Hameg CombiScope HM2008 User Manual

200 MHz Mixed Signal
CombiScope
®
HM2008
Manual
English
Subject to change without notice
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 emission 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 instrument 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 IEEE-bus purposes the double screened 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.
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: HM2008
mit / with / avec: HO720, HZ200
Optionen / Options / Options: HO730, HO740, HO2010
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
Angewendete harmonisierte Normen / Harmonized standards applied / Normes harmonisées utilisées:
Sicherheit / Safety / Sécurité: EN 61010-1:2001 (IEC 61010-1:2001) Überspannungskategorie / Overvoltage category / Catégorie de surtension: II Verschmutzungsgrad / Degree of pollution / Degré de pollution: 2
Elektromagnetische Verträglichkeit / Electromagnetic compatibility / Compatibilité électromagnétique
EN 61326-1/A1 Störaussendung / Radiation / Emission: Tabelle / table / tableau 4; Klasse / Class / Classe B.
Störfestigkeit / Immunity / Imunitée: 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
02. 04. 2007 Unterschrift / Signature / Signatur
Holger Asmussen Manager
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, 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 of 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
Hersteller HAMEG Instruments GmbH KONFORMITÄTSERKLÄRUNG Manufacturer Industriestraße 6 DECLARATION OF CONFORMITY Fabricant D-63533 Mainhausen DECLARATION DE CONFORMITE
General information regarding the CE marking
Subject to change without notice
Contents
General information regarding the CE marking 2
200 MHz Mixed Signal CombiScope
®
HM2008 4
Specifi cations 5
Important hints 6
List of symbols used: 6 Positioning the instrument 6 Safety 6 Proper operation 6 CAT I 6 Environment of use. 6 Environmental conditions 7 Warranty and repair 7 Maintenance 7 Line voltage 7
Front Panel Elements – Brief Description 8
Basic signal measurement 10
Signals which can be measured 10 Amplitude of signals 10 Values of a sine wave signal 10 DC and AC components of an input signal 11 Timing relationships 11 Connection of signals 11
First time operation and initial adjustments 12
Trace rotation TR 12 Probe adjustment and use 12 1 kHz – adjustment 12 1 MHz adjustment 13
Operating modes of the vertical amplifi er 13
XY operation 14 Phase measurements with Lissajous fi gures 14 Measurement of phase differences in
dual channel Yt mode 14
Measurement of amplitude modulation 15
Triggering and time base 15
Automatic peak triggering (MODE menu) 15 Normal trigger mode (See menu MODE) 16 Slope selection (Menu FILTER) 16 Trigger coupling (Menu: FILTER) 16 Video (tv triggering) 16 Frame sync pulse triggering 17 Line sync pulse triggering 17 LINE trigger 17 Alternate trigger 17 External triggering 17 Indication of triggered operation (TRIG’D LED) 17 Hold-off time adjustment 18 Time base B (2nd time base). Delaying, Delayed Sweep. Analog mode 18 Alternate sweep 18
AUTOSET 19
Component Tester 19
CombiScope® 21
Signal display modes 21 Vertical resolution 21 Horizontal resolution 22 Memory depth 22 Horizontal resolution using ZOOM 22 (variable X magnifi cation) 22 Maximum signal frequency in digital mode 23 Display of aliases 23 Vertical amplifier operating modes 23
Data transfer 24
Description 24
Accessories supplied + Options 24
General information concerning MENU 25
Menu and HELP displays 25
Controls and Readout 26
Subject to change without notice
HM2008
2GSa/s Real Time Sampling, 20GSa/s Random Sampling
2MPts Memory per Channel, Memory oom up to 100,000:1
FFT for spectral analysis
2 Channels + 4 Logic Channels with Option HO2010 (MSO)
Deflection coefficients 1mV/div.…5V/div.,
with adjustable DC offset voltage; Time Base 2ns/div.…50s/div.
Acquisition modes: Single, Refresh, Average, Envelope,
Roll, Peak-Detect
Front USB-Stick Connector for Screenshots
USB/RS-232, optional: IEEE-488 or Ethernet/USB
Signal display: Yt, XY and FFT;
Interpolation: Sinx/x, Pulse, Dot Join (linear)
Adjustable input impedance 1MΩ/50Ω
See HM2005-2 for analog mode
200MHz Mixed Signal
CombiScope
®
HM2008
HM2008
Frequency Analysis of a Video Signal with FFT
Rise Time Measurement in DSO Mode with 2ns/div., 2GSa/s
Logic Probe HO2010
Subject to change without notice
Specifications
200 MHz Mixed Signal CombiScope®HM2008
All data valid at 23 °C after 30 minute warm-up
Vertical Deflection
Channels:
Analog: 2 Digital: 2 + (additionally with Option HO2010) 4 Logic
Channels
Operating Modes:
Analog: CH 1 or CH 2 separate, DUAL (CH 1 and
CH 2 alternate or chopped), Addition
Digital: Analog Signal Channels: CH 1 or CH 2
separate, DUAL (CH 1 and CH 2) or Addition. Logic Signal Channels (LCH 0…3) switchable.
X in XY-Mode: CH 1 Invert: CH 1, CH 2 Bandwidth (-3dB): 2 x 0…200 MHz Rise time: ‹ 1,75 ns Bandwidth Limiter (switchable): approx. 20MHz (1 mV/div.…5V/div.) Deflection Coefficients (CH 1, 2): 12 calibrated steps
1…2 mV/div.: ± 3 % (0…100MHz (-3 dB)) 5 mV…5 V/div.: ± 3 % (1-2-5 sequence) variable (uncalibrated): › 1 mV/div.…5V/div., continuous
Inputs CH 1, 2:
Impedance: 1 MΩ II 13 pF Coupling: DC, AC, 50Ω, GND (ground) Offset control:
1 mV, 2 mV ± 0.2 V 5…50mV ±1V 100mV…5V ±20V
Max. Input Voltage: 250 V (DC + peak AC), 50Ω ‹ 5V
rms
Y Delay Line (analog): 70 ns Measuring Circuits: Measuring Category I Analog mode only:
Auxiliary input: Function (selectable): Ext. Trigger, Z (unblank in analog mode) Coupling (Ext. Trig./ Z): all/AC, DC
Max. input voltage: 100 V (DC + peak AC) Digital mode only: Logic Channels in combination with Option HO2010:
Quantity 4 (LCH 0…3) Select. switching thresholds: TTL, CMOS, ECL (common for all) User definable thresholds: 2
within the range: -2…+8 V (common for all)
Triggering
Analog and Digital Mode Automatic (Peak to Peak):
Min. signal height: 5mm
Frequency range: 10Hz…250 MHz
Level control range: from Peak- to Peak+ Normal (without peak):
Min. signal height: 5mm
Frequency range: 0…250MHz
Level control range: –10…+10 div. Operating modes: Slope/Video/Logic Slope: Rising, falling, both Sources: CH 1, CH 2, alt. CH 1/2 (8 mm, analog
mode only), Line, Ext.
