Die HAMEG Instruments GmbH bescheinigt die Konformität für das Produkt
The HAMEG Instruments GmbH herewith declares conformity of the product
HAMEG Instruments GmbH déclare la conformite du produit
Bezeichnung / Product name / Designation:
Oszilloskop/Oscilloscope/Oscilloscope
Typ / Type / Type: HM507
mit / with / avec: -
Optionen / Options / Options: -
mit den folgenden Bestimmungen / with applicable regulations / avec les directives
suivantes
EMV Richtlinie 89/336/EWG ergänzt durch 91/263/EWG, 92/31/EWG
EMC Directive 89/336/EEC amended by 91/263/EWG, 92/31/EEC
Directive EMC 89/336/CEE amendée par 91/263/EWG, 92/31/CEE
Niederspannungsrichtlinie 73/23/EWG ergänzt durch 93/68/EWG
Low-Voltage Equipment Directive 73/23/EEC amended by 93/68/EEC
Directive des equipements basse tension 73/23/CEE amendée par 93/68/CEE
EN 61326-1/A1
Störaussendung / Radiation / Emission: Tabelle / table / tableau 4; Klasse / Class / Classe B.
Störfestigkeit / Immunity / Imunitee: Tabelle / table / tableau A1.
EN 61000-3-2/A14
Oberschwingungsströme / Harmonic current emissions / Émissions de courant harmonique: Klasse / Class / Classe D.
EN 61000-3-3
Spannungsschwankungen u. Flicker / Voltage fl uctuations and fl icker /
Fluctuations de tension et du fl icker.
Datum /Date /Date Unterschrift / Signature /Signatur
15.01.2001
E. Baumgartner
Technical Manager /Directeur Technique
General information regarding the CE marking
HAMEG instruments fulfi ll the regulations of the EMC directive. The conformity test made by HAMEG is based on the actual
generic- and product standards. In cases where different limit values are applicable, HAMEG applies the severer standard.
For emission the limits for residential, commercial and light industry are applied. Regarding the immunity (susceptibility)
the limits for industrial environment have been used. The measuring- and data lines of the instrument have much infl uence
on emmission and immunity and therefore on meeting the acceptance limits. For different applications the lines and/or
cables used may be different. For measurement operation the following hints and conditions regarding emission and immunity should be observed:
1. Data cables
For the connection between instruments resp. their interfaces and external devices, (computer, printer etc.) suffi ciently
screened cables must be used. Without a special instruction in the manual for a reduced cable length, the maximum cable
length of a dataline must be less than 3 meters and not be used outside buildings. If an interface has several connectors
only one connector must have a connection to a cable. Basically interconnections must have a double screening. For IEEEbus purposes the double screened cables HZ72S and HZ72L from HAMEG are suitable.
2. Signal cables
Basically test leads for signal interconnection between test point and instrument should be as short as possible. Without
instruction in the manual for a shorter length, signal lines must be less than 3 meters and not be used outside buildings.
Signal lines must screened (coaxial cable - RG58/U). A proper ground connection is required. In combination with signal
generators double screened cables (RG223/U, RG214/U) must be used.
3. Infl uence on measuring instruments
Under the presence of strong high frequency electric or magnetic fi elds, even with careful setup of the measuring equipment an infl uence of such signals is unavoidable. This will not cause damage or put the instrument out of operation. Small
deviations of the measuring value (reading) exceeding the instruments specifi cations may result from such conditions in
individual cases.
4. RF immunity of oscilloscopes
4.1 Electromagnetic RF fi eld
The infl uence of electric and magnetic RF fi elds may become visible (e.g. RF superimposed), if the fi eld intensity is high. In
most cases the coupling into the oscilloscope takes place via the device under test, mains/line supply, test leads, control
cables and/or radiation. The device under test as well as the oscilloscope may be effected by such fi elds. Although the interior of the oscilloscope is screened by the cabinet, direct radiation can occur via the CRT gap. As the bandwidth of each
amplifi er stage is higher than the total –3dB bandwidth of the oscilloscope, the infl uence RF fi elds of even higher frequencies may be noticeable.
cable HZ72 from HAMEG is suitable.
4.2 Electrical fast transients / electrostatic discharge
Electrical fast transient signals (burst) may be coupled into the oscilloscope directly via the mains/line supply, or indirectly
via test leads and/or control cables. Due to the high trigger and input sensitivity of the oscilloscopes, such normally high
signals may effect the trigger unit and /or may become visible on the CRT, which is unavoidable. These effects can also be
caused by direct or indirect electrostatic discharge.
HAMEG Instruments GmbH
Subject to change without notice
3
Subject to change without notice
4
HM507
� 100MSa /s Real Time Sampling, 2GSa /s Random Sampling
� 2kPts Memory per Channel
� 2 Channels
� Deflection coefficients 1mV/div.…20V/div.,
Time Base 20ns/div.…100 s /div.
� 8-Bit Low Noise Flash A/D Converters
� Programmable Mathematical Signal Processing
� Acquisition modes: Single, Refresh, Envelope, Average, Roll
� RS-232 interface for control and signal data transfer,
incl. Windows
®
software
optional: Multifunction Interface HO79-6
� See HM504-2 for analog mode
5 0 M H z C o m b i S c ope
®
H M 5 0 7
HM507
Signal processing with
userdefined formulas
Cursor measurement
Automatic measurements
50MHz CombiScope®HM507
All data valid at 23 °C after 30 minute warm-up
Vertical Deflection
Operating Modes:Channel 1 or 2 only
Channels 1 and 2 (alternate or chopped)
Sum or Difference of CH 1 and CH 2
Operating Modes:Refresh, Roll, Single, XY, Envelope,
Average, Random Sampling
Interpolation:Linear Dot Join Function
Sampling Rate (Real Time): max 100MSa/s, 8 bit Flash A/D Converter
Sampling Rate (Random):2 GSa/s relative
Post/Pre-Trigger:-10.…+10 div. (continuous)
Display Refresh Rate:max. 180/s
Bandwidth:2 x 0…50 MHz (-3dB)
Signal Memory:3x 2 k x 8 bit
Reference Signal Memory:3x 2 k x 8 bit
Mathematical Signal Memory:3 x 2 k x 8 bit
Resolution (dots/div.) Yt Mode: X: 200/div., Y: 25/ div.
Resolution (dots/div.) XY Mode: X: 25/div., Y: 25/div.
