THE SERVICING INSTRUCTIONS CONTAINED IN THIS MANUAL ARE FOR
USE BY QUALIFIED PERSONNEL ONLY. TO AVOID ELECTRIC SHOCK, DO
NOT PERFORM ANY SERVICING OTHER THAN THAT CONTAINED IN THE
OPERATING INSTRUCTIONS UNLESS YOU ARE QUALIFIED TO DO SO.
2-3-1 Signal Connections ................................................................................................................................... 9
2-4-3 Time Interval Measurements ....................................................................................................................23
2-4-6 Frequency Measurements .........................................................................................................................27
The LBO-516, shown in Figure 1-1, is a 100 MHz oscilloscope
with all of the features normally found on a lab-grade scope: highfidelity pulse response, stable operation, dual timebase with
calibrated sweep delay, flexible triggering facilities, and a bright
CRT display with illuminated internal graticule. Moreover, it also has
a very unusual feature found on few scopes in any price class: it can
simultaneously display up to eight traces from three different input
signals! In addition to the two vertical-input channels and their difference signal, the signal used to externally trigger the main timebase
can also appear on the CRT display. The alternate sweep mode,
which allows the main and delayed timebases to simultaneously
sweep the CRT, effectively doubles this four-trace display to an
eight-trace display.
The comprehensive triggering facilities of the LBO-516 include
several features that ease the problem of triggering on complex
signals: a variety of frequency-selective coupling filters, a trigger
holdoff-control, and a trigger pickoff that alternates between the two
vertical channels.
1-2. SPECIFICATIONS
Specifications for the model LBO-516 oscilloscope are given in
Table 1-1.
Table 1-1
SPECIFICATIONS
Vertical Amplifiers (Ch. 1 & 2)
Bandwidth (-3 dB)
DC coupled DC - 100 MHz
AC coupled 10 Hz - 100 MHz
Rise Time 3.5 KS
Deflection Coefficients
Accuracy 5 mV/div to 5 V/div in 10 calibrated
steps, 1-2-5 sequence. Continuously
variable between steps. XI0
magnification adds 0.5, 1, and 2
mV/div steps for frequencies below 5
MHz
Input Impedance -+3%; -+5% with Xl0magniflca-tion
1 megohm +-2%, 25 pF +-3 pF
Maximum Input Voltage 400 V (DC plus AC peak)
1
Page 5
Signal Delay Leading edge displayed.
Leading edge displayed. CH-1 only, CH-2 only,
Common Mode Rejection 20dB at 20MHz
CH- 1 Output 25 mV/div into 50 ohms
Horizontal Amplifier (X-Y Mode)
Bandwidth (- 3 dB)
DC coupled DC - 3 MHz
AC coupled 10Hz - 3MHz
Rise Time 120 KS
Phase Shift <3° at 100 kHz
Deflection Coefficients 0.5 mV/div to 5 V/div in 13 calibrated
steps, 1-2-5 sequence, continuously
variable between steps
Accuracy +-3% for 5 mV/div to 5 V/div,
+-5% for 0.5 mV/div to 2 mV/div
Input Impedance 1 megohm -+2%, 25 pF +-3 pF
Maximum Input Voltage 400 V (DC plus AC peak)
Time-Base Generators
Display Modes Main timebase (TB) only,
Main TB intensified by delayed
TB,
Delayed timebase,
Main TB alternated with
delayed TB.
Main (A) Time Base 0.02 KS/div to 0.5 S/div in 23
calibrated steps, 1-2-5 sequence.
Continuously variable between steps.
Delayed (B) Time Base 0.2 PS/div to 50 mS/div in 20
calibrated steps, 1-2-5 sequence.
Magnifier XI0 deflection increase at any TB
setting extends sweep speeds of main
and delayed TB's to 2 KS/div.
Accuracy +- 3% unmagnified
+- 5% magnified
Delay Time Continuously variable multiplier with
1000 divisions.
Delayed TB Jitter 1/20,000
Trigger Circuits
Sources CH-l, CH-2, Alternate, Line, External
Modes Auto, Normal, Single-shot
Coupling AC, DC, HF reject, TV vertical, TV
horizontal
Slope + orHoldoff Normal, Variable (to greater than
one sweep), B ends A
Sensitivity
Internal Trigger DC – 10 MHz: 0.4div
External Trigger DC - 10MHz: 100mV
External Trigger Amplifier (Ch. 3)
Bandwidth (-3 dB)
DC coupled DC - 100 MHz
AC coupled 10Hz- l00 MHz
Rise Time 3.5 KS
Deflection Coefficients 0.2 V/div and 2 V/div
Accuracy +-3%
Input Impedance 1 megohm +-2%, 30 pF
Maximum Input Voltage 400 V (DC plus AC peak)
Z-Axis Modulation
Level for Blanking Standard TTL high (+ 2 to + 5V)
Coupling DC
Maximum Input Voltage 50 Vp-p
Input Impedance 10k:
Bandwidth DC-5 MHz
Calibrator
Output Voltage 500 m Vp-p--+ 2%, positive-going,
Frequency 1 kHz nominal
Waveform Fast-rise rectangular wave
CRT Display
Phosphor P31 (P39 optional)
Accelerating Potential 20 kV/2kV
Graticule Internal 1 cm square divisions, 8 div
Graticule Illumination Continuously variable
Trace Adjustments on Rotation, focus, intensity,
Front Panel B intensity
Other Features
"Out-of-Calibration"
Indicator
Other Indicators Main timebase triggered
Power Requirements
Line Voltage 100/120/200 VAC 220/240 VAC
Line Frequency 50-60 Hz
Power Consumption 55W
Physical & Environmental Data
Case Size (WxHxD) 12.3 x 5.8 x 16 inches
305 x 145 x 400 mm
Overall Size (WxHxD), 13.75 x 7.25 x 18.5 inches
handle folded back 350 x 185 x 470 mm
10 - 100 MHz: 1.5 divs
10 - 100 MHz: 400mV
ground referenced
high, 10 div wide.
Central axis subdivided into 0.2 cm
graduations.