Coupling: AC: 10 Hz…250MHz
DC: 0…250 MHz HF: 30 kHz…250MHz LF: 0…5 kHz
Noise Rej. switchable
Video: pos. /neg. Sync. Impulse
Standards: 525 Line/60 Hz Systems
625 Line/50 Hz Systems
Field: even/odd/both
Line: all/line number selectable
Source: CH 1, CH 2, Ext. Indicator for trigger action: LED External Trigger via: AUXILIARY INPUT (0.3 Vpp, 0…200MHz) Coupling: AC, DC Max. input voltage: 100V (DC + peak AC) Digital mode: Pre/Post Trigger: -100…+400 % relative to complete memory
Analog mode: 2nd Trigger
Min. signal height: 5mm
Frequency range: 0…250MHz
Coupling: DC
Level control range: -10…+10 div.
Horizontal Deflection
Analog Time Base
Operating modes: A, ALT (alternating A/B), B
Time base A: 20 ns/ div.…0.5 s/ div. (1-2-5 sequence)
Time base B: 20 ns/div…20 ms/div. (1-2-5 sequence)
Accuracy A and B: ±3%
X Magnification x10: to 2 ns/div.
Accuracy: ±5% Variable time base A/B: cont. 1:2.5 Hold Off time: var. 1:10 (LED-Indication)
Analog XY Mode Bandwidth X-Amplifier: 0…3 MHz (-3dB) X Y phase shift: ‹ 3° ‹ 220kHz Digital Time Base Time base range (1-2-5 sequence)
Refresh Mode: 2 ns/div.…50s/div. with Peak Detect: 500ns/div.…50 s/div. (min. Pulse Width 10 ns) Roll Mode: 50 ms/div.…50s/div.
Accuracy time base
Time coefficient: 50 ppm Display: ±1%
MEMORY ZOOM: max. 100,000:1 Digital XY Mode
Bandwidth X-Amplifier: 0…200 MHz (-3dB) XY phase shift: ‹ 3° ‹ 200 MHz
Digital Storage
Sampling Rate (real time): Analog channels: 2 x 1 GSa/s or 1 x 2GSa/s
(interleaved); Logic Channels: max. 4 x 500 MSa/s
Sampling Rate (random sampling): 20 GSa/s (1-Channel mode)
25 GSa/s (2-Channel mode)
Bandwidth: 2 x 0…200 MHz (Random) Memory: 2 x 2MPts (analog); 4 x 2 MPts (logic) Operating modes: Refresh, Average, Envelope, Roll:
Free Run/ Triggered, Peak-Detect
Resolution (vertical): 8Bit (25 Pts/ div.) Resolution (horizontal):
Yt: 11Bit (200 Pts/ div.) XY: 8Bit (25 Pts/div.)
Interpolation: Sinx/ x, Dot Join (linear) Delay: 2 Million x (1/Sampling Rate; max.)
8 Million x (1/Sampling Rate; max.)
Display refresh rate: max.170/s at 2 MPts Display: Dots (acquired points only), Vectors (inter-
polation), Optimal (complete memory weighting and vector display)
Reference Memories: 9 with 2 kPts each (for recorded signals) Display: 2 signals of 9 (freely selectable)
FFT Mode
Display X: Frequency Range Display Y: True rms value of spectrum
Scaling: Linear or logarithmic Level display: dBV, V
Window: Square, Hanning, Hamming, Blackman Control: Center frequency, Span Marker: Frequency, Amplitude Zoom (frequency axis): up to x20
Operation/Measuring /Interfaces
Operation: Menu (multilingual), Autoset, Help functions (multilingual) Save/Recall internal:
analog: 9 Instrument parameter settings digital: 9 Signals (each 2k) incl. instrument parameters Signal sources: CH 1, CH 2, LCH 0…3, ZOOM, Reference 1–9
or Mathematics
Signal display: max. 6 signals
USB Memory-Stick:
Save/Recall external: Instrument settings and Signals: CH1, CH2, LCH 0…3, ZOOM,
Reference 1–9 or Mathematics
Screen-shot: as Bitmap Signal display data (2k per channel): Binary (SCPI-Data), Text (ASCII-
Format), CSV (Spread Sheet)
Logic (with Option HO2010): AND/OR, TRUE/FALSE
Source: Logic Channel 0…3 State: X, H, L
Subject to change without notice
Important hints
Frequency counter:
6 digit resolution: › 1…250MHz 5 digit resolution: 0.5 Hz…1MHz Accuracy: 50 ppm
Auto Measurements:
Analog mode: Frequency, Period, V
dc
, Vpp, Vp+, V
p-
plus in digital mode: V
rms
, V
avg
Cursor Measurements:
Analog mode: Δt, 1/Δt (f), tr, ΔV, V to GND, ratio X, ratio Y plus in digital mode: V
pp
, Vp+, Vp-, V
avg
, V
rms
, pulse count
Resolution Readout/Cursor: 1000 x 2000 Pts, Signals: 250 x 2000 Interfaces (plug-in): USB/RS-232 (HO720) Optional: IEEE-488, Ethernet/USB
Mathematic functions
Number of Formula Sets: 5 with 5 formulas each Sources: CH 1, CH 2, Math 1 - Math 5 Targets: 5 math. memories (Math 1…5) Functions: ADD, SUB, 1/X, ABS, MUL, DIV, SQ, POS,
NEG, INV
Display: max. 2 math. memories (Math 1…5)
Display
CRT: D14-375GH Display area (with graticule): 8div. x 10 div. Acceleration voltage: approx. 14 kV
General Information
Component tester
Test voltage: approx. 7V
rms
(open circuit), approx. 50Hz
Test current: max. 7mA
rms
(short circuit)
Reference Potential: Ground (safety earth)
Probe ADJ Output: 1 kHz/ 1MHz square wave signal 0.2 V
pp
(tr ‹ 4 ns)
Trace rotation: electronic Line voltage: 105…253V, 50/60 Hz ±10 %, CAT II Power consumption: 48 Watt at 230 V, 50 Hz Protective system: 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: 5.6kg
Important hints
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.
