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9

Subject to change without notice

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 1M

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.

In the GD (ground coupling) setting, the signal path is interrupted
directly beyond the input. This causes the attenuator to be
disabled again, but now for both DC and AC voltages.

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 ACpeak 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. 22-
68nF) must be connected in series with the input tip of the
probe.

Total value of input voltage

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).

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.

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 of the 

TIME/DIV.

 switch, one or several signal

periods or only a part of a period can be displayed. The time
coefficients are stated in 

s/div.

ms/div.

 and 

µs/div.

 on the

TIME/DIV.

-switch. The scale is accordingly divided into three

fields.

The duration of a signal period or a part of it is determined by
multiplying the relevant time (horizontal distance in div.) by the
time coefficient set on the 

TIME/DIV.

-switch.

The variable time control (identified with an arrow knob
cap) must be in its calibrated position CAL.

 (arrow pointing

horizontally to the right).

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 s/div.

 on time base switch and

   the relation 

F = 1/T

, the following equations

   can be stated:

With depressed X-MAG. (x10) pushbutton the Tc value must be
divided by 10.

However, these four values are not freely selectable. They
have to be within the following limits:

L

between 0.2 and 10div., if possible 4 to 10div.,

T

between 0.01µs and 2s,

F

between 0.5Hz and 30MHz,

Tc

between 0.1µs/div. and 0.2s/div. in 1-2-5 sequence
(with 

X-MAG. (x10)

 in out position), and

Tc

between 10ns/div. and 20ms/div. in 1-2-5 sequence
(with pushed 

X-MAG. (x10)

 pushbutton).

Examples:
Displayed wavelength L = 7div.,
set time coefficient Tc = 0.1µs/div.,
required period T = 7x0.1x10

-6

 = 0.7µs

required rec. freq. F = 1:(0.7x10

-6

) = 1.428MHz.

Signal period T = 1s,
set time coefficient Tc = 0.2s/div.,
required wavelength L = 1:0.2 = 5div..

Displayed ripple wavelength L = 1div.,
set time coefficient Tc = 10ms/div.,
required ripple freq. F = 1:(1x10x10

-3

) = 100Hz.

TV-line frequency F = 15625Hz,
set time coefficient Tc = 10µs/div.,
required wavelength L = 1:(15 625x10

-5

) = 6.4div..

Sine wavelength L = min. 4div., max. 10div.,
Frequency F = 1kHz,
max. time coefficient Tc = 1:(4x10

3

) = 0.25ms/div.,

min. time coefficient Tc = 1:(10x10

3

) = 0.1ms/div.,

set time coefficient Tc = 0.2ms/div.,
required wavelength L = 1:(10

3

x0.2x10

-3

) = 5div.

Displayed wavelength L = 0.8div.,
set time coefficient Tc = 0.5µs/div.,
pressed X-MAG. (x10) button: Tc = 0.05µs/div.,
required rec. freq. F = 1:(0.8x0.05x10

-6

) = 25MHz,

required period T = 1:(25x10

-6

) = 40ns.

If the time is relatively short as compared with the complete
signal period, an expanded time scale should always be
applied (

X-MAG. x10

 button pressed). In this case, the

ascertained time values have to be divided by 

10

. The time

interval of interest can be shifted to the screen center using
the 

X-POS

. control.

Type of signal voltage

Summary of Contents for HM303-6

Page 1: ...O s c i l l o s c o p e H M 3 0 3 6 Manual English...

Page 2: ...lifiers 12 X Y Operation 13 Phase comparison with Lissajous figures 13 Phase difference measurement 13 in DUAL mode 13 Phase difference measurement in DUAL mode 14 Measurement of an amplitude modulati...

Page 3: ...effected by such fields Although the interior of the oscilloscope is screened by the cabinet direct radiation can occur via the CRT gap As the bandwidth of each amplifier stage is higher than the tot...

Page 4: ...oise Amplifiers Time Base 0 2 s 100 ns cm with X Magnification to 10 ns cm Triggering from 0 to 50 MHz from 5 mm signal level 100 MHz 8 mm Analog mode provides unexcelled signal presentation at high r...

