effects.
Statements made on methods of temperature compensation or estimating dissolved
solids are included to introduce common ways of refining and interpreting data, but
are not definitive. Authoritative sources to consult include the USGS Water-Supply
Paper 1473, The pH and Conductivity Handbook published by OMEGA
Engineering, physical chemistry texts, and other sources.
, NaHCO3, and/or NaCl,
2SO4
1.1 EC Sensor
The EC sensor consists of three stainless steel rings mounted in an epoxy tube
as shown in Figure 4-1. Resistance of water in the tube is measured by
excitation of the center electrode with positive and negative voltage.
This electrode configuration eliminates the ground looping problems associated
with sensors in electrical contact with earth ground.
Temperature is measured with a thermistor in a three wire half bridge
configuration.
1.2 A547 Interface
The interface contains the completion resistors and blocking capacitors. The
interface should be kept in a non-condensing environment that is maintained
within the temperature range of the unit.
1
CS547 Conductivity and Temperature Probe and A547 Interface
e
DATALOGGER
AG
SE TEMP
EX TEMP
EX COND
HI COND
LO COND
SHIELD
SHIELD
SENSOR
TEMP
COND
EX COND
EX TEMP
A547 INTERFACE
Logan, Utah
MADE IN USA
FIGURE 1-1. A547 Interface and CS547 Conductivity and Temperature Probe
2. Specifications
2.1 CS547 Probe
Construction
Size
Maximum Cable
Length
Depth Rating
pH Range
The prob e housing is stainless steel
Probe Length: 3.7 inches (94 mm)
Diameter: 0.95 inches (24.13 mm)
1000 ft. The sensor must be ordered with desired length
as cable cannot be added to existing probes.
Maximum 1000 feet
Solution pH of less than 3.0 or greater than 9.0 may damag
the stainless steel ho using.
Electrodes
Cell Constant
Temp. Range of Use
EC Range
Accuracy
2.2 A547 Interface
Size
Temperature Rating
Passivated 316 SS with DC isolation capacitors.
Individually calibrated. The cell constant (K
) is found on
c
a label near the termination of the cable.
0° to 50°C.
Approx. 0.005 to 7.0 mS cm
in KCl and Na
, NaHCO3, and NaCl standards at
2SO4
-1
.
25°C:
±5% of reading 0.44 to 7.0 mS cm
±10% of reading 0.005 to 0.44 mS cm
-1
.
-1
.
Dimensions: 2.5” x .875” x 1.750
Weight: 6 oz.
-15°C to +50°C
2
CS547 Conductivity and Temperature Probe and A547 Interface
2.3 Temperature Sensor
3. Installation
CAUTION
3.1 Site Selection
3.2 Mounting
Thermistor
Range
Accuracy
Rapid heating and cooling of the probe, such as leaving it
in the sun and then submersing it in a cold stream, may
cause irreparable damage.
The EC sensor measures the EC of water inside the stainless steel tube, so
detection of rapid changes in EC requires that the probe be flushed
continuously. This is easy to accommodate in a flowing stream by simply
orienting the sensor parallel to the direction of flow. In stilling wells and
ground wells, however, diffusion rate of ions limits the response time.
The stainless steel housing and sensor cable are made of water impervious,
durable materials. Care should be taken, however, to mount the probe where
contact with abrasives and moving objects will be avoided. Strain on cables
can be minimized by using a split mesh strain relief sleeve on the cable, which
is recommended for cables over 100 ft. The strain relief sleeve is available
from Campbell Scientific as part number 7421.
Betatherm 100K6A1.
0°C to 50°C.
Error ±0.4°C (See Section 8.2).
4. Wiring
WARNING
The A547 is usually mounted in the datalogger enclosure.
The excitation channel used for EC must be separate
from the one used for temperature or measurement
errors will result.