Main timebase
Single-shot ready
Power on
2
Page 6
S
1
2
3456789
Weight 20.9 lbs, 9.5 kg
Ambient Operating 0-40°C (32-104°F) maximum
Temperature 15-35°C (60-95°F) for guaranteed
specs
Vibration Tolerance 2 mmp-p displacement at 12-33 Hz
and 33-35 Hz
Shock Tolerance 30g
Accessories
Supplied Instruction Manual
Two (2) LP- 100X probes
Two (2) BNC-to-post adaptors
Optional LP-2017 Probe Pouch
LC-2016 Protective Front Cover
LR-2402 Rack Mount Adaptor
LH-2015 Hood
Specifications for the model LP-100X scope probe are given in
Table 1-2.
2. OPERATING INSTRUCTION
This section contains the information needed to operate the
LBO-516 and utilize it in a variety of basic and advanced
measurement procedures. Included are the identification and function
of controls, connectors, and indicators, initial startup procedures,
basic operating routines, and selected measurement applications.
2-1. FUNCTION OF CONTROLS, CONNECTORS, AND
INDICATORS
Before turning on
controls, connectors, indicators, and other features described in this
section. The descriptions given below are keyed to the items called
out in Figures 2-1 to 2-4.
2-1-1 Display Block
Refer to Figure 2-1 for reference (1) to (9).
POWER switch Push in to turn instrument power on
POWER lamp Lamp lights when power is on
A INTEN control To adjust the overall brightness of the
B INTEN control Provides adjustment of CRT brightness
FOCUS control To attain maximum trace sharpness.
ROTATION control Provides screwdriver adjustment of
horizontal trace alignment with regard
to the CRT graticule lines
Table 1-2
Attenuation Ratio 10:1 +-2% and 1:1, switch
selectable
Input Impedance
10X attenuation 10 megohms, 12 pF +
1X attenuation Scope input Z plus < 150 pF
Rise Time (10X atten.) 3.5 KS nominal
Overshoot & Ringing <10%
(10X atten.)
Bandwidth
10X attenuation DC- 100MHz
1X attenuation DC - 6 MHz
Maximum Input Voltage 600 V (DC plus AC peak)
Ambient Operating
Temperature
Maximum - 10 to + 55°C
For guaranteed
Specifications +5 to +35°C
Ambient Humidity
Maximum 40 to 90%
For guaranteed
Specifications 45 to 85%
CRT Display device having 1 cm square
ILLUM control To adjust graticule illumination.
Clockwise rotation increases
brightness
CAL connector Provides fast-rise waveform of precise
LP-100X SPECIFICATIONS
10%
graticule lines inscribed on the inner
CRT surface for parallax-free
measurements. Blue filter provides
good contrast and pleasing display.
amplitude for probe adjustment and
vertical amplifier calibration.
3
Page 7
2-1-2 Vertical Amplifier Block
10
11232212
1314
15
161718192021
Refer to Figure 2-2 for references (10) to (12) and (14) to (23).
Refer to Figure 2-3 for reference (13).
VOLTS/DIV switches To select the calibrated deflection
factor of the input signals fed to the
vertical amplifier.
VARIABLEcontrols Provide continuously variable
adjustment of deflection factor between
steps of the VOLTS/DIV switches.
Calibrations are accurate only when the
VARIABLE controls are detented in
PULL X 10 MAG Pulling these out will increase the
(on VARIABLE sensitivity of the associated vertical
controls) amplifiers by ten times at reduced
Ground Connector Provides convenient point to attach
CH-1 OUTPUT Provides scaled output of the channel 1
Connector signal suitable for driving a frequency
CH- 1 or X-IN For applying an input signal to vertical
connector amplifier channel 1, or the X-axis
CH-2 or Y-IN For applying an input signal to vertical
connector amplifier 2, or the Y-axis (vertical)
AC/GND/DC To select the method of coupling the
switches input signals to the vertical amplifiers.
Channel 1 Vertical For vertically positioning trace 1 on the
POSITION control CRT screen. Clockwise rotation moves
Channel 2 Vertical or For vertically positioning trace 2 on the
Y POSITION control CRT screen. Clockwise rotation moves
CH-2 INV switch Push in to invert the polarity of the
X-Y switch Push in to select X-Y operation.
V MODE switches To select the vertical amplifier display
their fully clockwise positions.
bandwidth.
separate ground lead to oscilloscope.
counter or other instrument.
(horizontal) amplifier during X-Y
operation.
amplifier during X-Y operation.
AC position connects a capacitor
between the input connector and its
associated amplifier circuitry to block
any DC component in the input signal.
GND position connects the amplifier
input to ground instead of the input
connector, so a ground reference can be
established. DC position connects the
amplifier inputs directly to the
associated input connector, thereby
passing alt signal components on to the
amplifiers.
the trace up. Inoperative during X-Y
operation.
the trace up. Adjusts the Y-axis of the
trace during X-Y operation.
Channel 2 signal.
CH-1
mode.
the input signal of channel 1 on the
CRT when pressed
push-button displays only
Figure 2-2
Vertical Amplifier Block
CH-2
push-button displays only the input signal
of channel 2 on the CRT when pressed.
ALT
push-button displays the input signals of
both channels 1 and 2 (or more) on the CRT
when pressed. The CRT beam is switched
between channels at the end of each sweep to
achieve this multi-channel display.
CHOP
push-button displays the input signals of
both channels 1 and 2 (or more) on the CRT
when pressed. The CRT beam is switched
between channels at a 250 kHz rate during the
horizontal sweep to achieve this multi-channel
display.
ADD
push-button displays a single trace that is
the algebraic sum of the input signals of channels
1 and 2 when pressed.
PULL TRIPLE control When pulled, displays traces for CH-1,
CH-2, and CH-3 (trigger), providing
ALT or CHOP push-button is also
pressed. Rotating this control also
vertically positions the CH-3 trace on
the CRT screen. This control is not
operative if any single-trace display
mode is selected.
PULL QUAD control When pulled, displays traces for CH-l,
CH-2, CH-3 (trigger), and algebraic
sum of CH-1 and CH-2 signals,
providing ALT of CHOP pushbutton is
also pressed. This control is not
operative if any single-trace display
mode is selected.
4
Page 8
2-1-3 Sweep and Trigger
24322526272829303133
Refer to Figure 2-3 for reference (24) to (42).
