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: HM504-2
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
KONFORMITÄTSERKLÄRUNG
DECLARATION OF CONFORMITY
DECLARATION DE CONFORMITE
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
25.6.2003
G. Hübenett
Product Manager
B.
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.
cable HZ72 from HAMEG is 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.
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
HM504-2
� 2 Channels with deflection coefficients 1mV/div.…20V/div.
� Time Base 50ns /div.…0.5s/div.,
with X Magnification to 10ns/div.
� Low Noise Measuring Amplifiers with high pulse fidelity
� Triggering 0…100MHz from 5mm signal level
� Time Base delay provide high X Magnification
of any portion of the signal
� 100MHz 4-Digit Frequency Counter,
Cursor and Automatic Measurement
� Save/Recall Memories for Instrument Settings
� Readout, Autoset, no Fan
� Yt, XY and component-test modes
� RS-232 Interface (for parameter queries and control only)
5 0 M H z An a lo g O s c i ll o s co p e
H M 5 04 - 2
HM504-2
Optimum deflection
linearity
Rise-time measurement
with cursor
Full screen display of
50 MHz sine wave
50MHz Analog Oscilloscope HM504-2
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
Hold-Off Time:variable to approx. 10 : 1
XY
Bandwidth X amplifier:0…3 MHz (-3dB)
XY Phase shift ‹ 3 °:‹120 kHz
Operation/Readout/Control
Manual:via controls
Autoset:automatic signal related parameter settings
Save and Recall:9 instrument parameter settings
Readout:display of menu, parameters, cursors and
results
Autom. Measurement:Freq./Period, V
dc
, Vpp, Vp+, Vp-,
Trigger Level
Cursor Measurement:Δt, 1/Δt, tr, ΔV, V to GND, Gain, Ratio X and Y
Frequency counter:4 digit (0.01 % ± 1 digit) 0.5 Hz…100MHz
Interface:RS-232
1)
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. 2kV
Trace Rotation:adjustable on front panel
Z-input (Intens. modulation): max. + 5 V (TTL)
Calibrator Signal (Square Wave):0.2V, 1 Hz…1MHz (tr ‹ 4 ns), DC
Power Supply (Mains):105…253 V, 50/60 Hz ± 10 %, CAT II
Power Consumption:approx. 34Watt 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. 5.4kg
1)
Device control and Parameter query, no CRT content transfer possible.
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:
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)
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
Automatic(Peak to Peak):20Hz…100MHz (≥5mm)Normal with Level Control:0…100MHz (≥5mm)Slope:Rising or fallingSources:Channel1or2,CH1/CH2alternate
(≥8mm),LineandExternal
Coupling:AC (10Hz…100MHz), DC (0…100MHz),
HF (50kHz…100MHz), LF (0…1.5kHz)
Trigger Indicator:LEDTriggering after Delay:with Level Control and Slope selectionExternal Trigger Signal:≥0.3V
pp
(0…50MHz)
Active TV sync. separator:Field and Line, +/-
Horizontal Deflection
Time Base:50ns/div.…0.5s/div. (1-2-5 Sequence)
Accuracy:± 3%Variable (uncalibrated):› 2.5:1 to › 1.25s/div.
X Magnification x 10:up to 10ns/div. (± 5%)
Accuracy:± 5%
Delay(selectable):200
ns…140ms (variable)
Hold-Off Time:variable to approx. 10 : 1XYBandwidth X amplifier:0…3MHz (-3dB)XY Phase shift ‹3°:‹120kHz
Operation/Readout/Control
Manual:via controlsAutoset:automatic signal related parameter settingsSave and Recall:9 instrument parameter settingsReadout:display of menu, parameters, cursors and
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):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. 34Watt 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. 5.4kg
1)
Device control and Parameter query, no CRT content transfer possible.