Operation/Readout /Control
Manual:via controls
Autoset:automatic signal related parameter settings
Save and Recall:9 user defined parameter settings
Readout:display of menu, parameters, cursors
and results
Auto Measurements:
Analog mode:Frequency, Period, V
DC
, Vpp, Vp+, Vp-,
also in digital mode:V
rms
, V
average
Cursor Measurements:
Analog mode:ΔV, Δt, 1/Δt (f), tr, V to GND, ratio X and Y
also in digital mode:Pulse count, Vt related to Trigger Point,
Peak to Peak, Peak+, Peak-
Frequency counter:4 digit (0.01 % ±1 digit) 0.5 Hz…100MHz
Interface (standard fitting):RS-232 (Control, Signal Data)
Interface Option:HO79-6 (IEEE-488, RS-232, Centronics)
Component Tester
Test Voltage:approx. 7V
rms
(open circuit)
Test Current:max. 7 mA
rms
(short-circuit)
Test Frequency:approx. 50Hz
Test Connection:2 banana jacks 4 mm Ø
One test circuit lead is grounded via protective earth (PE)
Miscellaneous
CRT:D14-363GY, 8 x 10 div. with internal graticule
Acceleration Voltage:approx. 2 kV
Trace Rotation:adjustable on front panel
Z-Input (Intens. modulation, analog): max. + 5V (TTL)
Calibrator Signal (Square Wave): 0.2 V, 1 Hz…1MHz (tr ‹ 4 ns), DC
Power Supply (Mains):105…253V, 50/60 Hz ±10%, CAT II
Power Consumption:approx. 42 Watt at 230 V/50 Hz
Safety class:Safety class I (EN61010-1)
Operating temperature:+5…+40°C
Storage temperature:-20…+70°C
Rel. humidity:5…80% (non condensing)
Dimensions (W x H x D):285 x 125 x 380 mm
Weight:approx. 6.0kg
Accessories supplied: Line Cord, Operators Manual and Software for Windows
on CD-ROM, 2 Probes 1:1 / 10:1 (HZ154), RS-232 Interface
Optional accessories:
HO79-6 Multifunction Interface
HZ14Interface cable (serial) 1:1
HZ20Adapter, BNC to 4mm banana
HZ33Test cable 50Ω, BNC/BNC, 0,5m
HZ34Test cable 50Ω, BNC/BNC, 1m
HZ4319''-Rackmount Kit 3RU
HZ51Probe 10:1 (150MHz)
HZ52Probe 10:1 RF (250MHz)
HZ53Probe 100:1 (100MHz)
HZ56-2 AC/DC Current probe
HZ70Opto Interface (with optical fiber cable)
HZ72GPIB-Cable 2m
HZ100 Differential probe 20:1 / 200:1
HZ109 Differential probe 1:1 / 10:1
HZ115 Differential probe 100:1 / 1000:1
HZ200 Probe 10:1 with auto attenuation ID (250MHz)
HZ350 Probe 10:1 with automatically identification (350MHz)
HZ355 Slimline probe 10:1 with automatically identification (500MHz)
HZO20 High voltage probe 1000:1 (400MHz,1000Vrms)
HZO30 Active probe 1GHz (0,9pF, 1MΩ, including many accessories)
HZO50 AC/DC Current probe 20A, DC...100kHz
HZO51 AC/DC Current probe 1000A, DC...20kHz
®
· DQS-certified in accordance with DIN EN ISO 9001:2000, Reg.-No.: DE-071040 QM
w w w . h a m e g . c o m
50MHz CombiScope®HM507
All data valid at 23 °C after 30 minute warm-up
Vertical Deflection
Channels 1 and 2 (alternate or chopped)Sum or Difference of CH 1 and CH 2
Accuracy:± 3%Variable (uncalibrated):› 2.5:1 to › 1.25s/div.
Accuracy:± 5%
ns…140ms (variable)
al
Accuracy:± 2%
Accuracy:± 2%
DigitalStorage
Average, Random Sampling
Operation/Readout/Control
Manual:via controlsAutoset:automatic signal related parameter settingsSave and Recall:9 user defined parameter settingsReadout:display of menu, parameters, cursors
and results
AutoMeasurements:
Analog mode:Frequency, Period, V
DC
, Vpp, Vp+, Vp-,
also in digital mode:V
rms
, V
average
Cursor Measurements:
Analog mode:ΔV,Δt,1/Δt(f),tr,VtoGND,ratioXandYalso in digital mode:Pulse count, Vt related to Trigger Point,
Test Frequency:approx. 50HzTest Connection:2 banana jacks 4mm Ø
One test circuit lead is grounded via protective earth (PE)
Miscellaneous
CRT:D14-363GY, 8 x 10div. with internal graticuleAccelerationVoltage:approx. 2kVTraceRotation:adjustable on front panelZ-Input (Intens.modulation,analog):max.+5V(TTL)Calibrator Signal (Square Wave):0.2V, 1Hz…1MHz (tr ‹ 4ns), DCPower Supply (Mains):105…253V, 50/60Hz ±10%, CAT IIPower Consumption:approx. 42 Watt at 230V/50HzSafety class:Safety class I (EN61010-1)Operating temperature:+5…+40°CStoragetemperature:-20…+70°CRel. humidity:5…80% (non condensing)Dimensions (W x H x D):285 x 125 x 380mmWeight:approx. 6.0kg
Accessories supplied: Line Cord, Operators Manual and Software for Windowson CD-ROM, 2 Probes 1:1 / 10:1 (HZ154), RS-232 Interface
Optional accessories:
HO79-6Multifunction InterfaceHZ14Interface cable (serial) 1:1HZ20Adapter, BNC to 4mm bananaHZ33Test cable 50Ω, BNC/BNC, 0,5m HZ34Test cable 50Ω, BNC/BNC, 1m HZ4319''-Rackmount Kit 3RUHZ51Probe 10:1 (150MHz)HZ52Probe 10:1 RF (250MHz)HZ53Probe 100:1 (100MHz)HZ56-2AC/DC Current probeHZ70Opto Interface (with optical fiber cable)HZ72GPIB-Cable 2mHZ100Differential probe 20:1 / 200:1HZ109Differential probe 1:1 / 10:1HZ115Differential probe 100:1 / 1000:1HZ200Probe 10:1 with auto attenuation ID (250MHz)HZ350Probe 10:1 with automatically identification (350MHz)HZ355Slimline probe 10:1 with automatically identification (500MHz)HZO20High voltage probe 1000:1 (400MHz,1000Vrms)HZO30Active probe 1GHz (0,9pF, 1MΩ, including many accessories)HZO50AC/DC Current probe 20A, DC...100kHzHZO51AC/DC Current probe 1000A, DC...20kHz
Subject to change without notice
Specifications
5
General information
General information
Please check the instrument for mechanical damage or loose
parts immediately after unpacking. In case of damage we advise
to contact the sender. Do not operate.
B
C
B
T
A
List of symbols used
Consult the manual High voltage
Important note Ground
Positioning the instrument
As can be seen from the fi gures, the handle can be set into different positions:
A and B = carrying
C = horizontal operating
D and E = operating at different angles
F = handle removal
T = shipping (handle unlocked)
Attention!
When changing the handle position, the instru-
ment must be placed so that it can not fall (e.g.
placed on a table). Then the handle locking knobs
must be simultaneously pulled outwards and
rotated to the required position. Without pulling
the locking knobs they will latch in into the next
locking position.
C
D
F
E
D
E
A
PUOPFGkT
PUOPFGkT PUOPFGkT
PUOPFGkT
PUOGkT
PUOPFGkT
PUOPFGkT
HM507
PUOPFGkT
PUOPFGkT
PUOPFGkT PUOPFGkT PUOPFGkT PUOPFGkT
PUOPFGkT
PUOPFGkT PUOPFGkT
PUk PUk PUk PUkPUk PUk
PUkT
HGOPFFD
B
PUOPFGkT
PUOPFGkT
PUkT
PUkT
PUkT
INPUT CHI
OPK
HJ
PUkT
VBN
PUOPFGkT
HJKL
PUOPFGkT
PUkT
PUOPFGkT
HGOFFD
PUkT
PUkT
PUkT
INPUT CHI
INPUT CHI
HAMEG
OPK
OPK
HJ
HJ
VBN
VBN
PUOPFGkT
HJKL
HJKL
T
Handle mounting/dismounting
The handle can be removed by pulling it out further, depending on
the instrument model in position B or F.