3
CS547 Conductivity and Temperature Probe and A547 Interface
FIGURE 4-1. CS547 Wiring Diagram for Example Below
5. Programming
5.1 Programming Overview
AG
SE3
EX2
EX1
1H
1L
Clear (Shield)
Red (Temp)
Orange (Cond)
Black (Ex Cond)
Green (Ex Temp)
AG
SE TEMP
EX TEMP
EX COND
HI COND
LO COND
SHIELD
SHIELD
TEMP
COND
EX COND
EX TEMP
DATALOGGERSENSOR
Typical datalogger programs to measure the CS547 consist of four parts:
1.Measurement of EC and temperature
2.Correction of ionization errors in EC measurements
3.Correction of temperature errors in EC measurements
4.Output processing
All example programs may require modification by the user to fit the specific
application's wiring and programming needs. All example programs in this
manual are for the CR10(X) and assume that datalogger wire connections are as
follows: the LO COND lead is connected to 1L, the HI COND to 1H, the EX
COND to EX1, the EX TEMP to EX2, and the SE TEMP to SE3 .
5.2 Measurement Programming.
EC: Results from Instructions 5 or 6 (chosen automatically as part of the
autoranging feature of the following program segment) are processed with
Instruction P59 to produce the resistance across the electrodes:
Input Location Labels
Definitions for the following program:
Rs Solution resistance
RpResistance of leads/cable and blocking caps
CtSolution EC with no temp. correction
C25mScm_1EC corrected for temperature
4
CS547 Conductivity and Temperature Probe and A547 Interface
*Table 1 Program
01: 5Execution Interval (seconds)
;Make a preliminary measurement of resistance for autoranging.
1: Full Bridge (P6)
1: 1Reps
2: 15±2500 mV Fast Range
3: 1DIFF Channel
4: 1Excite all reps w/Exchan 1
5: 2500mV Excitation
6: 1Loc [ Rs ]
7: -.001Mult
8: 1Offset
2: BR Transform Rf [X/(1-X)] (P59)
1: 1Reps
2: 1Loc [ Rs ]
3: 1Multiplier (Rf)
;
;Test the initial measurement to make a more accurate measurement.
;
3: CASE (P93)
1: 1Case Loc [ Rs ]
4: If Case Location < F (P83)
1: 1.8F
2: 30Then Do
5: AC Half Bridge (P5)
1: 1Reps
2: 15±2500 mV Fast Range
3: 2SE Channel
4: 1Excite all reps w/Exchan 1
5: 2500mV Excitation
6: 1Loc [ Rs ]
7: 1.0Mult
8: 0.0 Offset
6: BR Transform Rf[X/(1-X)] (P59)
1: 1Reps
2: 1Loc [ Rs ]
3: 1Multiplier (Rf)
7: End (P95)
8: If Case Location < F (P83)
1: 9.25F
2: 30Then Do
(cont.)
5
CS547 Conductivity and Temperature Probe and A547 Interface
9: Full Bridge (P6)
1: 1Reps
2: 15±2500 mV Fast Range
3: 1DIFF Channel
4: 1Excite all reps w/Exchan 1
5: 2500mV Excitation
6: 1Loc [ Rs ]
7: -.001Mult
8: 1Offset
10: BR Transform Rf[X/(1-X)] (P59)
1: 1Reps
2: 1Loc [ Rs ]
3: 1Multiplier (Rf)
11: End (P95)
12: If Case Location < F (P83)
1: 280F
2: 30Then Do
13: Full Bridge (P6)
1: 1Reps
2: 14±250 mV Fast Range
3: 1DIFF Channel
4: 1Excite all reps w/Exchan 1
5: 2500mV Excitation
6: 1Loc [ Rs ]
7: -.001Mult
8: 1Offset
14: BR Transform Rf[X/(1-X)] (P59)
1: 1Reps
2: 1Loc [ Rs ]
3: 1Multiplier (Rf)
15: End (P95)
16: End (P95)
;
;Subtract resistance errors (Rp) caused by the blocking capacitors
;(0.005Kohm) and the cable length (0.000032kohm/ft). Enter cable lead
;length in nnn below.