ATIME/DIV and To select either the calibrated
DELAY TIME sweep of the main (A) time-base
switch or the delay time range for delayed sweep operation.
B TIME/DIV switch To select the calibrated sweep rate of
A VARIABLE/ Provides continuously variable
PULL X 10 MAG adjustment of sweep rate between steps
Control of the TIME/DIV switches. TIME/DIV
UNCAL lamp Indicates when the VARIABLE control
DLY TIME MULT To determine the exact starting point
control within the A time base delay range at
Horizontal POSITION To adjust the horizontal position of the
control traces displayed on the CRT.
X FINE Position To adjust the horizontal position of the
control CRT traces as described above, but has
HORIZ DISPLAY To select the sweep mode.
Switches
Blocks
the delayed (B) time base.
calibrations are accurate only when the
A VARIABLE control is detented in its
fully clockwise position. Pulling the
control out expands the horizontal
deflection by 10 times for X-Y
operation. The effective time-base
sweep rate is also increased by 10
times, making 2 nS per division the
highest sweep rate available.
is not detented as described above.
which the B timebase will begin
sweeping. The absolute delay time is
equal to the sweep time rate (A
TIME/DIV) multiplied by the DLY
TIME MULT.
Clockwise rotation moves the trace(s)
to the right. During X-Y operation, this
control must be used for X-axis
positioning.
less effect per degree of rotation. This
facilitates precise positioning when Xl0
magnification is used.
A push-button sweeps the CRT at the
main (A) timebase rate when pressed.
INTEN BY B push-button sweeps the
CRT at the main (A) time-base rate
when pressed, and the delayed (B)
time-base intensifies a section of the
trace(s). The location of the intensified
section is determined by the DLY
TIME
MULT control, and under some
circumstances also by the START
switch (32).
B push-button sweeps the CRT at the
rate selected by the B TIMEY DIV
switch, after a delay determined by the
A TIME/DIV switch and DLY TIME
MULT control.
The trace displayed over the full CRT
graticule width corresponds to the
intensified section of trace displayed
during INTEN BY B operation.
ALT push-button alternately sweeps
the CRT at the main (A) time-base and
delayed (B) time-base rates when
pressed. This results in twice as many
traces displayed on the CRT as are displayed during any of the sweep modes
described above.
START switch When pressed in (TRIG'D position),
causes the B sweep to be triggered by
the first trigger pulse occurring after the
delay time set by the DLY TIME
MULT control. In this position, the
delay time is adjustable only in whole
increments of the time between trigger
pulses.
When released (AFTER DELAY
position), causes the B sweep to start
immediately after the delay time set by
the DLY TIME MULT control. In this
position, the delay time is adjustable
with infinite resolution.
A/B TRACE SEP Permits adjustments of the distance
control between corresponding A and B traces
when the ALT sweep mode is selected.
5
Page 9
SOURCE switch To select the signal used for A or B
34363735
36
383940
time-base triggering.
CH-1 position selects the channel 1
signal for triggering. CH-2 position
selects the channel 2 signal for
triggering.
ALT position selects the triggering
mode that allows a stable display of
two asynchronous signals on the CRT.
Must be used in conjunction with the
ALT vertical mode.
LINE position (A only) selects a trigger
signal derived from the AC power line,
permitting the scope to display
stabilized line-related components of a
signal even though they may be very
small compared to other signal
components.
0.2 V/DIV position selects the full
signal applied to the EXT TRIG IN
connector.
2 V/DIV position selects an attenuated
sample of the signal applied to the EXT
TRIG IN connector.
CH-3 or EXT TRIG For applying an external signal to the
IN connector oscilloscope for triggering the A
timebase and/or displaying the channel
3 trace.
COUPLING switch To select the frequency characteristics
of the coupling to the trigger circuits.
DC position selects direct trigger
coupling so all components of the
trigger signal are applied to the trigger
circuit.
AC position inserts a large capacitor in
the trigger-coupling chain to remove
any DC components from the trigger
signal. AC signals below 10 Hz are also
attenuated, as is the case in all of the
trigger coupling modes listed below.
HF-REJ position inserts a filter in the
trigger-coupling chain that removes
signal components higher in frequency
than 35 kHz.
TV-V (A only) position inserts a
shaping filter (TV sync separator)
whose low-frequency output (vertical
sync pulses) is used for triggering. This
trigger mode will also pass and
differentiate waveforms in the 1-100
Hz range.
TV-H position inserts a shaping filter
(TV sync separator) whose highfrequency output (horizontal sync
pulses) is used for triggering. This
trigger mode will also pass and
differentiate waveforms in the 2-500
kHz range.
When triggered B sweep is selected as
the horizontal-display mode, and the
COUPLING switch is set to any
position other than TV-V, the A- and
B- time base trigger signals are
identical. However, when the
COUPLING switch is set to TV-V
during triggered B sweep, the TV-V
shaping filter is inserted only in the Atime base trigger signal. The trigger
signal fed to the B time base will be
shaped by the TV-H filter.
SWEEP MODE To select the triggering mode. AUTO
switches push-button allows sweep to flee-run
and display a base-line in the absence
of signal when pressed. Automatically
switches to triggered sweep mode when
signal of 20 Hz or higher is present and
other trigger controls are properly set.
NORM push-button produces sweep
only when signal is present and other
triggering controls are properly set. No
trace is visible if any trigger
requirement is missing.
SINGLE pushbutton disables recurrent
sweep operation when pressed. The
sweep generator can then be manually
reset before each sweep by depressing
this switch again. No trace is visible
before or after sweep occurs.
READY lamp Indicates when sweep generator is
armed for single-sweep operation.
Lamp is extinguished at start of sweep.
SLOPE switch Push-button selects the positive or
negative slope of the trigger signal for
initiating sweep. +position n causes
triggering on the positive-going edge or
slope of the trigger signal. - .position
causes triggering on the negative-going
edge or slope of the trigger signal.
LEVEL control Selects the amplitude level at which the
sweep is triggered. When rotated
clockwise (+ direction), the trigger
point moves towards the positive peak
of the trigger signal. When rotated
counterclockwise (- direction), the
trigger point moves towards the
negative peak of the trigger signal.