Safety
The instrument fulfi ls the VDE 0411 part 1 regulations for
electrical measuring, control and laboratory instruments and
was manufactured and tested accordingly. It left the factory in
perfect safe condition. Hence it also corresponds to European
Standard EN 61010-1 resp. International Standard IEC 1010-1.
In order to maintain this condition and to ensure safe operation
the user is required to observe the warnings and other directions
for use in this manual. Housing, chassis as well as all measuring terminals are connected to safety ground of the mains.
All accessible metal parts were tested against the mains with
200 V
The oscilloscope may only be operated from mains outlets with a
safety ground connector. The plug has to be installed prior to connecting any signals. It is prohibited to separate the safety ground
connection.
Most electron tubes generate X-rays; the ion dose rate of this
instrument remains well below the 36 pA/kg permitted by law.
In case safe operation may not be guaranteed do not use the instrument any more and lock it away in a secure place.
. The instrument conforms to safety class I.
DC
T
Safe operation may be endangered if any of the following
was noticed:
– in case of visible damage.
– in case loose parts were noticed
– if it does not function any more.
– after prolonged storage under unfavourable conditions (e.g.
like in the open or in moist atmosphere).
– after any improper transport (e.g. insuffi cient packing not
conforming to the minimum standards of post, rail or transport
company)
Proper operation
Please note: This instrument is only destined for use by personnel
well instructed and familiar with the dangers of electrical measurements.
For safety reasons the oscilloscope may only be operated from
mains outlets with safety ground connector. It is prohibited to
separate the safety ground connection. The plug must be inserted
prior to connecting any signals.
6
Subject to change without notice
General information
CAT I
This oscilloscope is destined for measurements in circuits not
connected to the mains or only indirectly. Direct measurements,
i.e. with a galvanic connection to circuits corresponding to the
categories II, III, or IV are prohibited!
The measuring circuits are considered not connected to the mains
if a suitable isolation transformer fulfi lling safety class II is used.
Measurements on the mains are also possible if suitable probes
like current probes are used which fulfi l the safety class II. The
measurement category of such probes must be checked and
observed.
Measurement categories
The measurement categories were derived corresponding to the
distance from the power station and the transients to be expected
hence. Transients are short, very fast voltage or current excursions
which may be periodic or not.
Measurement CAT IV:
Measurements close to the power station, e.g. on electricity
meters
Measurement CAT III:
M e a su r e me n t s in t h e in t e r io r o f b ui l d i ng s ( p o w er d i s tr i b u tio n i n s t al lations, mains outlets, motors which are permanently installed).
Measurement CAT II:
Measurements in circuits directly connected to the mains (household appliances, power tools etc).
Measurement CAT I:
Electronic instruments and circuits which contain circuit breakers
resp. fuses.
Warranty and repair
HAMEG instruments are subjected to a strict quality control. Prior
to leaving the factory, each instrument is burnt-in for 10 hours.
By intermittent operation during this period almost all defects
are detected. Following the burn-in, each instrument is tested for
function and quality, the specifi cations are checked in all operating
modes; the test gear is calibrated to national standards.
The warranty standards applicable are those of the country in
which the instrument was sold. Reclamations should be directed
to the dealer.
Only valid in EU countries
In order to speed reclamations customers in EU countries may
also contact HAMEG directly. Also, after the warranty expired, the
HAMEG service will be at your disposal for any repairs.
Return material authorization (RMA):
Prior to returning an instrument to HAMEG ask for a RMA number
either by internet (http://www.hameg.com) or fax. If you do not
have an original shipping carton, you may obtain one by calling the
HAMEG service dept (++49 (0) 6182 800 500 ) or by sending an
email to service@hameg.com.
Maintenance
Clean the outer shell using a dust brush in regular intervals. Dirt can
be removed from housing, handle, all metal and plastic parts using
a cloth moistened with water and 1 % detergent. Greasy dirt may
be removed with benzene (petroleum ether) or alcohol, there after
wipe the surfaces with a dry cloth. Plastic parts should be treated
with an antistatic solution destined for such parts. No fl uid may
enter the instrument. Do not use other cleansing agents as they
may adversely affect the plastic or lacquered surfaces.
Environment of use.
The oscilloscope is destined for operation in industrial, business,
manufacturing, and living sites.
Environmental conditions
Operating ambient temperature: +5 °C to +40 °C. During transport
or storage the temperature may be –20 °C to +70°C.
Please note that after exposure to such temperature s or in case of
condensation proper time must be allowed until the instrument has
reached the permissible temperature, resp. until the condensation
has evaporated before it may be turned on! Ordinarily this will be
the case after 2 hours.
The oscilloscope is destined for use in clean and dry environments.
Do not operate in dusty or chemically aggressive atmosphere or if
there is danger of explosion.
The operating position may be any, however, suffi cient ventilation
must be ensured (convecti on cooling). P rolonged operation requires
the horizontal or inclined position.
Do not obstruct the ventilation holes!
Specifi cations are valid after a 30 minute warm-up period between
15 and 30 degr. C. Specifi cations without tolerances are average
values.
Line voltage
The instrument has a wide range power supply from 105 to 253 V,
50 or 60 Hz ±10%. There is hence no line voltage selector.
The line fuse is accessible on the rear panel and part of the line input
connector. Prior to exchanging a fuse the line cord must be pulled
out. Exchange is only allowed if the fuse holder is undamaged, it
can be taken out using a screwdriver put into the slot. The fuse
can be pushed out of its holder and exchanged.
The holder with the new fuse can then be pushed back in place
against the spring. It is prohibited to ”repair“ blown fuses or to
bridge the fuse. Any damages incurred by such measures will
void the warranty.
Type of fuse:
Size 5 x 20 mm; 250V~, C;
IEC 127, Bl. III; DIN 41 662
(or DIN 41 571, Bl. 3).
Cut off: slow blow (T) 0,8A.
Subject to change without notice
7
Type of signal voltage
Type of signal voltage
The oscilloscope HM507 allows examination of DC voltages
and most repetitive signals in the frequency range up to at least
40MHz (-3dB).
The vertical amplifiers have been designed for minimum
overshoot and therefore permit a true signal display.
The display of sinusoidal signals within the bandwidth limits
causes no problems, but an increasing error in measurement
due to gain reduction must be taken into account when
measuring high frequency signals. This error becomes
noticeable at approx. 14MHz. At approx. 18MHz the reduction
is approx. 10% and the real voltage value is 11% higher. The
gain reduction error can not be defined exactly as the -3dB
bandwidth of the amplifiers differ between 40MHz and 42MHz.
For sinewave signals the -6dB limit is approx. 50MHz.
When examining square or pulse type waveforms, attention
must be paid to the harmonic content of such signals. The
repetition frequency (fundamental frequency) of the signal
must therefore be significantly smaller than the upper limit
frequency of the vertical amplifier.
Displaying composite signals can be difficult, especially if they
contain no repetitive higher amplitude content which can be
used for triggering. This is the case with bursts, for instance.
To obtain a well-triggered display in this case, the assistance
of the variable holdoff function or the delayed time base may
be required. Television video signals are relatively easy to
trigger using the built-in TV-Sync-Separator (TV).
For optional operation as a DC or AC voltage amplifier, each
vertical amplifier input is provided with a DC/AC switch. DC
coupling should only be used with a series-connected attenuator
probe or at very low frequencies or if the measurement of the
DC voltage content of the signal is absolutely necessary.