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)
A
A
B
B
C
C
D
D
E
E
T
F
PUkT
PUkT
PUk PUk
PUk PUk
PUk PUk
PUkT PUkT
PUkT
PUkT
PUkT
HGOPFFD
PUkT HGOFFD
PUOPFGkT
PUkT
PUkTKl
15pF max
400 Vp
PUOPFGkT
PUOPFGkT
PUOPFGkT
PUOPFGkT
PGkT
PUOPFGkT
PUOPFGkT
PFGkT
PUOPFGkT PUOPFGkT
PUOPFGkT
PUOPFGkT
PUOPFGkT
HAMEG
PUOPFGkT
PUOPFGkT
PUOPFGkT
ANALOG DIGITAL
MIXED SIGNAL
COMBISCOPE
HM1508
1 GSa · 1MB
150 MHz
PUOGkT
VOLTS/DIVV HGOPFFD
VOLTS/DIVV HGOPFFD
VOLTS/DIVV HGOPFFD
PUkT HGOPFFD
PUkT HGOPFFD
PUkT
PUkT
PUkT
PUkT
PUkT
PUkT
PUkT
PUkTKl
15pF max 400 Vp
PUOPFGkT INPUTS
PUOPF
PUOPF
PUOPF
PUOPF PUOPF
C O M B I S C O P E
B
T
T
Attention!
When changing the handle position, the instrument
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.
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 2200 V
DC
. The instrument conforms to safety class I.
For Accessories supplied and options please refer
to page 24.
Subject to change without notice
Important hints
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.
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.
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 fi rm)
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.
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: Measurements in the interior of buildings (power distribution installations, 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.
Environmental conditions
The oscilloscope is destined for operation in industrial, business, manufacturing, and living sites. 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 (convection cooling). Prolonged 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.
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.
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.
Subject to change without notice
Front Panel Elements – Brief Description
Front Panel Elements – Brief Description
1
POWER (pushbutton) 26
Turns scope on and off.
2
INTENS (knob) 26
Intensity for trace- and readout brightness, focus and trace
rotation control.
3
FOCUS, TRACE, MENU (pushbutton) 26
Calls the Intensity knob menu to be displayed and enables
the change of different settings using the INTENS knob. See item 2.
4
CURSOR MEASURE (pushbutton) 26
Calls the CURSOR menu and offers measurement selection
and activation.
5
ANALOG/DIGITAL (pushbutton) 27
Switches between analog (green) and digital mode (blue).
6
RUN / STOP (pushbutton) 27 RUN: Signal data acquisition enabled. STOP (constantly lit): Signal data acquisition is stopped STOP (fl ashing): Signal data acquisition is in progress and
will be stopped after being completed.
7
MATH (pushbutton) 28 Calls mathematical function menu if digital mode is present.
8
ACQUIRE (pushbutton) 29 Calls the signal capture and display mode menu in digital
mode.
9
SAVE/RECALL (pushbutton) 30 Offers access to the reference signal (digital mode only) and
the instrument settings memory.
10
SETTINGS (pushbutton) 31 Opens menu for language and miscellaneous function; in
digital mode also signal display mode.
11
AUTOSET (pushbutton) 32 Enables appropriate, signal related, automatic instrument
settings.
12
HELP (pushbutton) 32 Switches help texts regarding controls and menus on/off.
13
POSITION 1 (knob) 32 Controls position of actual present functions
15
: Signal (current, reference or mathematics), Cursor and ZOOM (digital).
14
POSITION 2 (knob) 33
Controls position of actual present functions
15
: Signal (current, reference or mathematics) Cursor and ZOOM (digital).
15
CH1/2-CURSOR-MA/REF-ZOOM (pushbutton) 34
Calls the menu and indicates the current function of POSI-
TION 1 and 2 controls.
16
VOLTS/DIV-SCALE-VAR (knob) 34
Channel 1 Y defl ection coeffi cient, Y variabel and Y scaling setting.
17
VOLTS/DIV-SCALE-VAR (knob) 34
Channel 2 Y defl ection coeffi cient, Y variabel and Y scaling
setting.
18
AUTO MEASURE (pushbutton) 35
Calls menus and submenus for automatic measurement.
19
LEVEL A/B – FFT-Marker (knob) 36
Trigger level control for A- and B Time Base. Marker position
shift in FFT mode.
20
MODE (pushbutton) 36
Calls selectable trigger modes.
21
FILTER (pushbutton) 37
Calls menu for trigger fi lter (coupling), noise reject and slope
selection.
22
SOURCE (pushbutton) 38
Calls trigger source menu (e.g. CH1, CH2, Alt. 1/2, External,
AC Line).
23
TRIG’d (LED) 38
Lit when the trigger signal meets the trigger conditions.
24
NORM (LED) 38
Lit if normal or single event triggering is chosen.
25
HOLD OFF (LED) 38
Lit if a hold off time is set (only in analog mode) > 0% in the
HOR menu (HOR VAR pushbutton
30
).
26
X-POS / DELAY (pushbutton) 38
Calls and indicates (colour) the actual function of the HO-
RIZONTAL knob
27
, (X-POS = dark).
27
HORIZONTAL (knob) 39
Changes the X position or in digital mode, the delay time
(Pre- or Post-Trigger).
In FFT mode for center frequency control.
28
TIME/DIV-SCALE-VAR (knob) 39
Setting of A and B time base (defl ection coeffi cient), time
fi ne control (VAR; only in analog mode) and scaling; Span in FFT mode.