Pulling the HOLDOFF knob
(concentric to the LEVEL control)
selects PRESET level, a trigger point
near the zero-crossing point of the
trigger waveform.
6
Page 10
TRIG'D lamp Indicates when the sweep generator is
4142464748434445
being triggered.
HOLDOFF control Allows triggering on certain complex
signals by changing the hold-off (dead)
time of the main (A) sweep. This
avoids triggering on intermediate
trigger points within the repetition
cycle of the desired display. NORM is
a detented position at full CCW
rotation that is used for ordinary
signals.
B ENDS A is a detented position at full
clockwise rotation that increases the A
timebase repetition rate to the
maximum to improve the apparent
brightness of "short" duration (lowduty cycle) pulses in the delayed mode.
2-1-4 Miscellaneous
Refer to Figure 2-4 for references (43) to (48).
Z AXIS INPUT For applying signal to intensity
Connector modulate the CRT.
FUSE Receptacle permits quick fuse re-
placement without opening case
Power Connector Permits removal or replacement of AC
power cord.
Voltage Label Indicates the voltage of the oscil-
loscope's primary wiring.
Cord Caddy Provides a quick method of securing
the power cord, and supports the
oscilloscope for vertical operation.
Feet Supports the oscilloscope for shelf
mounting.
2-2. INITIAL OPERATION
Before the instrument is operated for the first time, perform the
following procedures in the order listed to ensure satisfaction and
prevent damage to the instrument.
2-2-1 Power Connections and Adjustments
The instrument is normally shipped wired for a 120-volt power
source but can be adapted to operate from power sources with - 10%
of the rated values given in Table 2-1. Operation with a voltage less
that t0% of the rated value may result in improper performance of the
instrument and a voltage more than 10% in excess of the rated value
may damage the power supply circuitry.
To check or alter the power-transformer wiring, proceed as
follows:
1. Disconnect the power cord from the Power Connector (45).
2. Remove the 14 Phillips-head screws around the periphery of the
top and bottom covers.
3. Remove the covers and carefully turn the LBO-516 upside
down.
7
Page 11
4. Compare the wiring of the power transformer to that shown in
Figure 2-5. If you want to adapt the instrument to operate from a
different voltage, determine the correct wiring diagram from
Table 2-1.
5. Unsolder any connections not appropriate to the desired
connection, and install the new wiring.
6. Change the fuse (if necessary) to the value indicated in Table 21 for the selected voltage range. In all cases the fuse must be the
delayed-action ("SLO-BLOW') type.
Table 2-1
POWER TRANSFORMER PRIMARY WIRING
Nominal
Voltage
100V
120V
200 V
220 V
240 V
2-2-2 Installation
The LBO-516 will operate in either a horizontal or vertical
position, so it is highly suited to field or laboratory work. It can
therefore be positioned on a bench top, riser shelf, or even the floor.
Voltage
Range
90-110V
110-130 V
180-220 V
200-240 V
215-265 V
Rating Wiring
Diagram
1.25 A
1.25 A
0.80 A
0.80 A
0.80 A
B
C
D
E
F
For bench-top mounting, it is advantageous to have the front of
the instrument tilted upward for straight-on viewing. Press in the two
Handle-position Locks and simultaneously rotate the Handle so it
points below the case, then release the locks.
If the instrument is placed on a riser shelf above the work bench,
rotate the Handle above the instrument and as far towards the back as
possible. It is not necessary to lock it in this position.
If lack of working space requires that the instrument be placed
on the floor, stand the LBO-516 on end. The Cord Caddy (47) will
act as legs to support the instrument. Rotate the Handle just enough
back for clear access to the front-panel controls.
The LBO-516 is designed to operate over a temperature range of
0°C to +40°C (32°F to 104°F) and a humidity range of 10 to 90%.
Operation in a more severe environment may shorten the life of the
instrument.
Operation in a powerful magnetic field may distort the
waveform or tilt the trace. This is most likely to occur if the
instrument is operated close to equipment having large motors or
power transformers.
2-2-3 Preliminary Control Settings and Adjustments
1. Set the following controls as indicated:
AC/GND/DC switches (16) ........... AC
8
Page 12
VOLTS/DIV switches (10) ............. 2V
VARIABLE VOLTS/DIV controls (11) Fully CW, and
pushed in
V MODE switches (21) ................ ALT
Vertical POSITION controls (17 & 18) Index up
A INTEN control (3) ................... Index up
FOCUS control (5) ..................... Index up
ILLUM control (8) ...................... Fully CCW
CH-2 INV switch (19) ................. Out
PULL TRIPLE control (22) ........... Pushed in
PULL QUAD control (23) ............. Pushed in
HORIZ DISPLAY switches (31) ..... A
B TIME/DIV switch (25) .............. Any Ps
A TIME/DIV switch (24) .............. .2 mS
A VARIABLE control (26)
Horizontal POSITION control (29) .. Index up
SOURCE switch (34) .................. CH-1
COUPLING switch (36) ............... AC
SWEEP MODE switches (37) ....... AUTO.
HOLDOFF control (42) ................ Fully CCW, and
2. Plug the power cord into a convenient AC receptacle and press
in the POWER switch (1). Shortly, two traces should appear. If
the traces appear extremely bright, turn the A INTEN control (3)
counterclockwise. Otherwise, let the instrument warm up for a
few minutes.
CAUTION:
in the CRT. However, if the CRT is left with an extremely
bright dot or trace for a very long time, the fluorescent
screen may be damaged. Therefore, if a measurement
requires high brightness, be certain to turn down the
INTEN control immediately afterward. Also, get in the
habit of turning the brightness way down if the scope is left
unattended for any period of time.
3. Turn the A INTEN control (3) to adjust the brightness to the
desired amount.
4. Turn the FOCUS control (5) for a sharp trace.
5. Turn the CH-1 vertical POSITION control (17) to move the CH1 trace two divisions down from the top of the graticule grid.
Turn the CH-2 vertical POSITION control (18) to move the CH2 trace two divisions up from the bottom of the graticule grid.
6. See if the traces are precisely parallel with the graticule lines. If
they are not, adjust the ROTATION control (6) with a small
screwdriver.
7. Turn the horizontal POSITION control (29) to align the left edge
of the traces with the left-most graticule line.