When displaying very low frequency pulses, the flat tops may be
sloping with AC coupling of the vertical amplifier (AC limit frequency
approx. 1.6 Hz for 3dB). In this case, DC operation is preferred, provided
the signal voltage is not superimposed on a too high DC level.
Otherwise a capacitor of adequate capacitance must be connected
to the input of the vertical amplifier with DC coupling. This capacitor
must have a sufficiently high breakdown voltage rating. DC coupling
is also recommended for the display of logic and pulse signals,
especially if the pulse duty factor changes constantly. Otherwise the
display will move upwards or downwards at each change. Pure direct
voltages can only be measured with DC-coupling.
The minimum signal voltage which must be applied to the Y input
for a trace of 1div height is 1mVpp (± 5%) when this deflection
coefficient is displayed on the screen (readout) and the vernier is
switched off (VAR-LED dark). However, smaller signals than this
may also be displayed. The deflection coefficients are indicated
in mV/div or V/div (peak-to-peak value).
The magnitude of the applied voltage is ascertained by multiplying
the selected deflection coefficient by the vertical display height in
div. If an attenuator probe x10 is used, a further multiplication by
a factor of 10 is required to ascertain the correct voltage value.
For exact amplitude measurements, the variable control (VAR)
must be set to its calibrated detent CAL position.
With the variable control activated the deflection sensitivity
can be reduced up to a ratio of 2.5 to 1 (please note “controls
and readout”). Therefore any intermediate value is possible
within the 1-2-5 sequence of the attenuator(s).
With direct connection to the vertical input, signals up to 400Vpp may be displayed (attenuator
set to 20V/div, variable control to 2.5:1).
With the designations
H = display height in div,
U = signal voltage in Vpp at the vertical input,
D = deflection coefficient in V/div at attenuator switch,
the required value can be calculated from the two given
quantities:
The input coupling is selectable by the AC/DC pushbutton. The
actual setting is displayed in the readout with the ” = ” symbol
for DC- and the ”
~”symbol for AC coupling.
Amplitude Measurements
In general electrical engineering, alternating voltage data normally
refers to effective values (rms = root-mean-square value). However,
for signal magnitudes and voltage designations in oscilloscope
measurements, the peak-to-peak voltage (Vpp) value is applied.
The latter corresponds to the real potential difference between the
most positive and most negative points of a signal waveform.
If a sinusoidal waveform, displayed on the oscilloscope screen,
is to be converted into an effective (rms) value, the resulting peakto-peak value must be divided by 2x√2 = 2.83. Conversely, it
should be observed that sinusoidal voltages indicated in Vrms
(Veff) have 2.83 times the potential difference in Vpp. The
relationship between the different voltage magnitudes can be
seen from the following figure.
8
However, these three values are not freely selectable. They
have to be within the following limits (trigger threshold,
accuracy of reading):
H between 0.5 and 8div, if possible 3.2 to 8div,
U between 0.5mVpp and 160Vpp,
D between 1mV/div and 20V/div in 1-2-5 sequence.
Examples:
Set deflection coefficient D = 50mV/div 0.05V/div,
observed display height H = 4.6div,
required voltage U = 0.05x4.6 = 0.23Vpp.
Input voltage U = 5Vpp,
set deflection coefficient D = 1V/div,
required display height H = 5:1 = 5div.
Signal voltage U = 230Vrmsx2
(voltage
> >
> 160Vpp, with probe 10:1: U = 65.1Vpp),
> >
√√
√
2 = 651Vpp
√√
desired display height H = min. 3.2div, max. 8div,
Subject to change without notice
Type of signal voltage
max. deflection coefficient D = 65.1:3.2 = 20.3V/div,
min. deflection coefficient D = 65.1:8 = 8.1V/div,
adjusted deflection coefficient D = 10V/div.
The previous examples are related to the CRT graticule reading.
The results can also be determined with the aid of the DV
cursor measurement (please note “controls and readout”).
The input voltage must not exceed 400V, independent from
the polarity.
If an AC voltage which is superimposed on a DC voltage is
applied, the maximum peak value of both voltages must not
exceed + or - 400V. So for AC voltages with a mean value of zero
volt the maximum peak to peak value is 800Vpp.
If attenuator probes with higher limits are used, the probes limits
are valid only if the oscilloscope is set to DC input coupling.
If DC voltages are applied under AC input coupling conditions
the oscilloscope maximum input voltage value remains 400V.
The attenuator consists of a resistor in the probe and the 1MΩ
input resistor of the oscilloscope, which are disabled by the AC
input coupling capacity when AC coupling is selected. This
also applies to DC voltages with superimposed AC voltages.
It also must be noted that due to the capacitive resistance of
the AC input coupling capacitor, the attenuation ratio depends
on the signal frequency. For sinewave signals with frequencies
higher than 40Hz this influence is negligible.
Time Measurements
As a rule, most signals to be displayed are periodically
repeating processes, also called periods. The number of
periods per second is the repetition frequency. Depending
on the time base setting (TIME/DIV.-knob) indicated by the
readout, one or several signal periods or only a part of a period
can be displayed. The time coefficients are stated in ms/div,
µs/div or ns/div. The following examples are related to the
CRT graticule reading. The results can also be determined
with the aid of the ∆T and 1/
note “ controls and readout”).
The duration of a signal period or a part of it is determined by
multiplying the relevant time (horizontal distance in div) by the
(calibrated) time coefficient displayed in the readout.
Uncalibrated, the time base speed can be reduced until a
maximum factor of 2.5 is reached. Therefore any intermediate
value is possible within the 1-2-5 sequence.
With the designations
L = displayed wave length in div of one period,
T = time in seconds for one period,
F = recurrence frequency in Hz of the signal,
Tc = time coefficient in ms, µs or ns/div and the relation
F = 1/T, the following equations can be stated:
∆∆
∆T cursor measurement (please
∆∆
With the above listed exceptions HAMEG 10:1 probes can be
used for DC measurements up to 600V or AC voltages (with a
mean value of zero volt) of 1200Vpp. The 100:1 probe HZ53
allows for 1200V DC or 2400Vpp for AC.
It should be noted that its AC peak value is derated at higher
frequencies. If a normal x10 probe is used to measure high
voltages there is the risk that the compensation trimmer
bridging the attenuator series resistor will break down causing
damage to the input of the oscilloscope. However, if for
example only the residual ripple of a high voltage is to be
displayed on the oscilloscope, a normal x10 probe is sufficient.
In this case, an appropriate high voltage capacitor (approx. 2268nF) must be connected in series with the input tip of the
probe.
With Y-POS. control (input coupling to GD) it is possible to use
a horizontal graticule line as reference line for ground potential
before the measurement. It can lie below or above the horizontal
central line according to whether positive and/or negative
deviations from the ground potential are to be measured.
Total value of input voltage
However, these four values are not freely selectable. They
have to be within the following limits:
Lbetween 0.2 and 10div, if possible 4 to 10div,
Tbetween 10ns and 5s,
Fbetween 0.5Hz and 100MHz,
Tcbetween 100ns/div and 500ms/div in 1-2-5 sequence
(with X-MAG. (x10) inactive), and
Tcbetween 10ns/div and 50ms/div in 1-2-5 sequence
(with X-MAG. (x10) active).