Accessories supplied:Line Cord, Operators Manual and Software for Windowson CD-ROM, 2 Probes 1:1/10:1(HZ154), RS-232 Interface
Optional accessories:
HZ14Interface 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)HZ100Differential 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
Specifications
Subject to change without notice
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 u il d i n gs ( p o w e r d i s t ri b u t i on i n s ta l 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 temperatures 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 HM504-2 allows examination of DC voltages
and most repetitive signals in the frequency range up to at least
50 MHz (–3 dB).
The Y 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.
14 MHz. At approx. 30 MHz the reduction is approx. 10% and the
real voltage value is 11% higher. The gain reduction error can not
be defined exactly as the –3 dB bandwidth of the Y amplifiers
differs between 50 MHz and 55 MHz.
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 Y amplifiers.
Displaying composite signals can be difficult, especially if they
contain no repetitive higher amplitude content that 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 Y
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.
Voltage values of a sine curve
= effective value; Vp = simple peak or crest value;
V
rms
= peak to peak value; V
V
pp
= momentary value.
mom
The minimum signal voltage which must be applied to the Y input
for a trace of 1div height is 1mV
(± 5%) with this deflection
pp
coefficient displayed on the screen (readout) and the vernier
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.
This factor can be entered into the oscilloscope’s memory for
automatic calculation.
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 (
readout”
). Therefore any intermediate value is possible within
please note ”controls and
the 1-2-5 sequence of the attenuator(s).
When displaying very low frequency pulses, the flat tops may be
sloping with AC coupling of the Y 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 too high a DC
level. Otherwise a capacitor of adequate capacitance must be
connected to the input of the Y 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.
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 (V
) value
pp
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 peak
to peak value must be divided by 2 x √2 = 2.83. Conversely, it
should be observed that sinusoidal voltages indicated in Vrms
) have 2.83 times the potential difference in Vpp. The
(V
eff
relationship between the different voltage magnitudes can be
seen from the following figure.
With direct connection to the Y input, signals up to 400 V
pp
may be displayed (attenuator set to 20 V/div, variable
control to 2.5:1).
With the designations
H = display height in div,
U = signal voltage in V
at the Y input,
pp
D = deflection coefficient in V/div at attenuator switch,
the required value can be calculated from the two given quantities:
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 0.5 mV
and 160 Vpp,
pp
D between 1 mV/div and 20 V/div in 1-2-5 sequence.
Examples:
Set deflection coefficient D = 50 mV/div 0.05 V/div,
observed display height H = 4.6 div,
required voltage U = 0.05x4.6 = 0.23 V
pp
.
8
Subject to change without notice
Type of signal voltage
Input voltage U = 5 Vpp,
set deflection coefficient D = 1 V/div,
required display height H = 5:1 = 5 div.
Signal voltage U = 230 V
x 2√2 = 651 V
rms
pp
(voltage > 160 Vpp, with probe 10:1: U = 65.1 Vpp),
desired display height H = min. 3.2 div, max. 8 div,
max. deflection coefficient D = 65.1:3.2 = 20.3 V/div,
min. deflection coefficient D = 65.1:8 = 8.1 V/div,
adjusted deflection coefficient D = 10 V/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 400 V, irrespective of 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 –400 V. So for AC voltages with a mean value of zero
volt the maximum peak to peak value is 800 Vpp.
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 400 V.
The attenuator consists of a resistor in the probe and the
1 MOhm input resistor of the oscilloscope, which is 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 reactance of the
AC input coupling capacitor, the attenuation ratio depends on the
signal frequency. For sine wave signals with frequencies higher
than 40 Hz this influence is negligible.
Apart from the above listed exceptions, HAMEG 10:1 probes can
be used for DC measurements up to 600 V or AC voltages (with
a mean value of zero volt) of 1200 V
allows for use up to 1200 V DC or 2400 V
. The 100 :1 probe HZ53
pp
for AC.
pp
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.
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).
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 Dt and 1/Dt cursor
measurement (
please 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 can be stated:
).
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.
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.