;
17: Z=F (P30)
1: nnnFEnter cable length in feet.
2: 00Exponent of 10
3: 5Z Loc [ Rp ]
18: Z=X*F (P37)
1: 5X Loc [ Rp ]
2: .00032F
3: 5Z Loc [ Rp ]
(cont.)
6
CS547 Conductivity and Temperature Probe and A547 Interface
19: Z=X*F (P37)
1: 5X Loc [ Rp ]
2: -.1F
3: 5Z Loc [ Rp ]
20: Z=X+F (P34)
1: 5X Loc [ Rp ]
2: -.005F
3: 5Z Loc [ Rp ]
21: Z=X+Y (P33)
1: 1X Loc [ Rs ]
2: 5Y Loc [ Rp ]
3: 1Z Loc [ Rs ]
;
;EC is then calculated by multiplying the reciprocal of resistance,
;which is conductance, by the cell constant.
;
NOTE: The cell constant (Kc) is printed on the label of each sensor or it can be calculated
(see Section 6.4). It is entered in place of nnn below.
22: Z=1/X (P42)
1: 1X Loc [ Rs ]
2: 2Z Loc [ l_over_Rs ]
23: Z=X*F (P37)
1: 2X Loc [ l_over_Rs ]
2: nnnFEnter cell constant.
3: 3Z Loc [ Ct ]
Temperature: Temperature is measured with a single instruction, P11, that
measures the thermistor resistance and calculates temperature. Output is °C
when a multiplier of 1 and an offset of 0 is used. See Section 10 of datalogger
manual for detailed information on the function of Instruction P11.
5.3 Correction of Ionization Errors in EC Measurement
Ionization caused by the excitation of the EC sensor can cause large errors.
Campbell Scientific has developed a linear correction for conductivity between
0.005 and 0.44 mS cm
0.44 and 7.0 mS cm
containing KCl, Na
-1
, and a quadratic correction for conductivity between
-1
. Corrections were determined in standard salt solutions
, NaHCO3, and NaCl.
2SO4
(cont.)
(cont.)
7
CS547 Conductivity and Temperature Probe and A547 Interface
The following program segment automatically chooses which correction to
apply to the measurement.
;
;The following program set corrects for errors of ionization in the EC
;measurement.
;
The effect of temperature on the sample solution can cause large errors in the
EC measurement. A simple method of correcting for this effect is to assume a
linear relationship between temperature and EC. This method generally
produces values to within 2% to 3% of a measurement made at 25°C.
The best corrections are made when the temperature coefficient is determined
at a temperature near field conditions. See Section 9 for details on how to
determine the temperature coefficient. If determining the temperature
coefficient is not possible, use a value of 2%/°C as a rough estimate.
(cont.)
The following program segment implements a previously determined
temperature coefficient (TC) and calculates the corrected conductivity.
8
CS547 Conductivity and Temperature Probe and A547 Interface
;This next program set will correct errors in the EC measurement resulting
;from temperature differences.
;
31: Z=X+F (P34)
1: 4X Loc [ Temp_degC ]
2: -25F
3: 6Z Loc [ A ]
32: Z=X*F (P37)
1: 3X Loc [ Ct ]
2: 100F
3: 7Z Loc [ lOO_Ct ]
33: Z=X*F (P37)
1: 6X Loc [ A ]
2: nnnFEnter TC (%/°C) to correct cond. reading.
3: 8Z Loc [ TC_Proces ]
34: Z=X+F (P34)
1: 8X Loc [ TC_Proces ]
2: 100F
3: 8Z Loc [ TC_Proces ]
35: Z=X/Y (P38)
1: 7X Loc [ lOO_Ct ]
2: 8Y Loc [ TC_Proces ]
3: 9Z Loc [ C25mScm_l ]EC corrected for temperature.