Examples:Examples:
Examples:
Examples:Examples:
Displayed wavelength L = 7div,Displayed wavelength L = 7div,
Displayed wavelength L = 7div,
Displayed wavelength L = 7div,Displayed wavelength L = 7div,
set time coefficient Tc = 100ns/div,set time coefficient Tc = 100ns/div,
set time coefficient Tc = 100ns/div,
set time coefficient Tc = 100ns/div,set time coefficient Tc = 100ns/div,
required period T = 7x100x10required period T = 7x100x10
required period T = 7x100x10
required period T = 7x100x10required period T = 7x100x10
required rec. freq. F = 1:(0.7x10required rec. freq. F = 1:(0.7x10
required rec. freq. F = 1:(0.7x10
required rec. freq. F = 1:(0.7x10required rec. freq. F = 1:(0.7x10
Signal period T = 1s,Signal period T = 1s,
Signal period T = 1s,
Signal period T = 1s,Signal period T = 1s,
set time coefficient Tc = 0.2s/div,set time coefficient Tc = 0.2s/div,
set time coefficient Tc = 0.2s/div,
set time coefficient Tc = 0.2s/div,set time coefficient Tc = 0.2s/div,
required wavelength L = 1:0.2 = 5div.required wavelength L = 1:0.2 = 5div.
required wavelength L = 1:0.2 = 5div.
required wavelength L = 1:0.2 = 5div.required wavelength L = 1:0.2 = 5div.
Displayed ripple wavelength L = 1div,Displayed ripple wavelength L = 1div,
Displayed ripple wavelength L = 1div,
Displayed ripple wavelength L = 1div,Displayed ripple wavelength L = 1div,
set time coefficient Tc = 10ms/div,set time coefficient Tc = 10ms/div,
set time coefficient Tc = 10ms/div,
set time coefficient Tc = 10ms/div,set time coefficient Tc = 10ms/div,
required ripple freq. F = 1:(1x10x10required ripple freq. F = 1:(1x10x10
required ripple freq. F = 1:(1x10x10
required ripple freq. F = 1:(1x10x10required ripple freq. F = 1:(1x10x10
-9-9
-9
-9-9
= 0.7µs = 0.7µs
= 0.7µs
= 0.7µs = 0.7µs
-6-6
-6
-6-6
) = 1.428MHz.) = 1.428MHz.
) = 1.428MHz.
) = 1.428MHz.) = 1.428MHz.
-3-3
-3
-3-3
) = 100Hz.) = 100Hz.
) = 100Hz.
) = 100Hz.) = 100Hz.
The dotted line shows a voltage alternating at zero volt level.
If superimposed on a DC voltage, the addition of the positive
peak and the DC voltage results in the max. voltage (DC +
ACpeak).
Subject to change without notice
TV-line frequency F = 15625Hz,TV-line frequency F = 15625Hz,
TV-line frequency F = 15625Hz,
TV-line frequency F = 15625Hz,TV-line frequency F = 15625Hz,
set time coefficient Tc = 10µs/div,set time coefficient Tc = 10µs/div,
set time coefficient Tc = 10µs/div,
set time coefficient Tc = 10µs/div,set time coefficient Tc = 10µs/div,
required wavelength L = 1:(15 625x10required wavelength L = 1:(15 625x10
required wavelength L = 1:(15 625x10
required wavelength L = 1:(15 625x10required wavelength L = 1:(15 625x10
Sine wavelength L = min. 4div, max. 10div,Sine wavelength L = min. 4div, max. 10div,
Sine wavelength L = min. 4div, max. 10div,
Sine wavelength L = min. 4div, max. 10div,Sine wavelength L = min. 4div, max. 10div,
Frequency F = 1kHz,Frequency F = 1kHz,
Frequency F = 1kHz,
Frequency F = 1kHz,Frequency F = 1kHz,
max. time coefficient Tc = 1:(4x10max. time coefficient Tc = 1:(4x10
max. time coefficient Tc = 1:(4x10
max. time coefficient Tc = 1:(4x10max. time coefficient Tc = 1:(4x10
min. time coefficient Tc = 1:(10x10min. time coefficient Tc = 1:(10x10
min. time coefficient Tc = 1:(10x10
min. time coefficient Tc = 1:(10x10min. time coefficient Tc = 1:(10x10
set time coefficient Tc = 0.2ms/div,set time coefficient Tc = 0.2ms/div,
set time coefficient Tc = 0.2ms/div,
set time coefficient Tc = 0.2ms/div,set time coefficient Tc = 0.2ms/div,
required wavelength L = 1:(10required wavelength L = 1:(10
required wavelength L = 1:(10
required wavelength L = 1:(10required wavelength L = 1:(10
Displayed wavelength L = 0.8div,Displayed wavelength L = 0.8div,
Displayed wavelength L = 0.8div,
Displayed wavelength L = 0.8div,Displayed wavelength L = 0.8div,
set time coefficient Tc = 0.5µs/div,set time coefficient Tc = 0.5µs/div,
set time coefficient Tc = 0.5µs/div,
set time coefficient Tc = 0.5µs/div,set time coefficient Tc = 0.5µs/div,
If the time is relatively short as compared with the complete
signal period, an expanded time scale should always be applied
(X-MAG. (x10) active). In this case, the time interval of interest can
be shifted to the screen center using the X-POS. control.
When investigating pulse or square waveforms, the critical
feature is the risetime of the voltage step. To ensure that
transients, ramp-offs, and bandwidth limits do not unduly influence
the measuring accuracy, the risetime is generally measured
between 10% and 90% of the vertical pulse height. For
measurement, adjust the Y deflection coefficient using its variable function (uncalibrated) together with the Y-POS. control so
that the pulse height is precisely aligned with the 0% and 100%
lines of the internal graticule. The 10% and 90% points of the
signal will now coincide with the 10% and 90% graticule lines.
The risetime is given by the product of the horizontal distance in
div between these two coincident points and the calibrated time
coefficient setting. The fall time of a pulse can also be measured
by using this method.
The following figure shows correct positioning of the oscilloscope
trace for accurate risetime measurement.
with approximately constant group delay (therefore good pulse
transmission performance) the following numerical relationship
between rise time tr (in ns) and bandwidth B (in MHz) applies:
Connection of Test Signal
In most cases briefly depressing the AUTO SET causes a useful
signal related instrument setting. The following explanations
refer to special applications and/or signals, demanding a manual
instrument setting. The description of the controls is explained
in the section “controls and readout”.
Caution:
When connecting unknown signals to the oscilloscope
input, always use a x10 probe, automatic triggering
and set the input coupling switch to DC (readout). The
attenuator should initially be set to 20V/div.
Sometimes the trace will disappear after an input signal has
been applied. Then a higher deflection coefficient (lower input
sensitivity) must be chosen until the vertical signal height is
only 3-8div. With a signal amplitude greater than 160Vpp and
the deflection coefficient (VOLTS/DIV.) in calibrated condition,
an attenuator probe must be inserted before the vertical input.
If, after applying the signal, the trace is nearly blanked, the
period of the signal is probably substantially longer than the set
time deflection coefficient (TIME/DIV.). It should be switched
to an adequately larger time coefficient.
With a time coefficient of 10ns/div (X x10 magnification active),
the example shown in the above figure results in a total measured
risetime of
= 1.6div x 10ns/div = 16ns
t
tot
When very fast risetimes are being measured, the risetimes of
the oscilloscope amplifier and of the attenuator probe has to be
deducted from the measured time value. The risetime of the
signal can be calculated using the following formula.