29
MAG x10 (pushbutton) 40
10 fold expansion in X direction in analog Yt mode, with
simultaneous change of the defl ection coeffi cient display in the readout.
30
HOR / VAR (pushbutton) 41
Calls ZOOM function (digital); in analog mode time base A
and B, time base variable and hold off control.
31
CH1 / VAR (pushbutton) 42
Calls channel 1 menu with input coupling (AC, DC, 50 Ohm,
GND), inverting, probe, signal input offset and Y variable control.
32
VERT/XY (pushbutton) 43
Calls vertical mode selection, addition, XY mode and band-
width limiter.
33
CH2 / VAR (pushbutton) 44
Calls channel 1 menu with input coupling (AC, DC, 50 Ohm,
GND), inverting, probe, signal input offset and Y variable control.
The fi gures indicate the page for complete discription
in the chapter CONTROLS AND READOUT
Subject to change without notice
Front Panel Elements – Brief Description
34
INPUT CH1 (BNC-socket) 45
Channel 1 signal input and input for horizontal defl ection in
XY mode.
35
INPUT CH2 (BNC-socket) 45
Channel 2 signal input and input for vertical deflection in XY
mode.
36
LC/AUX (pushbutton) 45
Digital mode: Logic signal channels LC0 to LC3 activa-
tion/deactivation and threshold setting. Analog mode: If external triggering is not chosen, activation/deactivation of AUXILIARY INPUT
38
for intensity modulation (Z) and input
coupling selection.
37
FFT (pushbutton) 46
Calls FFT menu, offers window and scaling selection, as
well as function switch off.
Calls FFT menu if FFT mode is present. Direct switch over
from digital Yt mode to FFT mode.
38
AUXILIARY INPUT (BNC socket) 46 Digital mode: Input for external trigger signals. Analog mode: Input for intensity modulation (Z) or external
trigger signals.
39
LC0 ... LC3 LOGIC PROBE (multi pin connector) 47
Digital mode: In connection with Option HO2010 input for
logic signals.
40
PROBE / ADJ (socket) 47
Square wave signal output for frequency compensation of
x10 probes.
41
PROBE / ADJ (pushbutton) 47
Calls menu that offers COMPONENT Tester operation, fre-
quency selection of PROBE ADJ square wave signal, hard­ware and software information and details about interface (rear side) and USB Stick (fl ash drive) connector.
42
COMPONENT TESTER (2 sockets with 4 mm Ø) 47
Connectors for test leads of the Component Tester. Left
socket is galvanically connected with protective earth.
43
USB Stick (USB fl ash drive connector; front side) 47
Enables storage and load of signals and signal parameters
in connection with USB fl ash drives.
44
MENU OFF (pushbutton) 47
Switches the menu display off or one step back in the menu
hierarchy.
FFT­Marker
VAR VAR VA R x10
VOLTS / DIV
SCALE · VAR
VOLTS / DIV
SCALE · VAR
TIME / DIV
SCALE · VAR
AUTO
MEASURE
5 V 1 mV 5 V 1 mV
X-POS
AUXILIARY INPUTLC0 ... LC
3
LOGIC PROBE
Use recommended
probe only!
TRIG. EXT. / Z-INP.
INTENS
!
LEVEL A/B
HM2008
2 GSa · 2 MB
200 MHz
50s 2ns
LC/AUX
FFT
1MΩ II
15pF
max
100 Vp
HORIZONTAL
INPUTS
1MΩII15pF
max
250 Vp
DIGITAL
ANALOG
DELAY
CH 1/2
CURSOR
X-INP
FOCUS TRACE
MENU
CURSOR
MEASURE
MA/REF
ZOOM
MATH
SAVE/
RECALL
AUTOS ET
RUN / STOP ACQUIRE SETTINGS HELP
MODE
FILTER
SOURCE
TRIG ’d
NORM
HOLD OFF
TRIGGER
POSITION 1 POSITION 2
CH 1
VERT/XY
CH 2 HOR MAG
CAT I
!
50Ω 5V RMS 50Ω 5V RMS
CH 1 CH 2
!
ANALOG
DIGITAL
MIXED SIGNAL
OSCILLOSCOPE
POWER
POWER
MENU
MENU
OFF
OFF
1 2 3 4 5 76
10
8
12911
19
26
27
23
24
25
29
30
38
22
20
21
28
373936353332343144
13
15
14
17
16
18
COMBISCOPE
USB
Stick
COMP.
TESTER
PROBE
ADJ
POWER
MENUMENU
OFFOFF
4440414243
10
Subject to change without notice
Basic signal measurement
Signals which can be measured
The following description pertains to analog and digital ope­ration. The different specifications in both operating modes should be kept in mind.
The oscilloscope HM2008 can display all repetitive signals with a fundamental repetition frequency of at least 200 MHz. The frequency response is 0 to 200 MHz (–3 dB). The vertical amplifi ers will not distort signals by overshoots, undershoots, ringing etc.
Simple electrical signals like sine waves from line frequency ripple to hf will be displayed without problems. However, when measuring sine waves, the amplitudes will be displayed with an error increasing with frequency. At 120 MHz the amplitude error will be around –10 %. As the bandwidths of individual instruments will show a certain spread (the 200 MHz are a guaranteed minimum) the actual measurement error for sine waves cannot be exactly determined.
Pulse signals contain harmonics of their fundamental fre­quency which must be represented, so the maximum useful repetition frequency of nonsinusoidal signals is much lower than 200 MHz (5 to 10 times). The criterion is the relationship between the rise times of the signal and the scope; the scope’s rise time should be <1/3 of the signal’s rise time if a faithful reproduction without too much rounding of the signal shape is to be preserved.
The display of a mixture of signals is especially diffi cult if it con­tains no single frequency with a higher amplitude than those of the other ones as the scope’s trigger system normally reacts to a certain amplitude. This is e.g. typical of burst signals. Display of such signals may require using the HOLD-OFF control.
Composite video signals may be displayed easily as the instru­ment has a TV SYNC separator.
The maximum sweep speed of 2 ns/cm allows suffi cient time resolution, e.g. a 200 MHz sine wave will be displayed one period per 2.5 cm. The vertical amplifi er inputs may be DC or AC coupled. Use DC coupling only if necessary and preferably with a probe.