8. Connect the CH- 1 (14) and CH-2 (15) input connectors to the
CAL connector (9). The TRIG'D lamp (41) should light and two
rectangular waveforms appear on the CRT screen.
9. Carefully examine the waveform, particularly at the corners,
while adjusting the FOCUS control to assure sharpest focus.
10. Disconnect the vertical inputs from the calibrator.
...........
A burn-resistant fluorescent material is used
Fully CW, and
pushed in
pulled out
2-3 BASIC OPERATING PROCEDURES
The following paragraphs in this section describe how to operate
the LBO-516, beginning with the most elementary operating modes,
and progressing to the less frequently-used and/or complex modes.
2-3-1 Signal Connections
There are three methods of connecting an oscilloscope to the
signal you wish to observe. They are: a simple wire lead, coaxial
cable, and scope probes.
A simple lead wire may be sufficient when the signal level is
high and the source impedance low (such as TTL circuitry), but is not
often used. Unshielded wire picks up hum and noise; this distorts the
observed signal when the signal level is low. Also, there is the
problem of making secure mechanical connection to the input
connectors. A binding post-to-BNC adapter is advisable in this case.
Coaxial cable is the most common method of connecting an
oscilloscope to signal sources and equipment having output
connectors. The outer conductor of the cable shields the central signal
conductor from hum and noise pickup. These cables are usually fitted
with BNC connectors on each end, and specialized cables and
adaptors are readily available for mating with other kinds of
connectors.
Scope probes are the most common method of connecting the
oscilloscope to circuitry. These probes are available with 1X
attenuation (direct connection), 10X and 100X attenuation. The 10X
attenuator probe increases the effective input impedance of the
probe/scope combination to 10 megohms shunted by a few
picofarads. The 100X probe increases the effective input impedance
of the probe/scope combination to anywhere from 10 to 100
megohms shunted by a few picofarads, depending upon probe model.
The reduction in input capacitance is the most important reason for
using attenuator probes at high frequencies, where capacitance is the
major factor in loading down a circuit and distorting the signal.
Despite their high input impedance, attenuator probes do not
pick up appreciable hum or noise. As was the case with coaxial cable,
the outer conductor of the probe cable shields the central signal
conductor. Scope probes, of any attenuation, are also quite
convenient from a mechanical standpoint. Nearly all quality probes
have a spring-loaded hook end that quickly and securely holds the
probe to wiring and component leads (see Figure 2-6). This hook can
be removed to expose a needlepoint, excellent for use on the foil side
of a pc board, or for quickly moving from one point to another.
To determine if a direct connection with shielded cable is
permissible, you must know the source impedance of the circuit you
are connecting to, the highest frequencies involved, and the
capacitance of the cable. If any of these factors are unknown, use a
10X low-capacitance probe.
An alternative connection method at high frequencies is
terminated coaxial cable. A feed-thru terminator having an
impedance equal to that of the signal-source impedance, is connected
to the input connector of the oscilloscope. A coaxial cable of
matching characteristic impedance connects the signal source to the
terminator. This technique allows using cables of nearly any practical
length without signal loss.
9
10
Page 13
Page 14
If a low-resistance ground connection between oscilloscope
and circuit is not established, enormous amounts of hum will
appear in the displayed signal. Generally, the outer conductor
of shielded cable provides the ground connection. If you are
using plain lead wire, be certain to first connect a ground
wire between the LBO-516 Ground connector (12) and the
chassis or ground bus of the circuit under observation.
WARNING:
chassis (via the 3-prong power cord). Be certain the
device to which you connect the scope is transformer
operated. Do NOT connect the LBO-516 or any other
test equipment to "AC/ DC", "hot chassis", or
"transformerless" devices. Similarly, do NOT connect
the LBO-516 directly to the AC power line or any
circuitry connected directly to the power line. Damage
to the instrument and severe injury to the operator may
result from failure to heed this warning.
2-3-2 Single-trace Operation
Single trace operation with single timebase and internal
triggering is the most elementary operating mode of the
LBO-516. Use this mode when you want to observe only a
single signal, and not be disturbed by other traces on the
CRT. Since the LBO-516 is fundamentally a two-channel instrument, you have a choice for your single channel. Channel
1 has an output terminal; use channel 1 if you also want to
measure frequency with a counter while observing the
waveform. Channel 2 has a polarity-inverting switch. While
this adds flexibility, it is not ordinarily used in single-trace
operation.
The LBO-516 is set up for single-trace operation as follows:
1. Set the following controls as indicated. Any controls not
mentioned here or in the following steps can be
neglected. Note that the trigger source selected (CH-1 or
CH-2 SOURCE) must match the single channel selected
(CH-1 or CH-2 V MODE).
VARIABLE VOLTS/DIV Fully CW,
controls (11) and pushed in
AC/GND/DC switches (16) .......... AC
V MODE switches (21) ............... CH- 1 or CH-2*
CH-2 INV switch (19) .................. Out
A INTEN control (3) ................... APS**
FOCUS control (5) ..................... APS**
POWER switch (1) ..................... In
HORIZ DISPLAY switches (31) ..... A
B TIME/DIV switch (25) .............. 0.5/KS
A VARIABLE control (26) ............ Fully CW, and
SOURCE switch (34) .................. CH- 1 or CH-2*
COUPLING switch (36) ............... AC
SWEEP MODE switches (37) ........ AUTO
HOLDOFF control (42) ................ Pulled out
Horizontal POSITION control (29) ..APS**
*These selections must match.
**As previously set.
2. Use the corresponding vertical POSITION control (17)
or (18) to set the trace near mid screen.
The LBO-516 has an earth-grounded
pushed in
PRESET level
3. Connect the signal to be observed to the corresponding
input connector (14) or (15), and adjust the
corresponding VOLTS/DIV switch (10) so the
displayed signal is totally on screen.
CAUTION:
4. Set the A TIME/DIV switch (24) so the desired number
of cycles of signal are displayed. For some
measurements just 2 or 3 cycles are best; for other
measurements 50-100 cycles (appears like a solid band)
works best.