5.5 Output Processing
Over large ranges, EC is not linear and is best reported as samples using
instruction P70. In limited ranges, averaging (P71) measurements over time
may be acceptable. Convention requires that the temperature at the time of the
measurement be reported.
;Output processing, convention states that the temperature be reported
;with the EC measurement.
;
36: Do (P86)
1: 10Set Output Flag High (Flag 0)
37: Sample (P70)
1: 1Reps
2: 3Loc [ Ct ]
38: Sample (P70)
1: 1Reps
2: 4Loc [ Temp_degC ]
(cont.)
39: Sample (P70)
1: 1Reps
2: 9Loc [ C25mScm_l ]
(cont.)
9
CS547 Conductivity and Temperature Probe and A547 Interface
*Table 2 Program
02: 0.0Execution Interval (seconds)
*Table 3 Subroutines
End Program(End)
6. Calibration
6.1 Conversion Factors
1 S (Siemens) = 1 mho = 1/ohm
-1
Although mS·cm
unit is S·m
EC measurements can be used to estimate dissolved solids. For high accuracy,
calibration to the specific stream is required. However, for rough estimates,
values between 550 and 750 mg·l
generally being associated with waters high in sulfate concentration (USGS
Water-Supply Paper #1473, p. 99). A common practice is to multiply the EC in
mS·cm
-1
-1
by 500 to produce ppm or mg·l-1.
and µS·cm-1 are the commonly used units of EC, the SI base
. The result of the example programs is mS·cm
-1
-1
/ mS·cm-1 are typical with the higher values
6.2 Typical Ranges
Single distilled water will have an EC of at least 0.001 mS·cm-1. ECs of melted
snow usually range from 0.002 to 0.042 mS·cm
range from 0.05 to 50.0 mS·cm
water (USGS Water-Supply Paper 1473, p. 102).
6.3 Factory Calibration
The CS547 is shipped with a cell constant calibrated in a 0.01 molal KCl
solution at 25.0°C ±0.05°C. The solution has a EC of 1.408 mS cm
6.4 Field Calibration
The cell constant is a dimensional number expressed in units of cm-1. The unit
-1
is slightly easier to understand when expressed as cm·cm-2. Because it is
cm
dimensional, the cell constant as determined at any one standard, will change
only if the physical dimensions inside the CS547 probe change. Error due to
thermal expansion and contraction is negligible. Corrosion and abrasion,
however, have the potential of ca using significant errors.
A field calibration of the CS547 cell constant can be accomplished as follows:
1.Make a 0.01 molal KCL solution by dissolving 0.7456 g of reagent grade
KCl in 1000 g of distilled water, or purchase a calibration solution.
-1
-1
, the higher value being close to the EC of sea
. ECs of stream water usually
-1
.
10
2.Clean the probe thoroughly with the bl ack nylon brush shipped with the
CS547 and a small amount of soapy water. Rinse thoroughly with distilled
water, dry thoroughly, and place in the KCl solution.
CS547 Conductivity and Temperature Probe and A547 Interface
3.Connect the CS547 and A547 or probe and interface to the datalogger
using the wiring described in Section 4. Enter the following program into
the datalogger.
The calibration solution temperature must be between 1°C and 35°C; the
polynomial in step 11 (P58) corrects for temperature errors within this range.
-1
The solution constant of 1.408 mS cm
(for prepared solution mentioned above),
entered in step 13 (P37), is valid only for a 0.01 molal KCl solution. Location 8
[Kc (cm-1)], generated by step 14, will contain the resultant cell constant.