In this t
oscilloscope amplifier (approx. 8.75ns), and t
probe (e.g. = 2ns). If t
as the risetime of the pulse, and calculation is unnecessary.
is the total measured risetime, t
tot
is greater than 100ns, then t
tot
is the risetime of the
osc
the risetime of the
p
can be taken
tot
Calculation of the example in the figure above results in a
signal risetime
= √162 - 8.752 - 22 = 13.25ns
t
r
The measurement of the rise or fall time is not limited to the trace
dimensions shown in the above diagram. It is only particularly simple
in this way. In principle it is possible to measure in any display position
and at any signal amplitude. It is only important that the full height
of the signal edge of interest is visible in its full length at not too great
steepness and that the horizontal distance at 10% and 90% of the
amplitude is measured. If the edge shows rounding or overshooting,
the 100% should not be related to the peak values but to the mean
pulse heights. Breaks or peaks (glitches) next to the edge are also
not taken into account. With very severe transient distortions, the
rise and fall time measurement has little meaning. For amplifiers
The signal to be displayed can be connected directly to the Yinput of the oscilloscope with a shielded test cable such as HZ32
or HZ34, or reduced through a x10 or x100 attenuator probe. The
use of test cables with high impedance circuits is only
recommended for relatively low frequencies (up to approx.
50kHz). For higher frequencies, the signal source must be of low
impedance, i.e. matched to the characteristic resistance of the
cable (as a rule 50Ω). Especially when transmitting square and
pulse signals, a resistor equal to the characteristic impedance
of the cable must also be connected across the cable directly
at the Y-input of the oscilloscope. When using a 50Ω cable such
as the HZ34, a 50Ω through termination type HZ22 is available
from HAMEG. When transmitting square signals with short rise
times, transient phenomena on the edges and top of the signal
may become visible if the correct termination is not used. A
terminating resistance is sometimes recommended with sine
signals as well. Certain amplifiers, generators or their attenuators
maintain the nominal output voltage independent of frequency
only if their connection cable is terminated with the prescribed
resistance. Here it must be noted that the terminating resistor
HZ22 will only dissipate a maximum of 2Watts. This power is
reached with 10Vrms or at 28.3Vpp with sine signal. If a x10 or
x100 attenuator probe is used, no termination is necessary. In
this case, the connecting cable is matched directly to the high
impedance input of the oscilloscope. When using attenuators
probes, even high internal impedance sources are only slightly
loaded (approx. 10MΩ II 12pF or 100MΩ II 5pF with HZ53).
Therefore, if the voltage loss due to the attenuation of the probe
can be compensated by a higher amplitude setting, the probe
should always be used. The series impedance of the probe
provides a certain amount of protection for the input of the
vertical amplifier. Because of their separate manufacture, all
attenuator probes are only partially compensated, therefore
accurate compensation must be performed on the oscilloscope
(see Probe compensation ).
Standard attenuator probes on the oscilloscope normally reduce
its bandwidth and increase the rise time. In all cases where the
oscilloscope bandwidth must be fully utilized (e.g. for pulses
10
Subject to change without notice
Controls and readout
with steep edges) we strongly advise using the probes HZ51
(x10) HZ52 (x10 HF) and HZ54 (x1 and x10). This can save the
purchase of an oscilloscope with larger bandwidth.
The probes mentioned have a HF-calibration in addition to low
frequency calibration adjustment. Thus a group delay correction
to the upper limit frequency of the oscilloscope is possible
with the aid of an 1MHz calibrator, e.g. HZ60.
In fact the bandwidth and rise time of the oscilloscope are not
noticeably changed with these probe types and the waveform
reproduction fidelity can even be improved because the probe can
be matched to the oscilloscopes individual pulse response.
If a x10 or x100 attenuator probe is used, DC input
coupling must always be used at voltages above 400V.
With AC coupling of low frequency signals, the
attenuation is no longer independent of frequency,
pulses can show pulse tilts. Direct voltages are
suppressed but load the oscilloscope input coupling
capacitor concerned. Its voltage rating is max. 400 V
(DC + peak AC). DC input coupling is therefore of quite
special importance with a x100 attenuation probe
which usually has a voltage rating of max. 1200 V (DC
+ peak AC). A capacitor of corresponding capacitance
and voltage rating may be connected in series with the
attenuator probe input for blocking DC voltage (e.g. for
hum voltage measurement).
With all attenuator probes, the maximum AC input voltage
must be derated with frequency usually above 20kHz.
Therefore the derating curve of the attenuator probe type
concerned must be taken into account. The selection of
the ground point on the test object is important when
displaying small signal voltages. It should always be as
close as possible to the measuring point. If this is not done,
serious signal distortion may result from spurious currents
through the ground leads or chassis parts. The ground
leads on attenuator probes are also particularly critical.
They should be as short and thick as possible. When the
attenuator probe is connected to a BNC-socket, a BNCadapter, should be used. In this way ground and matching
problems are eliminated. Hum or interference appearing
in the measuring circuit (especially when a small deflection
coefficient is used) is possibly caused by multiple
grounding because equalizing currents can flow in the
shielding of the test cables (voltage drop between the
protective conductor connections, caused by external
equipment connected to the mains/line, e.g. signal
generators with interference protection capacitors).
B: Menu Display and Operation
Operation of some pushbuttons activates the display of menus.
There are Standard and Pulldown Menus.
Standard menus:
When a standard menu is displayed, all other readout
information (e.g. parameter settings) are switched off. The
readout then consists of the menu headline, and the respective
menu functions. At the bottom of the graticule are displayed
symbols and commands which can be operated by the
pushbuttons related to them below.
“Esc”switches one step back in the menu hierarchy.
“Exit” closes the menu and switches back to the operating
conditions present before calling the menu.
“Set”calls the selected menu item or starts a function.
“SAVE”results in storage.
“Edit” calls the edit menu.
The pushbuttons below the triangle and arrow symbols select
one item that is then highlighted. If in addition “Use INT./FOC.
knob to select” is displayed, the INT./FOC. knob can be used
to select within the item. Where a “[ ]” symbol appears in an
activated line, a “[x]/[ ]” symbol is displayed with the other
command symbols at the bottom of the screen. The
pushbutton below the symbol is used for switchover (toggle).
Pulldown menus:
After pressing a pushbutton which calls a pulldown menu, the
instrument parameter settings are still displayed. The readout
only changes in respect to the called parameter (e.g. input
coupling) and now shows all selectable parameter options (in
case of input coupling: AC, DC and GND). The previously
displayed parameter doesn‘t change but is displayed
highlighted. Each time the pushbutton is briefly pressed the
next parameter becomes active and highlighted, as long as
the pulldown menu is displayed. Without further pressing of
the pushbutton, the pulldown menu extinguishes after a few
seconds and the selected parameter, the CURSOR line(s) and
the measuring result are displayed in the normal way.
C: READOUT Information
Controls and Readout
A: Basic settings
The following description assumes that:
1. “Component Tester” is switched off.
2. The following settings are present under
MAIN MENU > SETUP & INFO > MISCELLANEOUS:
2.1 CONTROL BEEP and ERROR BEEP activated (x),
2.2 QUICK START not activated.
3. The screen Readout is visible.
The LED indicators on the large front panel facilitate operation
and provide additional information. Electrical end positions of
controls are indicated by acoustic signal (beep).