Page 5: ...1 s div 1 2 5 Sequence Accuracy 3 Variabel uncalibrated 2 5 1 to 0 5 s div X Magnification x 10 up to 10 ns div Accuracy 5 Hold Off Time variable to approx 10 1 XY Bandwidth X Amplifier 0 2 5 MHz 3 d...

Page 6: ...Without pulling the locking knobs they will latch in into the next locking position Handle mounting dismounting The handle can be removed by pulling it out further depending on the instrument model in...

Page 7: ...e atmosphere or if there is danger of explosion The operating position may be any however sufficient ventilation mustbeensured convectioncooling Prolongedoperationrequires the horizontal or inclined p...

Page 8: ...83 times the potential difference in Vpp The relationship between the different voltage magnitudes can be seen from the following figure Voltage values of a sine curve Vrms effective value Vp simple p...

Page 9: ...frequency Depending on the time base setting of the TIME DIV switch one or several signal periods or only a part of a period can be displayed The time coefficients are stated in s div ms div and s div...

Page 10: ...d The attenuator switch must then be turned back to the left until the vertical signal height is only 3 8div With a signal amplitude greater than 160Vpp an attenuator probe must be inserted before the...

Page 11: ...be visible after a short warm up period of approx 10 seconds Adjust Y POS I and X POS controls to center the baseline Adjust INTENS intensity and FOCUS controls for medium brightness and optimum sharp...

Page 12: ...is slightly more difficult but causes a better result The rising edge should be as steep as possible with a pulse top remaining as straight and horizontal as possible After completion of the HF adjus...

Page 13: ...uite simple with the following formula and a pocket calculator with trigonometric functions Apart from the reading accuracy the signal height has no influence on the result The following must be noted...

Page 14: ...tion F 1 MHz f 1 kHz m 50 UT 28 3 mVrms If the two values a and b are read from the screen the modulation factor is calculated from where a UT 1 m and b UT 1 m The variable controls for amplitude and...

Page 15: ...a positive potential That has nothing to do with zero or ground potential and absolute voltage values The positive slope may also lie in a negative part of a signal A falling edge sign triggers when...

Page 16: ...ossible in this trigger mode External triggering The internal triggering is disconnected by depressing the TRIG EXT button The time base can be triggered externally via the TRIG EXT socket using a 0 3...

Page 17: ...are required The test leads are connected to the insulated socket and the adjacent ground socket beneath the screen The component can be connected to the test leads either way round After use to retu...

Page 18: ...can be identified by comparison with a known diode Testing Transistors Three different tests can be made to transistors base emitter base collector and emitter collector The resulting test patterns ar...

Page 19: ...soldered This terminal should then be connected to the insulated COMP TESTER socket avoiding hum distortion of the test pattern Another way is a test pattern comparison to an identical circuit which i...

Page 20: ...II display SLOPE Selects the slope of the trigger signal Element Function SLOPE rising edge pushbutton switch falling edge TR LED lights if sweep is triggered LED LEVEL Adjustment of trigger level kno...

Page 21: ...ast 2 5 fold For time measurements turn to right hand stop Element Function XY Selects X Y operation pushbutton switch stops sweep X signal via CH I Attention Phosphor burn in without signal TRIG EXT...

Page 22: ...ggering TRIG EXT pushbutton depressed sync signal 0 3Vpp to 3Vpp to TRIG EXT socket Line triggering normal triggering AT NM and ALT pushbuttons depressed Select trigger coupling with TRIG MODE selecto...

Page 23: ...M A N U A L H A N D B U C H M A N U E L...

Page 24: ...stra e 6 A Rohde Schwarz Company D 63533 Mainhausen registrierte Marke Tel 49 0 61 82 800 0 DQS Zerti kation DIN EN ISO 9001 2000 Fax 49 0 61 82 800 100 Reg Nr 071040 QM sales hameg de Oscilloscopes S...

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