Low frequency signals when AC coupled will show tilt (AC low frequency – 3 dB point is 1.6 Hz), so if possible use DC coupling. Using a probe with 10:1 or higher attenuation will lower the –3 dB point by the probe factor. If a probe cannot be used due to the loss of sensitivity DC coupling the scope and an external large capacitor may help which, of course, must have a suffi cient DC rating. Care must be taken, however, when charging and discharging a large capacitor.
DC coupling is preferable with all signals of varying duty cycle, otherwise the display will move up and down depending on the duty cycle. Of course, pure DC can only be measured with DC coupling. The readout will show which coupling was chosen: = stands for DC, ~ stands for AC. For hf measurement an internal 50 Ω terminator can be activated which is indicated by an Ω-symbol in the readout.
Amplitude of signals
In contrast to the general use of rms values in electrical engi­neering oscilloscopes are calibrated in Vpp as that is what is displayed.
Derive rms from V
pp
: divide by 2.84. Derive Vpp from rms: mul-
tiply by 2.84.
Values of a sine wave signal
V
rms
= rms value
V
pp
= pp – value
V
mom
= momentary value, depends on time vs. period.
The minimum signal for a one cm display is 1 mV
pp
±5 % provi­ded 1 mV/cm was selected and the variable is in the calibrated position.
The available sensitivities are given in mV
pp
or Vpp. The cursors allow to indicate the amplitudes of the signals immediately on the readout as the attenuation of probes is automatically taken into account. Even if the probe attenuation was selected manu­ally this will be overridden if the scope identifi es a probe with an identifi cation contact as different. The readout will always give the true amplitude.
It is important that the variable be in its calibrated position. The sensitivity may be continuously decreased by using the variable (see Controls and Readout). Each intermediate value between the calibrated positions 1–2–5 may be selected. Without using a probe thus a maximum of 100 V
PP
may be displayed (20 V/div
x 8 cm screen x 2.5 variable).
Amplitudes may be directly read off the screen by measuring the height and multiplying by the V/div. setting.
Please note: Without a probe the maximum permis-
sible voltage at the inputs must not exceed 250 Vp irrespective of polarity.
In case of signals with a DC content the peak value DC + AC peak must not exceed + or –250 V
p
. Pure AC of up to 500 Vpp is
permissible.
If probes are used their possibly higher ratings are
only usable if the scope is DC coupled.
In case of measuring DC with a probe while the scope input is AC coupled the capacitor in the scope input will see the input DC voltage as it is in series with the internal 1 MΩ resistor. This means that the maximum DC voltage (or DC + peak AC) is that of the scope input, i.e. 250 V
P
! With signals which contain DC and AC the DC content will stress the input capacitor while the AC content will be divided depending on the AC impedance
Basic signal measurement
V
p
V
rms
V
mom
V
pp
11
Subject to change without notice
of the capacitor. It may be assumed that this is negligible for frequencies >40 Hz.
Considering the foregoing you may measure DC signals of up to 600 V or pure AC signals of up to 1200 V
PP
with a HZ200 probe. Probes with higher attenuation like HZ53 100:1 allow to measure DC up to 1200 V and pure AC of up to 2400 V
PP
. (Please note the derating for higher frequencies, consult the HZ53 manual). Stressing a 10:1 probe beyond its ratings will risk destruction of the capacitor bridging the input resistor with possible ensuing damage of the scope input!
In case the residual ripple of a high voltage is to be measured a high voltage capacitor may be inserted in front of a 10:1 probe, it will take most of the voltage as the value of the probe’s internal capacitor is very low, 22 to 68 nF will be suffi cient.
If the input selector is switched to Ground the reference trace on the screen may be positioned at graticule center or else­where.
DC and AC components of an input signal
The dashed curve shows an AC signal symmetrical to zero. If there is a DC component the peak value will be DC + AC peak.
Timing relationships
In most cases repetitive signals must be measured. The repe­tition frequency of a signal is equal to the number of periods per second. Depending on the TIME/DIV setting one or more periods or part of a period of the signal may be displayed. The time base settings will be indicated on the readout in s/cm, ms/cm, μs/cm and ns/cm (1 cm is the equivalent of 1 div. on the crt graticule). Also the cursors may be used to measure the frequency or the period.
Without cursor the cycle duration can be determined by multi­plying the length (cm) with the (calibrated) time coeffi cient. The reciprocal value is the frequency.
If portions of the signal are to be measured use delayed sweep (analog mode) or zoom (digital mode) or the magnifi er x 10. Use the HORIZONTAL positioning control to shift the portion to be zoomed into the screen center.
Pulse signals are characterized by their rise and fall times which are measured between the 10 % and 90 % portions. The following example uses the internal graticule of the crt, but also the cursors may be used for measurement.
Measurement:
– Adjust the rising portion of the signal to 5 cm.
– Position the rising portion symmetrically to the graticule
centre line, using both Y and X positioning controls.
– Notice the intersections of the signal with the 10 and 90 %
lines and project these points to the centre line in order to read the time difference.
In the example it was 1.6 cm at 5 ns/cm equals 8 ns rise time.
When measuring very short rise times coming close to the scope rise time it is necessary to subtract the scope’s (and if used the probe’s) rise times geometrically from the rise time as seen on the screen. The true signal rise time will become:
t
tot
is the rise time seen, t
osc
is the scope’s own rise time (1.75
ns with the HM2008), t
t
is the rise time of the probe, e.g. 2 ns. If the signal’s rise time is >22 ns, the rise times of scope and probe may be neglected.
For the measurement of rise times it is not necessary to proceed as outlined above. Rise times may be measured anywhere on the screen. It is mandatory that the rising portion of the signal be measured in full and that the 10 to 90 % are observed. In case of signals with over- or undershoot the 0 and 100 % levels are those of the horizontal portions of the signal, i.e. the over­resp. undershoots must be disregarded for rise and fall time measurements. Also, glitches will be disregarded. If signals are very distorted, however, rise and fall time measurements may be of no value.
For most amplifi ers, even if their pulse behaviour is far from ideal, the following relationship holds:
350 350 t
a
=
——
B =
——
B t
a
tr/ns = 350/Bandwidth/MHz
Connection of signals
In most cases pressing the AUTOSET button will yield a satisf­actory display (see AUTOSET). The following relates to special cases where manual settings will be advisable. For a description of controls refer to ”Controls and Readout“.