5. If the signal you wish to observe is so weak that even
the 5 mV position of the VOLTS/DIV switch cannot
produce sufficient trace height for triggering or a usable
display, pull the VARIABLE (X10 MAG) control (11)
outwards. This produces 1 mV/div sensitivity when the
VOLTS/DIV switch is set to 10 mV, and .5 mW/div
when it is set to 5 mV.
6. If the signal you wish to observe is so high in frequency
that even the .02/KS position of the A TIME/DIV switch
results in too many cycles displayed, pull the A VARIABLE (X10 MAG) control (28) outwards. This
increases the effective sweep speed by a factor of 10, so
.02 KS/div becomes 2KS/div, .1/KS becomes .01 KS/div,
etc. The 2KS/div sweep speed achievable by
magnification is fast enough to display a single cycle of
a 50 MHz signal across the CRT face!
7. If the signal you wish to observe is either DC or low
enough in frequency that AC coupling attenuates or
distorts the signal, flip the AC/GND/DC switch (16) to
DC.
CAUTION:
2-3-3 Triggering Alternatives
Triggering is often the most difficult operation to
perform on an oscilloscope because of the many options
available and the exacting requirements of certain signals. By
using PRESET trigger level and the AUTO sweep mode,
error-free triggering is obtainable from the LBO-516. These
were the trigger options selected for the single-trace
operating procedure described in paragraph 2-3-2, and the
multi-trace and dual-time base operating modes described in
the following section. They will in fact work well with most
signals. However, for complex or otherwise difficult signals,
the LBO-516 operator may choose from an extensive
selection of trigger options. These are categorized as triggersource options, coupling options, sweep mode, and
triggerpoint selection.
Sweep Mode Selection. Normally, the CRT beam is not
swept horizontally across the face of the CRT until a sample
of the signal being observed, or another signal harmonically
related to it, triggers the timebase. This is the situation when
NORM SWEEP MODE (37) is selected. However, this trigger mode is inconvenient because no baseline appears on the
CRT screen in the absence of an input signal, or if the trigger
controls are improperly set. Since an absence of a trace can
also be due to an improperly set vertical position control or
VOLTS/DIV switch, much time can be wasted determining
the cause. The AUTO sweep mode solves this problem by
causing the timebase to automatically free run when not
triggered. This yields a single horizontal line with no signal,
greater than 400 V (DC + AC peak).
If the observed waveform is low-level
AC, make certain it is not riding on a highamplitude DC voltage.
Do not apply a signal
11
Page 15
and a vertically-deflected but non-synchronized display when
vertical signal is present but the trigger controls improperly
set. This immediately indicates what is wrong. The only
problems with AUTO operation are that signals below 20 Hz
cannot, and complex signals of any frequency may · not,
reliably trigger the timebase. Therefore, the usual practice is
to leave the AUTO pushbutton pushed in, but press NORM if
any signal (particularly one below 20 Hz) fails to produce a
stable display.
The third sweep mode, obtained by pressing the
SINGLE pushbutton, produces a nonrepetitive sweep. Its use
is described in
Trigger Source Options.
obtained from the signal applied to the vertical inputs, or
from a separate source of the same or a harmonically-related
frequency. The SOURCE switch (34) offers several choices.
The CH-1 and CH-2 positions offer a choice of which of
the two input channels the trigger signal is derived. The
choice of channels remains even if the trigger channel is not
displayed; the only requirements are that signal be applied to
the trigger-source channel and the associated VOLTS/DIV
switch be set to provide sufficient signal amplitude. The minimum trigger amplitude is around half a division below 10
MHz, and increases to 1 1/2 divisions at 100 MHz. For insurance, use at least a full division below 10 MHz, and two divisions above 10 MHz.
If both channels are displayed, and the two signals are
different but harmonically-related frequencies, trigger from
the low-frequency channel if possible. This will ensure that
traces are stable.
Select the ALT position when you want to display two
signals not harmonically related (720 Hz and 939 Hz, for
example). The ALT SOURCE position must be used in
conjunction with the ALT V MODE (21) pushbutton for this
type of dual-trace display.
The LINE position provides trigger signal at the local
power-line frequency. This is of great use when you wish to
observe a low-level ripple component imposed on a large DC
voltage, or within a mixture of other AC voltages. The linefrequency trigger will sync signal at any reasonable multiple
of the power-line frequency.
2-3-10 Single-shot Operation.
Trigger signal can be
The 0.2 V/DIV and 2 V/DIV positions both select
external trigger signal applied to the EXT TRIG IN
connector (35). Use 0.2 V/DIV position when the external
trigger amplitude is between 100 mV and 2000 mV peak-topeak. Use the 2 V/ DIV position when the signal amplitude is
between 2 V and 20 V peak-to-peak.
CAUTION:
V (DC + AC peak).
Using a trigger source not derived from the channel you
are watching has the advantage that changes in the amplitude
of the signal under observation will not cause the display to
lose sync, even if the amplitude of the observed signal falls
below a half graticule division. External trigger also has the
advantage that complex and/or noisy signals can be stably
displayed, providing the trigger signal is free of noise.
Trigger Coupling Options.
coupling options for the main (A) and delayed (B) timebases
increase the probability of stable triggering on difficult
signals, such as those containing several frequencies and/or
hum and noise.
The first two COUPLING positions (36) are frequencyselective filters that pass certain frequencies on to the trigger
circuitry and reject others. The AC position removes any DC
component in the trigger signal.
The HF-REJ position cuts off frequencies higher than
35 kHz, passing only signals in the 10 Hz to 35 kHz region.
Select this position if high-frequency noise (the CHOP
switching pulses for example) is mixed with a low-frequency
signal.
The DC position removes all filters from the trigger
chain, so everything in the trigger signal from DC to the
upper bandwidth limit of the oscilloscope is passed to the
trigger circuits. Select DC COUPLING if the trigger signal is
below 10 Hz, or may be expected to be below this frequency
at some time during a series of measurements.