Subject to change without notice
However, these four values are not freely selectable. They
have to be within the following limits:
L between 0.2 and 10 div, if possible 4 to 10 div,
T between 10 ns and 5 s,
F between 0.5 Hz and 100 MHz,
Tc between 100 ns/div and 500 ms/div in 1-2-5 sequence
(with X-MAG. (x10) inactive), and
Tc between 10 ns/div and 50 ms/div in 1-2-5 sequence (with
X-MAG. (x10) active).
9
Type of signal voltage
Examples:
Displayed wavelength L = 7 div,
set time coefficient Tc = 100 ns/div,
-9
thus period T = 7 x 100 x 10
thus freq. F = 1/(0.7 x 10
= 0.7 µs
-6
) = 1.428 MHz.
Signal period T = 1s,
set time coefficient Tc = 0.2 s/div,
thus wavelength L = 1/0.2 = 5 div.
Displayed ripple wavelength L = 1 div,
set time coefficient Tc = 10 ms/div,
-3
thus ripple freq. F = 1/(1 x 10 x 10
) = 100 Hz.
TV Line frequency F = 15625 Hz,
set time coefficient Tc = 10 µs/div,
required wavelength L = 1/(15,625 x 10-5) = 6.4 div.
Sine wavelength L = min. 4 div, max. 10 div,
Frequency F = 1 kHz,
max. time coefficient Tc = 1/(4 x 10
min. time coefficient Tc = 1/(10 x 10
3
) = 0.25 ms/div,
3
) = 0.1 ms/div,
set time coefficient Tc = 0.2 ms/div,
required wavelength L = 1/(103 x 0.2 x 10-3) = 5 div.
Displayed wavelength L = 0.8 div,
set time coefficient Tc = 0.5 µs/div,
pressed X-MAG. (x10) button: Tc = 0.05 µs/div,
-6
thus freq. F = 1/(0.8 x 0.05 x 10
thus period T = 1/(25 x 10
6
) = 25 MHz,
) = 40 ns.
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.
Rise Time Measurement
When investigating pulse or square waveforms, the critical
feature is the rise time of the voltage step. To ensure that
transients, ramp-offs, and bandwidth limits do not unduly influence
the measuring accuracy, the rise time 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 rise time measurement.
With a time coefficient of 10 ns/div (X x10 magnification active),
the example shown in the above figure results in a total measured
risetime of
t
= 1.6 div x 10 ns/div = 16 ns
tot
When very fast risetimes are being measured, the risetimes of
the oscilloscope amplifier and of the attenuator probe have to be
deducted from the measured time value. The risetime of the
signal can be calculated using the following formula.
2
2
= √ t
t
r
In this t
– t
tot
osc
is the total measured risetime, t
tot
oscilloscope amplifier (approx. 7 ns), and t
probe (e.g. = 2 ns). If t
2
– t
p
is the risetime of the
osc
p
is greater than 100 ns, then t
tot
the risetime of the
can be
tot
taken as the risetime of the pulse, and calculation is unnecessary.
Calculation of the example in the figure above results in a signal
risetime:
= √162 – 72 – 22 = 14.25 ns
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 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 AUTOSET causes a useful
signal related instrument setting. The following explanations
refer to special applications and/or signals, demanding a manual
instrument setting.
in the section ”controls and readout”.
Caution:
When connecting unknown signals to the oscilloscope input,
always use automatic triggering and set the input coupling switch to AC. The attenuator should initially be set to
20 V/div.
The description of the controls is explained
10
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 – 8 div.
With a signal amplitude greater than 160 V
and the deflection
pp
coefficient (VOLTS/DIV.) in calibrated condition, an attenuator
probe must be inserted before the Y 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.
Subject to change without notice
Controls and Readout
The signal to be displayed can be connected directly to the Y input
of the oscilloscope with a shielded test cable such as HZ32 orHZ34, 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. 50 kHz).