Take care when connecting unknown signals to the
inputs!
It is recommended to use probes whenever possible. Without a probe start with the attenuator set to its 20 V/cm position. If the trace disappears the signal amplitude may be too large overdriving the vertical amplifi er or/and its DC content may be too high. Reduce the sensitivity until the trace will reappear
Basic signal measurement
ta= 82 - 2.32 - 22 = 7,5 ns
ta= t
tot
2
– t
osc
2
– t
t
2
voltage
peak
AC
DC
DC
AC
DC + AC
peak
= 400 V
max
5 cm
t
tot
100%
90%
10%
0%
12
Subject to change without notice
onscreen. If calibrated measurements are desired it will be necessary to use a probe if the signal becomes >40 V
pp
. Check the probe specifi cations in order to avoid overstressing. If the time base is set too fast the trace may become invisible, then reduce the time base speed.
If no probe is used at least screened cable should be used, such as HZ32 or HZ34. However, this is only advisable for low impedance sources or low frequencies (<50 kHz). With high frequencies impedance matching will be necessary.
Non sinusoidal signals particularly require impedance matching, preferably at both ends. At the scope input, a 50 Ω termination is selectable with a maximum load of 0.5 Watt (5 V
rms
, or in case of
sine wave signals, 14.7 V
pp
). If proper terminations are not used, sizeable pulse aberrations will result. Also sine wave signals of >100 kHz should be properly terminated. Most generators control signal amplitudes only if correctly terminated. For higher loads (up to 1 Watt; 7 V
rms
or 20 Vpp) HAMEG offers
the external 50 Ω termination HZ22.
For probes terminations are neither required nor allowed, they would ruin the signal.
Probes feature very low loads at fairly low frequencies: 10 MΩ in parallel to a few pF, valid up to several hundred kHz. How­ever, the input impedance diminishes with rising frequency to quite low values. This has to be borne in mind as probes are, e.g., entirely unsuitable to measure signals across high impe­dance high frequency circuits such as bandfi lters etc.! Here only FET probes can be used. Use of a probe as a rule will also protect the scope input due to the high probe series resistance (9 MΩ). As probes cannot be calibrated exactly enough during manufacturing individual calibration with the scope input used is mandatory! (See Probe Calibration).
Passive probes will, as a rule, decrease the scope bandwidth resp. increase the rise time. We recommend to use HZ200 pro­bes in order to make maximum use of the combined bandwidth. HZ200 features 2 additional hf compensation adjustments.
Whenever the DC content is > 250 V
DC
coupling must be used in order to prevent overstressing the scope input capacitor. This is especially important if a 100:1 probe is used as this is specifi ed for 1200 V
DC
+ peak AC.
AC coupling of low frequency signals may produce tilt.
If the DC content of a signal must be blocked it is possible to insert a capacitor of proper size and voltage rating in front of the probe, a typical application would be a ripple measurement.
When measuring small voltages the selection of the ground connection is of vital importance. It should be as close to voltage take-off point as possible, otherwise ground currents may de­teriorate the measurement. The ground connections of probes are especially critical, they should be as short as possible and of large size.
If a probe is to be connected to a BNC connector use
a probe tip to BNC adapter.
If ripple or other interference is visible, especially at high sen­sitivity, one possible reason may be multiple grounding. The scope itself and most other equipment are connected to safety ground, so ground loops may exist. Also, most instruments will have capacitors between line and safety ground installed which conduct current from the live wire into the safety ground.
First time operation and initial adjustments
Prior to fi rst time operation the connection between the instru­ment and safety ground must be ensured, hence the plug must be inserted fi rst.
Use the red pushbutton POWER to turn the scope on. Several displays will light up. The scope will then assume the set-up, which was selected before it was turned off. If no trace and no readout are visible after approximately 20 sec, push the AUTOSET button.
As soon as the trace becomes visible select an average inten­sity with INTENS, then select FOCUS and adjust it, then select TRACE ROTATION and adjust for a horizontal trace.
With respect to crt life use only as much intensity as necessary and convenient under given ambient light conditions, if unused turn the intensity fully off rather than turning the scope off and on too much, this is detrimental to the life of the crt heater. Do not allow a stationary point to stay, it might burn the crt phosphor.
With unknown signals start with the lowest sensitivity 5 V/cm, connect the input cables to the scope and then to the measu­ring object which should be deenergized in the beginning. Then turn the measuring object on. If the trace disappears, push AUTOSET.
Trace rotation TR
The crt has an internal graticule. In order to adjust the defl ected beam with respect to this graticule the Trace Rotation control is provided. Select the function Trace Rotation and adjust for a trace which is exactly parallel to the graticule.
Probe adjustment and use
In order to ensure proper matching of the probe used to the scope input impedance the scope contains a calibrator with short rise time and an amplitude of 0.2 Vpp ± 1 %, equivalent to 4 cm at 5 mV/cm when using 10:1 probes.
The inner diameter of the calibrator connector is 4.9 mm and standardized for series F probes. Using this special connec­tor is the only way to connect a probe to a fast signal source minimizing signal and ground lead lengths and to ensure true displays of pulse signals.
1 kHz – adjustment
This basic adjustment will ensure that the capacitive at­tenuation equals the resistive attenuation thus rendering the attenuation of the probe independent of frequency. 1:1 probes can not be adjusted and need no such adjustment anyway.
First time operation and initial adjustments
incorrect correct incorrect
13
Subject to change without notice
Operating modes of the vertical amplifi er
The controls most important for the vertical amplifi er are: VERT/ XY
32
, CH 1 31, CH 2 33 – and in digital mode also – LC/AUX 36. They give access to the menus containing the operating modes and the parameters of the individual channels.
Changing the operating mode is described in the chapter: ”Controls and Readout“.
Remark: Any reference to ”both channels“ always refers to channels 1 and 2.
Usually oscilloscopes are used in the Yt mode. In analog mode the amplitude of the measuring signal will defl ect the trace vertically while a time base will defl ect it from left to right.