01: AC Half Bridge (P5)
01:1Rep
02:152500 mV fast Range (5000 mV fast for 21X)
03:2IN Chan
04:1Excite all reps w/EXchan 1
05:2500mV Excitation (5000 mV for 21X)
06:1Loc [Rs ]
07:1Mult
08:0Offset
02: BR Transform Rf[X/(1-X)] (P59)
01:1Rep
02:1Loc [Rs ]
03:1Multiplier (Rf)
03: Z=F (P30)
01:nnnF Enter Cable Length in Feet
02:00Exponent of 10
03:5Loc [Rp ]
CS547 Conductivity and Temperature Probe and A547 Interface
09: Z=X+F (P34)
01:2X Loc t
02:-25F
03:3Z Loc [(t-25).01]
10: Z=X*F (P37)
01:3X Loc (t-25).01
02:.01F
03:3Z Loc [(t-25).01]
11: Polynomial (P55)
01:1Rep
02:3X Loc (t-25).01
03:4F(X) Loc [f(t) ]
04:.99124 C0
05:-1.8817C1
06:3.4789C2
07:-3.51C3
08:-1.2C4
09:-43C5
12: Z=1/X (P42)
01:4X Loc f(t)
02:6Z Loc [1/f(t) ]
13: Z=X*F (P37)
01:6X Loc 1/f(t)
02:1.408F EC of calibration solution
03:7Z Loc [Act'l Con]
14: Z=X*Y (P36)
01:7X Loc Act'l Con
02:1Y Loc Rs
03:8Z Loc [Kc (cm-1)]
7. Maintenance
Routine maintenance inc ludes thoroughly clea ning the orifice of the CS547
probe with the black nylon brush provided and a little soapy water. Rinse
thoroughly.
3.Ionization Error of KCl and Na+ Solutions After Correction:
< 2.0%, 0.45 to 7.0 mS cm
< 8.0%, 0.005 to 0.45 mS cm
-1
-1
CS547 Conductivity and Temperature Probe and A547 Interface
Correction of Ionization Errors: Figures 8.1-1 and 8.1-2 show the amount of
correction applied by the example program to compensate for ionization effects on
the measurements. Also shown is an ideal correction. Factors were derived by
measuring the standard solutions described in Section 2.2 with values of 0.0234,
-1
0.07, 0.4471, 07, 1.413, 2.070, 3.920, and 7.0 mS cm
.
FIGURE 8.1-1. Plot of Ideal and Actual Correction between
0 and 0.44 mS cm
-1
FIGURE 8.1-2. Plot of Ideal and Actual Correction between
0.44 and 7.0 mS cm
-1
13
CS547 Conductivity and Temperature Probe and A547 Interface
8.2 Temperature Measurement Error
The overall probe accuracy is a combination of the thermistor's interchangeability
specification, the precision of the bridge resistors, and the polynomial error. In a
"worst case" all errors add to an accuracy of ±0.4°C over the range of -24° to 48°C
and ±0.9°C over the range of -38°C to 53°C. The major error component is the
interchangeability specification of the thermistor, tabulated in Table 8.2-1. For the
range of 0° to 50°C the interchangeability error is predominantly offset and can be
determined with a single point calibration. Compensation can then be done with an
offset entered in the measurement instruction. The bridge resistors are 0.1%
tolerance with a 10 ppm temperature coefficient. Polynomial errors are tabulated in
Table 8.2-2 and plotted in Figure 8.2-1.
TABLE 8.2-1. Ther mistor
Interchangeability Specification
Temperature
Temperature (°C)Tolerance (±°C)
−40
−30
−20
−10
0 to +500 .20
0.40
0.40
0.32
0.25
TABLE 8.2-2. Polynomial Error
-40 to +56
-38 to +53
-24 to +48
<±1.0°C
<±0.5°C
<±0.1°C
14
FIGURE 8.2-1. Error Produced by Polynomial Fit to Published Values
CS547 Conductivity and Temperature Probe and A547 Interface
9. Deriving a Temperature Compensation Coefficient
1.Place the CS547 in a sample of the solution to be measured. Bring the
sample and the probe to 25°C.