For higher frequencies, the signal source must be of low
impedance, i.e. matched to the characteristic resistance of the
cable (as a rule 50 Ohm). 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 50 Ohm cable such as
the HZ34, a 50 Ohm 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 2 Watts. This power is
reached with 10 V
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 attenuator
probes, even high internal impedance sources are only slightly
loaded (approx. 10 MOhm II 12 pF or 100 MOhm II 5 pF 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 Y
amplifier. Because of their separate manufacture, all attenuator
probes are only partially compensated, therefore accurate
compensation must be performed on the oscilloscope
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 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 an HF-adjustment 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 a 1 MHz 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 oscilloscope’s individual pulse response.
If a x10 or x100 attenuator probe is used, DC input coupling
must always be used at voltages above 400 V. With AC
coupling of low frequency signals, the attenuation is no
longer independent of frequency, pulse tops can show pulse
tilts. Direct voltages are suppressed but charge 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).
(28.3 Vpp) with sine signal. If a x10 or x100
rms
.
(see Probe
With all attenuator probes, the maximum AC input voltage must
be derated with frequency, usually above 20 kHz. 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 BNC adapter 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).
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.
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” CT pushbutton [37] switches one step back in the menu
hierarchy.
“Exit” SELECT – ON/OFF pushbutton [34] closes the menu and
switches back to the operating conditions present before calling
the menu.
The pushbuttons underneath the triangle symbols pointing
upwards UNIT CAL.SEL. [35] and downwards SOURCE GLUE
[33] enable you to select one item which becomes highlighted.
Subject to change without notice
11
Controls and Readout
A
FO
O
M
“SET” MAIN MENU-pushbutton [31] calls the selected menu
item, starts a function or switches a function on/off.
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 the pushbutton, the Pulldown menu
extinguishes after a few seconds and the selected parameter is
displayed in the normal way.
C: READOUT Information
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:
1st time deflection coefficient
2nd trigger source, slope and coupling
3rd operating condition of delay time base
4th measuring results
Bottom of the graticule from left to right:
1st probe symbol (x10), Y deflection coefficient and input
coupling channel I
2nd “+” symbol (addition)
3rd probe symbol (x10), Y deflection coefficient and input
coupling channel II
4th channel mode
The trigger point symbol is displayed at the left graticule border
line. The CURSOR lines can take any position within the graticule.
[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
or DUAL).
The instrument is set automatically to normal (undelayed)
time base mode, even if the previous Yt mode was present
in combination with search (“sea”), delay (“del”) or triggered
delay (“dTr”) time base mode.
Please also note ”AUTO-
SET” in section “First Time Operation”.
Automatic CURSOR positioning:
If CURSOR lines are displayed and AUTOSET is chosen the
CURSOR lines are set automatically under suitable conditions
and the readout briefly displays “SETTING CURSOR”.
If the signal height is insufficient, the CURSOR lines do not
change. In DUAL mode the CURSOR lines are related 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.
[3] INTENS/FOCUS – Knob with associated LEDs and TRACE
ROT.-pushbutton.
If the readout (RO) is not switched off, briefly pressing the
READOUT pushbutton switches over the INTENS/FOCUS
knob function indicated by a LED in the sequence A, FOC,
RO, A. In condition READOUT deactivated, the switching
sequence is A, FOC, A.
Description of Controls
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.
1345
2
POWER
AUTOSET
[1] POWER – Pushbutton and symbols for ON (I) and OFF (O).
INTENS / FOCUS
!
C
R
TRACE
ROT.
Instruments
50 MHz
R
ANALOG OSCILLOSCOPE
HM504-2
RECALL
SAVE
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. Then the last used settings become activated and
LED [3] indicates the ON condition.
“A”:
The INTENS/FOCUS control knob adjusts 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.
“FOC”:
The INTENS/FOCUS control knob adjusts 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
centre, it is unavoidable that the trace sharpness decreases
with an increasing distance from the centre.
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.
“RO”:
The INTENS/FOCUS control knob adjusts the READOUT
intensity. Turning this knob clockwise increases and counter
clockwise decreases the intensity. Only the minimum required
intensity should be used.
12
Subject to change without notice
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