The vertical amplifi ers offer these modes: – One signal only with CH1. – One signal only with CH2.
− Two signals with channels 1 and 2 (DUAL trace mode).
− Two signals displayed as one in addition (ADD) mode.
In digital mode the Option HO2010 additionally enables the logic state display of 4 logic channels (LC0 ... LC3).
In DUAL mode both channels are operative. In analog mode the method of signal display is governed by the time base (see also ”Controls and Readout“). Channel switching may either take place after each sweep (alternate) or during sweeps with a high frequency (chopped).
The normal choice is alternate, however, at slow time base set­tings the channel switching will become visible and disturbing, when this occurs select the chopped mode in order to achieve a stable quiet display.
In digital mode no channel switching is necessary as each input has its own A/D converter, signal acquisition is simultaneous.
In ADD mode the two channels 1 and 2 are algebraically ad­ded (±CH1 ±CH2). With + polarity the channel is normal, with – polarity inverted. If + Ch1 and – CH2 are selected the difference will be displayed or vice versa.
Same polarity input signals:
Both channels not inverted: = sum Both channels inverted: = sum Only one channel inverted: = difference
Opposite polarity input signals:
Both channels not inverted: = difference Both channels inverted: = difference One channel inverted: = sum.
Please note that in ADD mode both position controls will be operative. The INVERT function will not affect positioning.
Often the difference of two signals is to be measured at signal take-offs which are both at a high common mode potential. While this one typical application of the difference mode one important precaution has to be borne in mind: The oscillosco­pe vertical amplifi ers are two separate amplifi ers and do not constitute a true difference amplifi er with as well a high CM rejection as a high permissible CM range! Therefore please observe the following rule: Always look at the two signals in the one channel only or the dual modes and make sure that
Prior to adjustment make sure that the trace rotation adjust­ment was performed.
Connect the 10:1 probe to the input. Use DC coupling. Set the VOLTS/DIV knob for a signal display height of 4 cm and TIME/ DIV to 0.2 ms/cm, both calibrated. Insert the probe tip into the calibrator connector PROBE ADJ.
You should see 2 signal periods. Adjust the compensation ca­pacitor (see the probe manual for the location) until the square wave tops are exactly parallel to the graticule lines (see picture 1 kHz). The signal height should be 4 cm ±1.6 mm (3% oscillo­scope and 1% probe tolerance). The rising and falling portions of the square wave will be invisible.
1 MHz adjustment
The HAMEG probes feature additional adjustments in the compensation box which allow to optimise their hf behaviour. This adjustment is a precondition for achieving the maximum bandwidth with probe and a minimum of pulse aberrations.
This adjustment requires a calibrator with a short rise time (typ. 4 ns) and a 50 Ω output, a frequency of 1 MHz, an amplitude of 0.2 V
pp
. The PROBE ADJ. output of the scope fulfi ls these
requirements.
Connect the probe to the scope input to which it is to be adjusted. Select the PROBE ADJ. signal 1 MHz. Select DC coupling and 5 mV/cm with VOLTS/DIV. and 0.1 μs/cm with TIME/DIV., both calibrated. Insert the probe tip into the calibrator output connec­tor. The screen should show the signal, rise and fall times will be visible. Watch the rising portion and the top left pulse corner, consult the manual for the location of the adjustments.
The criteria for a correct adjustment are:
– short rise time, steep slope.
– clean top left corner with minimum over- or undershoot,
fl at top.
After adjustment check the amplitude which should be the same as with 1 kHz.
It is important to fi rst adjust 1 kHz, then 1 MHz. It may be ne­cessary to check the 1 kHz adjustment again.
Please note that the calibrator signals are not calibrated with respect to frequency and thus must not be used to check the time base accuracy, also their duty cycle may differ from 1:1.The probe adjustment is completed if the pulse tops are horizontal and the amplitude calibration is correct.
Operating modes of the vertical amplifier
incorrect correct incorrect
14
Subject to change without notice
they are within the permissible input signal range; this is the case if they can be displayed in these modes. Only then switch to ADD. If this precaution is disregarded grossly false displays may result as the input range of one or both amplifi ers may be exceeded. Another precondition for obtaining true displays is the use of two identical probes at both inputs. But note that normal probe tolerances (percent) will cause the CM rejection to be expected to be rather moderate. In order to obtain the best possible re­sults proceed as follows: First adjust both probes as carefully as possible, then select the same sensitivity at both inputs and then connect both probes to the output of a pulse generator with suffi cient amplitude to yield a good display. Readjust one (!) of the probe adjustment capacitors for a minimum of over­or undershoot. As there is no adjustment provided with which the resistors can be matched a residual pulse signal will be unavoidable. When making difference measurements it is good practice to fi rst connect the ground cables of the probes to the object prior to connecting the probe tips. There may be high potentials between the object and the scope. If a probe tip is connected fi rst there is danger of overstressing the probe or/and the scope inputs! Never perform difference measurements without both probe ground cables connected.
XY operation
This mode is accessed by VERT/XY 32 > XY. In analog mode the time base will be turned off. The channel 1 signal will defl ect in X direction (X-INP. = horizontal input), hence the input attenuators, the variable and the POSITION 1 control will be operative. The HORIZONTAL control will also remain functional.
Channel 2 will defl ect in Y direction.
The x10 magnifi er will be inoperative in XY mode. Please note the differences in the Y and X bandwidths, the X amplifi er has a lower –3 dB frequency than the Y amplifi er. Consequently the phase difference between X and Y will increase with frequency.
In XY mode the X signal (CH1 = X-INP). can not be inverted.
The XY mode may generate Lissajous fi gures which simplify some measuring tasks and make others possible:
– Comparison of two signals of different frequency or adjust-
ment of one frequency until it is equal to the other resp. becomes synchronized.
– This is also possible for multiples or fractions of one of the
frequencies.
Phase measurements with Lissajous fi gures
The following pictures show two sine waves of equal amplitude and frequency but differing phase.
0° 35° 90° 180°
ab
Calculation of the phase angle between the X- and Y-signals (af­ter reading a and b off the screen) is possible using the following formulas and a pocket calculator with trigonometric functions. This calculation is independent of the signal amplitudes:
Please note:
– As the trigonometric functions are periodic limit the calcu-
lation to angles <90 degrees. This is where this function is most useful.