2.Enter the example program from Section 5.2 in the datalogger and record
at 25°C from Location 3. This number will be C25 in the formula in
C
t
Step 4.
3.Bring the solution and the probe to a temperature (t) near the temperature
at which field measurements will be made. This temperature will be t (in
°C) in the formula. Record C
This number will be C in the formula in Step 4.
4.Calculate the temperature coefficient (TC) using the following formula.
()
CC
−
TC
Enter TC in the appropr iate location (nnn) as shown in the program segment in
Section 5.4.
()
25
tC
−∗
25
25
at the new temperature from Location 3.
t
%/=
C=∗
°100
10. Instruction 11 Details
Understanding the details in this section are not necessary for general operation
of the CS547 probe with CSI's dataloggers.
Instruction 11 outputs a precise 2 VAC excitation (4 V with the 21X) and
measures the voltage drop due to the sensor resistance. The thermistor
resistance changes with temperature. Instruction 11 calculates the ratio of
voltage measured to excitation voltage (Vs/Vx) which is related to resistance,
as shown below:
Vs/Vx = 1000/(Rs+249000+1000)
where Rs is the resistance of the thermistor.
See the measurement section of the datalogger manual for more information on
bridge measurements.
Instruction 11 then calculates temperature using a fifth order polynomial equation
correlating Vs/Vx with temperature. The polynomial coefficients are given in
Table 10-2. The polynomial input is (Vs/Vx)*800. Resistance and datalogger
output at several temperatures are shown in Table 10-1.
15
CS547 Conductivity and Temperature Probe and A547 Interface
TABLE 10-1. Temperature , Resistance, and
Datalogger Output
0.00351017-0.06
2.003152881.96
4.002835583.99
6.002553376.02
8.002302108.04
10.0020780710.06
12.0018780312.07
14.0016992414.06
16.0015392316.05
18.0013958818.02
20.0012672919.99
22.0011517921.97
24.0010479623.95
26.009544925.94
28.008702627.93
30.007942829.95
32.007256731.97
34.006636533.99
36.006075236.02
38.005566838.05
40.005105840.07
42.004687342.07
44.004307144.05
46.003961346.00
48.003646547.91
50.003359849.77
52.003098351.59
54.002859553.35
56.002641355.05
58.002441956.70
60.002259358.28
TABLE 10-2. Polynomial
Coefficients
COEFFICIENTVALUE
C0-53.4601
C19.08067
C2-8.32569 x 10
C35.22829 x 10
C4-1.67234 x 10
C52.21098 x 10
-01
-02
-03
-05
11. Electrically Noisy Environments
AC power lines can be the source of electrical noise. If the datalogger is in an
electronically noisy environment, the 107/107B temperature measurement
should be measured with the AC half bridge (Instruction 5) with the 60 Hz
rejection integration option on the CR10(X) and slow integration on the 21X
and CR7 (see Section 13 of the datalogger manual for more information on
noise). Instruction 11's fast integration will not reject 60 Hz noise.
16
CS547 Conductivity and Temperature Probe and A547 Interface
Example 2. Sample CR10(X) Instructions Using AC Half Bridge
01:1Rep
02:11*X Loc Air_Temp
03:11*F(X) Loc [:Air_Temp ]
04:-53.46C0
05:90.807C1
06:-83.257C2
07:52.283C3
08:-16.723C4
09:2.211C5
* Proper entries will vary with program and datalogger channel and input location
assignments.
**On the 21X and CR7 use the 15 mV input range and 4000 mV excitation.
12. Long Lead Lengths Temperature
If the CS547 has lead lengths of more than 300 feet, use the DC Half Bridge
instruction (Instruction 4) with a 2 millisecond delay to measure temperature.
The delay provides a longer settling time before the measurement is made. Do
not use the CS547 with long lead lengths in an electrically noisy environment.
Example 3. Sample Program CR10 Using DC Half Bridge with Delay