The TV-V and TV-H positions insert a TV sync
separator into the trigger chain, so a clean trigger signal at
either the vertical or horizontal repetition rates can be
removed from a composite video signal. The TV-V position
is also effective in securing stable triggering at the low frequency (60 or 70 Hz) of an audio intermodulation distortion
Do not apply a signal greater than 400
The various trigger
12
Page 16
test signal. To trigger the scope at the vertical (field) rate,
select the TV-V position. To trigger the scope at the horizontal (line) rate, select the TV-H position. When either TV position is used, the SLOPE switch (39) must be matched to the
polarity of the video signal. Leave the SLOPE pushbutton out
(+ position) for positive-sync signals (Figure 2-7a), and push
it in (- position) for negative-sync video signals (Figure 2-7b).
timebase must be triggered at the exact same point on the re-
Trigger Point Selection
current waveform each time the timebase is swept. This is
sometimes difficult to achieve, so the LBO-516 has three
controls that enable the operator to achieve this condition.
They are the LEVEL control (40), the SLOPE switch (39),
and the HOLDOFF control (42).
. For a stable display, the
The SLOPE switch determines whether the sweep will begin
on a positive-going or negative-going slope of the trigger
signal (see Figure 2-8). In some cases, the choice of slope is
unimportant; in others, it is vitally important to attain a stable
and/or jitter-free display. Always select the steepest and most
stable slope or edge. For example, small changes in the
amplitude of the sawtooth shown in Figure 2.8a will cause
jitter if the timebase is triggered on the positive (ramp) slope,
but have no effect if triggering occurs on the negative slope (a
fast-fall edge). In the example shown in Figure 2-8b, both
leading and trailing edges are very steep (fast rise and fall
times). However, this particular pulse is the output of a
leading-edge triggered monostable, and has pulse-width jitter.
Triggering from the jittering trailing edge will cause the entire
trace to jitter, making observation diffi-
13
Page 17
cult. Triggering from the stable leading edge (+ slope) yields a
trace that has only the trailing-edge jitter of the original signal. If
you are ever in doubt, or have an unsatisfactory display, try both
slopes to find the best way.
The LEVEL control determines the point on the selected
slope at which the main (A) timebase or delayed (B) timebase will
be triggered. The effect of the LEVEL control on the displayed
trace is shown in Figure 2-9a. The +, 0, and - panel markings for
this control refer to the waveform's zero crossing and points more
positive (+) and more negative (-) than this. If the trigger slope is
very steep, as with square waves or digital pulses, there will be no
apparent change in the displayed trace until the LEVEL control is
rotated past the most positive or most negative trigger point,
whereupon the display will free run (AUTO sweep mode) or
disappear completely (NORM sweep mode). Try to trigger at the
mid point of slow-rise waveforms (such as sine and triangular
waveforms), since these are usually the cleanest spots on such
waveforms. As figure 2-9b shows, triggering on a noisy area will
cause instability in the display. Pulling the HOLDOFF control
outwards to the PRESET level position automatically triggers the
timebase near the zero-crossing point of the trigger signal.
The larger the amplitude of the trigger signal inputted to the
trigger circuits, the greater is the degree of rotation (control range)
over which the LEVEL control will maintain a stable display.
With internally-derived trigger, the actual trigger amplitude is
proportional to the number of graticule divisions occupied by the
trace. Therefore, the trigger point is more critical with small
signals than large. This is one reason why it is important to use as
much trace height as practical for the number of traces displayed.
The HOLDOFF control is used for special circumstances
only. It allows the operator to alter the mandatory "dead" time
between the end of one sweep and the start of the next (in
response to a trigger pulse). This prevents the triggering of
subsequent sweeps by the wrong trigger pulse in a complex
waveform. During normal operation, leave the HOLDOFF control
click-stopped at NORM. When viewing complex waveforms
containing multiple trigger points per repetition, rotate the
HOLDOFF control clockwise until the proper waveform is
secured, as shown in Figure 2-10. For example, the waveform
shown contains three pulses in each group capable of triggering
the timebase, but sweep must begin only on the first pulse in each
burst to obtain the proper display. In the lower display, the dead
time has been extended enough to make it impossible for last
pulse in the second burst to start the next sweep.
Rotate the HOLDOFF control fully clockwise to its B ENDS
A click-stopped position when using the delayed (B) timebase and
the difference between the A and B TIME/DIV setting is large (6
positions or more). The resulting brightness improvement is
greatest when the delay time between B and A timebases is short.
2-3-4 Probe Compensation
The LP- 100X probes furnished with the LBO-516 must be
adjusted to the input capacitance of the. channel(s) with which
they are used. If the probes are used only with vertical input
channels 1 and 2, this adjustment need be performed only when
the probes are first used, and the probes can be used
interchangeably between these channels without adjustment.
However, if an additional probe is purchased for the trigger input
channel (CH-3), mark it and compensate it separately, as the CH-3
input capacitance is somewhat different.
To compensate a probe for CH-1 or CH-2, proceed as follows:
1. Connect the probe to the CH-1 input connector (14) and the
CAL connector (9).
2. Set the CH- 1 VOLTS/DIV switch (10) to 20 mV, the CH- 1
AC/GND/DC switch (16) to DC, and the A TIME/DIV
switch (24) to .2 mS.
3. Press the CH-1 V MODE pushbutton (21) and A HORIZ
DISPLAY pushbutton (35), and select CH-1 SOURCE (34).
4. With a small screwdriver, adjust the capacitance-correction
trimmer (Figure 2-6a) for a correct-appearing square wave.
(Figure 2-6d).
14
Page 18
To compensate a probe for CH-3, proceed as follows:
1. Connect the probe to the CH-3 or EXT TRIG IN connector
(35) and a 1000 Hz signal source set for 8 Vp.p output
amplitude.
2. Set the A TIME/DIV switch to .2 mS, the SOURCE
switch to .2 V/DIV, and the COUPLING switch to DC.
3. Press the ALT V MODE pushbutton (21), the A HORIZ
DISPLAY pushbutton (35), and push in the HOLDOFF
control (42).
4. Pull the PULL TRIPLE control (22) and adjust it to position
the CH-3 trace at midscreen. Adjust the LEVEL control (40)
if needed.
5. With a small screwdriver, adjust the capacitance-correction
trimmer (Figure 2-6a) for a correct-appearing square wave.
(Figure 2-6d).
2-3-5 Dual Trace Operation
Dual-trace operation is the major operating mode of the
LBO-516, since full amplification and attenuation facilities are
provided for the two channels. As was the case with Single-trace
Operation, you have a choice here too, not of channel selection,
but of how to display the two channels.