– Do not use too high frequencies,
because, as explained above, the two amplifiers are not identical, their phase difference increases with frequency. The spec gives the frequency at which the phase diffe­rence will stay <3 degrees.
– The display will not show which of the two frequencies does
lead or lag. Use a CR combination in front of the input of the frequency tested. As the input has a 1 MΩ resistor it will be suffi cient to insert a suitable capacitor in series. If the ellipse increases with the C compared to the C short-circuited the test signal will lead and vice versa. This is only valid <90 degrees. Hence C should be large and just create a barely visible change.
If in XY mode one or both signals disappear, only a line or a point will appear, mostly very bright. In case of only a point there is danger of phosphor burn, so turn the intensity down immedia­tely; if only a line is shown the danger of burn will increase the shorter the line is. Phosphor burn is permanent.
Measurement of phase differences in dual channel Yt mode
Please note: Do not use ”alternate trigger“ because the time differences shown are arbitrary and depend only on the respec­tive signal shapes! Make it a rule to use alternate trigger only in rare special cases. The best method of measuring time or phase differences is using the dual channel Yt mode. Of course, only times may be read off the screen, the phase must then be calculated as the frequency is known. This is a much more accurate and convenient method as the full bandwidth of the scope is used, and both amplifi ers are almost identical. Trigger the time base from the signal which shall be the reference. It is necessary to position both traces without signal exactly on the graticule center (POSITION 1 and 2). The variables and trigger level controls may be used, this will not infl uence the time difference measurement. For best accuracy display only one period at high amplitude und observe the zero crossings. One period equals 360 degrees. It may be advantageous to use AC coupling if there is an offset in the signals.
In this example t = 3 cm and T = 10 cm, the phase difference in degrees will result from:
5 3 ϕ° =
· 360° = — · 360° = 108°
T 10
or in angular units:
t 3 arc ϕ° =
· 2π = — · 2π = 1,885 rad
T 10
Operating modes of the vertical amplifier
t = horizontal spacing of the zero
transitions in div
T= horizontal spacing for one
period in div
a sin ϕ =
b
a cos ϕ = 1 –
(—)
2
b
a ϕ = arc sin
b
15
Subject to change without notice
Very small phase differences with moderately high frequencies may yield better results with Lissajous fi gures.
However, in order to get higher precision it is possible to switch to higher sensitivities – after accurately positioning at graticule centre – thus overdriving the inputs resulting in sharper zero crossings. Also, it is possible to use half a period over the full 10 cm. As the time base is quite accurate increasing the time base speed after adjusting for e.g. one period = 10 cm and positioning the fi rst crossing on the fi rst graticule line will also give better resolution.
Measurement of amplitude modulation
Please note: Use this only in analog mode because in digital mode alias displays may void the measurement! For the display of low modulation frequencies a slow time base (TIME/DIV) has to be selected in order to display one full period of the modu­lating signal. As the sampling frequency of any digital must be reduced at slow time bases it may become too low for a true representation.
The momentary amplitude at time t of a hf carrier frequency modulated by a sinusoidal low frequency is given by:
u = UT · sinΩt + 0,5 m · UT · cos (Ω - ω) t - 0,5 m · UT · cos (Ω - ω) t
where: UT = amplitude of the unmodulated carrier Ω = 2πF = angular carrier frequency ω = 2πf = modulation angular frequency m = modulation degree (1
v100%)
In addition to the carrier a lower side band F – f and an upper side band F + f will be generated by the modulation.
Picture 1: Amplitudes and frequencies with AM (m = 50 %) of the spectra
As long as the frequencies involved remain within the scope’s bandwidth the amplitude-modulated hf can be displayed. Pre­ferably the time base is adjusted so that several signal periods will be displayed. Triggering is best done from the modulation frequency. Sometimes a stable displayed can be achieved by twiddling with the time base variable.
Picture 2: Amplitude modulated hf. F = 1 MHz, f = 1 kHz, m = 50 %, U
T
= 28,3 mV
rms
Set the scope controls as follows in order to display the picture 2 signal:
CH1 only, 20 mV/cm, AC TIME/DIV: 0.2 ms/cm Triggering: NORMAL, AC, internal. Use the time base variable or external triggering.
Reading a and b off the screen the modulation degree will result:
a – b a – b m =
——
bzw. m =
—— · 100 [%]
a + b a + b
a = U
T
(1 + m) and b = UT (1 – m)
When measuring the modulation degree the amplitude and time variables can be used without any infl uence on the result.
Triggering and time base
The most important controls and displays for these functions are to be found in the shaded TRIGGER area, they are described in „Controls and Readout“.-
In YT mode the signal will defl ect the trace vertically while the time will defl ect it horizontally, the speed can be selected. In general periodic voltage signals are displayed with a peri­odically repeating time base. In order to have a stable display successive periods must trigger the time base at exactly the same time position of the signal (amplitude and slope).
Pure DC can not trigger the time base, a voltage
change is necessary.
Triggering may be internal from any of the input signals or externally from a time-related signal.
For triggering a minimum signal amplitude is required which can be determined with a sine wave signal. With internal trigge­ring the trigger take-off within the vertical amplifi ers is directly following the attenuators. The minimum amplitude is specifi ed in mm on the screen. Thus it is not necessary to give a minimum voltage for each setting of the attenuator.
For external triggering the appropriate input connector is used, the amplitude necessary there is given in V
pp
. The voltage for triggering may be much higher than the minimum, however, it should be limited to 20 times the minimum. Please note that for good triggering the voltage resp. signal height should be a good deal above the minimum. The scope features two trigger modes to be described in the following:
Automatic peak triggering (MODE menu)
Consult the chapters MODE 20 > AUTO, LEVEL A/B 19, FILTER
21
and SOURCE 22 in ”Controls and Readout“. Using AUTOSET this trigger mode will be automatically selected. With DC coup­ling and with alternate trigger this mode will be left while the automatic triggering will remain.
Automatic triggering causes a new time base start after the end of the foregoing and after the hold-off time has elapsed even
Triggering and time base
F – f F F + f
0,5 m · U
T
0,5 m · U
T
U
T
ba
m · U
T
U
T
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