All controls, except the power switch (POWER), are
electronically set and interrogated. Thus, all electronically set
functions and their current settings can be stored and also
remotely controlled.
Subject to change without notice
The readout alphanumerically displays the scope parameter
settings, measurement results and CURSOR lines. Which
information is displayed depends on the actual instrument
settings. The following list contains the most important display
information.
Top of the graticule from left to right:
1. time deflection coefficient and additionally the sampling
rate in digital mode.
11
Controls and readout
2. trigger source, slope and coupling.
3. operating condition of delay time base in analog mode;
or in digital mode, pre or post trigger time.
4. measuring results.
Bottom of the graticule from left to right:
1. probe symbol (x10), Y deflection coefficient and input
coupling channel I.
2. “+” symbol (addition).
3. probe symbol (x10), Y deflection coefficient and input
coupling channel II.
4. channel mode (analog) or signal display mode (digital).
The trigger point symbol is displayed at the left graticule border
line (analog mode). The CURSOR lines can take any position
within the graticule.
D: Description of Controls
Preliminary note:
For better identification all controls are numbered consecutively.
A number within a square indicates a control which is for digital
mode. The latter will be described at the end of the listing.
The large front panel is, as usual with Hameg oscilloscopes,
marked with several fields.
The following controls and LED indicators are located
on the top, to the right of the screen, above the
horizontal line:
If the signal height is insufficient, the
not change. In
to the signal which is used for internal triggering.
Voltage CURSOR
If voltage measurement is present, the CURSOR lines are
automatically set to the positive and negative peak value
of the signal. The accuracy of this function decreases with
higher frequencies and is also influenced by the signal‘s
pulse duty factor.
Time/Frequency CURSOR
If complex waveforms such as video signals are applied,
the cursor lines may not align exactly with one period and
give a false reading.
DIGITAL MODE ONLY
If ROLL (“rol”) or SINGLE (“sgl”) is active, AUTOSET
switches to the last used REFRESH mode.
(3) INT./FOC. Knob for intensity and focus setting, with
associated LEDs and TRACE ROT. pushbutton.
3.1 Briefly pressing the TRACE ROT. pushbutton switches
over the INT./FOC. knob to another function, which is
indicated by an LED. If the readout
off, the sequence is A, FOC, RO, A. In condition READOUT
deactivated, the switching sequence is A, FOC, A.
3.1.1 “A”:
The INT./FOC. knob controls the signal(s) intensity. Turning
this knob clockwise increases the intensity. Only the
minimum required trace intensity should be used,
depending on signal parameters, oscilloscope settings and
light conditions.
DUAL
..
.
..
mode the
..
.
..
CURSOR
CURSOR
(RO)
lines do
lines are related
is not switched
(1) POWER
After the oscilloscope is switched on, all LEDs are lit and
an automated instrument test is performed. During this time
the HAMEG logo and the software version are displayed on
the screen. After the internal test is completed successfully,
the overlay is switched off and the normal operation mode is
present. The last used settings and the readout then become
activated. An LED (3) indicates the ON condition.
(2) AUTOSET
Briefly pressing this pushbutton results in an automatic
instrument setting selecting Yt mode as the default. The
instrument is set to the last used Yt mode setting (CH I,
CH II
intensity had been present before. The operation mode
(analog or digital) will not be changed.
The instrument is set automatically to normal (undelayed)
time base mode, even if the previous Yt mode included
search (“sea”), delay (“del”) or triggered delay (“dTr”) time
base mode.
Please also note ”AUTOSET” in section “First Time
Operation”.
Automatic
If CURSORCURSOR lines are set automatically under suitable conditions
and the readout briefly displays “SETTING CURSOR”.
Pushbutton and symbols for ON (I) and OFF (O).
or
DUAL)
and to a medium trace intensity, if less
CURSOR
lines are displayed and AUTOSET is chosen the
positioning:
3.1.2 “FOC“:
The INT./FOC. knob controls both the trace and the readout
sharpness. Note: The electron beam diameter gets larger
with a higher trace intensity and the trace sharpness
decreases. This can be corrected to a certain extent.
Assuming that the trace sharpness was set to optimum in
the screen center, it is unavoidable that the trace sharpness
decreases with an increasing distance from the center.
Since the settings of the signal(s) intensity (A) and the
READOUT (RO) are usually different, the FOCUS should
be set for optimum signal(s) sharpness. The sharpness of
the READOUT then can be improved by reducing the
READOUT intensity.
(4) RM
The remote control mode can be switched on or off (”RM”
LED dark) via the
lit, all electronically selectable controls on the front panel
are inactive. This state can be cancelled by depressing the
AUTOSET
the interface.
(5) RECALL / SAVE
The instrument contains 9 non volatile memories. These
can be used by the operator to save instrument settings
and to recall them.
SAVE:
Press and hold the RECALL/SAVE button to start a storage
process. This causes the SAVE menu (Standard menu, note
“B: Menu-Display and Operation”) to be displayed. Choose
the memory location cipher (highlighted) by pressing a
RS232
interface. When the ”RM” LED is
pushbutton provided it was not deactivated via
Pushbutton for instrument settings
12
Subject to change without notice
Controls and readout
pushbutton underneath the triangle symbols. Briefly press
the pushbutton underneath “SET” to store the last
instrument setting and return from menu display to
previous mode. If the SAVE function was called inadvertently, it can be switched off with “Esc”.
Switching the instrument off automatically stores the
current settings in memory location 9 (PWR OFF = Power
Off), with the effect that different settings previously stored
in this location get lost. To prevent this, RECALL 9 before
switching the instrument off.
RECALL:
Briefly pressing calls the RECALL menu. You can select
the required memory location using a “triangle” pushbutton. Recall the previously stored instrument settings
by briefly pressing the “SET” pushbutton or briefly press
“Esc” if the function was called inadvertently.
RECALL also offers the item DEFAULTS, which covers all
functions.
The setting controls and LED’s for the Y amplifiers,
modes, triggering and time base are located underneath the sector of the front panel described above.
coupling, a
trace position in vertical direction. The DC voltage then
can be determined by taking the deflection coefficient,
the probe factor and the trace position change with respect
to the previous 0 Volt position into account.
”0 Volt” Symbol:
The READOUT indicates the “0 Volt” trace position of
channel I by a
center line in CHI and DUAL
used, this symbol changes to an “arrow” symbol pointing
outside the graticule just before the trace goes outside
the graticule limits
If addition mode (“add”) is present just one ”?
is visible.
In XY mode the “0 Volt” trace position for channel I (X) and
channel II (Y) is symbolised by “triangle” symbols at the
right graticule border (Y) and above the Y deflection
coefficient display. The “triangle” symbol(s) point(s)
outside the graticule when the “0 Volt” trace position is
outside the graticule.
CURS.I:
The CURSOR lines marked by the symbol “I” can be shifted
by the Y-POS/CURS. I control knob, if the CURSOR POS
LED (7) is lit.
DCDC
DC signal applied at the input changes the
DCDC
””
⊥⊥
””
”
⊥
” symbol to the left of the screen‘s vertical
””
⊥⊥
””
mode. When Y position is
⊥” symbol
(6) Y-POS/CURS. I Control knob with several functions.
This knob allows position control of channel I trace or
CURSOR line(s). Briefly pressing the CURSOR POS
pushbutton (7) selects the function. If the CURSOR line(s)
are not displayed the CURS. I function is not selectable.
Y-POS:
The vertical trace position of channel I can be set with
this control knob, if the CURSOR POS (7) LED isn’t lit. In
addition (“add”) mode both (Y-POS/CURS. I (6) and Y POS/CURS. II) control knobs are active. If the instrument is set
XY XY
to
XY mode this control knob is
XY XY
(12)
knob must be used for horizontal positioning.
DC voltage measurement:
If no signal is applied at the INPUT CHI (25), the vertical trace
position represents 0 Volt. This is the case if INPUT CHI (25)
or in addition (ADD) mode, both INPUT CHI (25) and INPUTCHII (28), are set to GND (ground) (26) (29) and automatic
triggering (AT (9)) is present to make the trace visible.
The trace can then be set to the vertical position best
suited for the following DC voltage measurement. After
switching GND
(ground) off and selecting DC input
inactiveinactive
inactive and the
inactiveinactive
X POS.
STORAGE MODE ONLY
In contrast to analog mode the Y-POS/CURS.I (6) knob must
be used for X position shift in XY mode and the X-POS.
knob is disabled.
The Y-POS/CURS.I (6) knob can also be used for shifting a
signal position although it is stored by HOLD (“hld“).
If a REFERENCE or MATH (mathematic) signal is displayed
and the M/R [38] LED is lit, the Y-POS/CURS.I (6) knob serves
as a MATHEMATIC or REFERENCE position control.
(7) CURSOR POS
Briefly pressing this pushbutton determines the function
of the Y POS/CURS.I (6) and Y POS/CURS.II (8) controls.
If the CUR LED is not lit the Y position control function is
active.
Provided that the CURSOR lines are activated, the LED
can be switched on by briefly pressing the CURSOR POS
pushbutton. Then the controls (6) and (8) are switched
over from Y position to CURSOR position control (CURS.I
(6) and CURS.II (8)). Briefly pressing this pushbutton once
again switches back to the Y position control function.
The CUR LED extinguishes after a
(mathematic) signal is displayed and the M/R LED is switched
on by the MATH/REF POS [38] pushbutton. Under these
conditions the Y-POS/CURS.I (6) knob serves as a REFERENCE
or MATH (mathematic) signal position control, while Y-POS/
CURS.II (8) affects the channel II signal if present.
(8) Y POS/CURS. II Control knob with two functions.
This knob enables position control of channel II trace or
CURSOR line(s). Briefly pressing the CURSOR POS
pushbutton (7) selects the function. If the CURSOR line(s)
are not displayed the CURS. I function is not selectable.
Pushbutton and LED.
STORAGE MODE ONLY
REFERENCE or MATH
Subject to change without notice
13
Controls and readout
Y POS:
The vertical trace position of channel II can be set with
this control knob, if the CURSOR POS LED isn’t lit. In
addition (“add”) mode both (Y POS/CURS. I (6) and
Y
POS/CURS. II) control knobs are active. If the instrument
is set to
POS. (12) POS. (12)
POS. (12) knob must be used for horizontal positioning.
POS. (12) POS. (12)
XY XY
XY mode, this control knob is
XY XY
inactiveinactive
inactive and the
inactiveinactive
X X
X
X X
DC voltage measurement:
If no signal is applied at the INPUT CHII (28), the vertical
trace position represents 0 Volt. This is the case if INPUTCHII (28) or in addition (ADD) mode, both INPUT CHI (25)
and INPUT CHII
automatic triggering (AT (9))
(28), are set to GND (ground) (26) (29) and
is present to make the trace
visible.
The trace can then be set to the vertical position best
suited for the following DC voltage measurement. After
switching GND
(ground) off and selecting DC input
coupling, a DC signal applied at the input changes the
trace position in vertical direction. The
DCDC
DC voltage then
DCDC
can be determined by taking the deflection coefficient,
the probe factor and the trace position change with respect
to the previous 0 Volt position into account.
”0 Volt” Symbol:
The READOUT indicates the “0 Volt” trace position of
channel II by a ”
vertical center line in CHII and DUAL
⊥⊥
⊥” symbol to the right of the screen‘s
⊥⊥
mode. When Y position
is used, this symbol changes to an “arrow” symbol
pointing outside the graticule just before the trace goes
outside the graticule limits
If addition mode (“add”) is present just one ”⊥” symbol is
visible.
In the automatic peak value triggering condition the LEVEL
control (11) range is limited to the trigger signal positive
and negative peak values. Automatic triggering without
peak value detection enables the trigger point to be set
outside the signal amplitude range. In the latter case,
although untriggered, there is still a signal display.
Whether the peak value detection is active or not depends
on the operating mode and the selected trigger coupling.
The actual state is recognised by the behaviour of the
trigger point symbol when changing the LEVEL setting.
NM:
Normal triggering disables both the automatic trigger and
the peak value detection so even low frequency signals
can be displayed in a stable manner. Without suitable input
signal height, trigger coupling and LEVEL settings, no trace
will be displayed.
Analog only:
The last LEVEL setting of the time base is stored, then the
control again becomes active when selecting triggering
after delay (DEL.MODE (“dTr”)) time base mode (quasi
2nd time base). In combination with In “dTr” mode the
LEVEL control is operative for the “2
nd
time base”.
/ \ (Slope selection):
Each time this pushbutton is briefly pressed, the slope direction
switches from falling edge to rising edge and vice versa. The
current setting is displayed in the readout by a slope symbol.
The last setting in undelayed time base mode is stored and
still active if triggered delay
(“dTr”)
time base mode is selected
(analog only). This allows for a different slope setting for the
triggered
DELAY (dtr)
time base mode.
In XY mode the “0 Volt” trace position for channel I (X) and
channel II (Y) is symbolised by “triangle” symbols at the
right graticule border (Y) and above the Y deflection
coefficient display. The “triangle” symbol(s) point(s)
outside the graticule when the “0 Volt” trace position is
outside the graticule.
CURS.II:
If the CUR (7) LED is lit, the CURSOR line(s) marked with
the symbol “II” can be shifted by the Y-POS/CURS. II (8)
control knob.
STORAGE MODE ONLY
The Y-POS/CURS.II (8) knob can also be used for shifting a
signal position although it is stored by HOLD (“hld“).
(9) NM AT Pushbutton with a double function and associated
NM LED.
NM AT selection:
Press and hold the pushbutton to switch over from
automatic (peak value) to normal triggering (NM LED
above the pushbutton lit) and vice versa. If the LED is
dark, automatic or automatic peak value triggering is
selected.
AT:
Automatic triggering can be carried out with or without
peak capture. In both cases the LEVEL control (11) is
effective and the trace is visible even if no signal is applied
or trigger settings are unsuitable. Signal frequencies
below the automatic trigger frequency can not be
triggered as the automatic trigger cycle starts to early for
such signals.
(10) TR Trigger indicator LED.
The
TR
LED is lit in
Yt
mode if the triggering conditions
are met for the first trigger unit used in undelayed time
base mode. Whether the LED flashes or is lit constantly
depends on the frequency of the trigger signal.
In XY mode the TR LED is switched off.
(11) LEVEL Control knob.
Turning the
LEVEL
knob causes a different trigger point
setting (voltage). The trigger unit starts the time base when
the edge of a trigger signal crosses the trigger point. In
most Yt modes the trigger point is displayed in the readout
by the symbol on the left vertical graticule line. If the trigger
point symbol would overwrite other readout information
14
Subject to change without notice
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