The LBO-516 is set up for dual-trace operation as follows:
1. Set the following controls as indicated below. Any controls not
mentioned here or in the following steps can be neglected.
VARIABLE VOLTS/DIV controls (11) Fully CW, and
pushed in
AC/GND/DC switches (16) ......................... AC
CH-2 INV switch (19) ................................. Out
PULL TRIPLE control (22) ......................... In
PULL QUAD control (23) ........................... In
A INTEN control (3) ................................... APS*
FOCUS control (5) ...................................... APS*
POWER switch (1) ..................... In
HORIZ DISPLAY switches (31) ..... A
B TIME/DIV switch (25) .............. 0.5/PS
A VARIABLE control (26) ........... Fully CW, and
pushed in.
SOURCE switch (34) .................. CH-I or CH-2**
COUPLING switch (36) ............... AC
SWEEP MODE switches (37) ........ AUTO
HOLDOFF control (42) ............................... Pulled out
Horizontal POSITION control (29) .............. APS*
*As previously set.
**See Step 6.
15
Page 19
2. Press either ALT or CHOP V MODE pushbutton (21). Press
ALT for relatively high-frequency displays (A TIME/DIV
switch set at .2 mS or faster); press CHOP for relatively lowfrequency displays (A TIME/DIV switch set at .5 mS or
slower). If the CHOP pushbutton is pressed when fast sweep
speeds are used, the displayed traces will appear broken (as
in Figure 2-11) when signals are applied. If the ALT
pushbutton is pressed when slow sweep speeds are used, the
display will flicker excessively.
3. Use the vertical POSITION controls (17 and 18) to set the
CH-1 trace about two divisions down from the top graticule
line, and the CH-2 trace about two divisions up from the
bottom graticule line.
The LBO-516 is set up for dual-trace operation as follows:
4. Connect the signals to be observed to the CH-1 and CH-2 IN
connectors (14) and (15), and adjust the VOLTS/DIV
switches (10) so the displayed signals are totally on screen
and clear of each other.
CAUTION:
(DC + AC peak).
5. Set the A TIME/DIV switch (24) so the desired number of
cycles are displayed. Be certain the display mode (ALT or
CHOP) selected is consistent with this sweep speed (as per
Step 2).
6. If both channels are handling signals of the same frequency,
trigger from the channel having the steepest-slope waveform.
If the signals are different but harmonically-related
frequencies, trigger from the channel carrying the lowest
frequency. Also, bear in mind that if you disconnect the
signal to the channel serving as the trigger source, the entire
display will free run.
7. If the signals are different frequencies and not harmonically
related, select the ALT trigger SOURCE position (34) and
the ALT V MODE pushbutton (21) regardless of the A
TIME/DIV switch setting.
8. If the signal you wish to observe is so weak that even the 5
mV position of the VOLTS/DIV switch cannot produce
sufficient trace height for triggering a usable display, pull the
VARIABLE (XI0 MAG) control (11) outward. This
produces 1 mV/ div sensitivity when the VOLTS/DIV switch
is set to I0 mV, and .5 mV/div when it is set to 5 mV.
Do not apply signals greater than 400 V
9. If the signal you wish to observe is so high in frequency that
even the .02/aS position of the A TIME/DIV switch results in
too many cycles displayed. Pull the A VARIABLE (XI0
MAG) control (26) outward. This increases the effective
sweep by a factor of 10, so .02 PS/div becomes 2 KS/div,
0.1PS/div becomes .01 /PS/div, etc. The 2 KS/div sweep
speed achievable by magnification is fast enough to display a
single cycle of a 50 MHz signal across the CRT face.
10. If the signal you wish to observe is either DC or low enough
in frequency that AC coupling attenuates or distorts the
signal, flip the AC/GND/DC switch (16) to DC.
CAUTION:
low-level AC, make certain it is not riding
2-3-6 Additive and Differential Operation
Additive and differential operation are forms of two-channel
operation where two signals are combined to display one trace. In
additive operation, the resultant trace represents the algebraic sum
of the CH-1 and CH-2 signals. In differential operation, the
resultant trace represents the algebraic
CH-I and CH-2 signals.
To set up the LBO-516 for additive operation, proceed as
follows:
1. Set up the dual-trace operation per paragraph 2-3-5, Steps 1
to 6 and 8 to I0.
2. Make sure both VOLTS/DIV switches (I0) are set to the
same position; and the VARIABLE controls (11) are detented in their CAL'D position. If the signal levels are very
different, set both VOLTS/DIV switches to the position
producing a large on-screen display of the
signal.
3. Trigger from the channel having the biggest signal.
4. Press the ADD V MODE (21) pushbutton. The single trace
resulting is the algebraic sum of the CH- 1 and CH-2 signals.
Either or both of the vertical POSITION controls (17) and
(18) can he used to shift the resultant trace.
5. If the p-p amplitude of the resultant trace is very small, mm
both
Make sure both VOLTS/DIV controls are set to the same
position.
To set up the LBO-516 for differential operation, proceed as
follows:
1. Set up for dual-trace operation per paragraph 2-3-5,
2. Ensure that both VOLTS/DIV switches (10) are set to
3. Trigger from channel having the larger signal.
4. Press in the CH-2 INV pushbutton (19).
on a high-amplitude DC voltage.
NOTE: If the input signals are in-phase, the amplitude
of the resultant trace will be the arithmetic sum of the
individual traces (e.g., 4.2 div + 1.2 div = 5.4 div). If the
input signals are 180° out of phase, the amplitude of the
resultant trace will be the arithmetic difference of the
two traces (e.g., 4.2 div - 1.2 div = 3.0 div).
VOLTS/DIV switches to increase the display height.
Steps 1 to 6 and 8 to I0.
the same position. If the signal levels are very different,
temporarily set both VOLTS/DIV switches to the
position needed to produce a large on-screen display of
the highest-amplitude signal.
If the observed waveform is
difference
between the
higher amplitude
16
Page 20
5. Press the ADD V MODE pushbutton (21)· The single trace
resulting is the algebraic difference of the CH-1 and CH-2
signals. Either or both of the vertical POSITION controls
(17) and (18) can be used to shift the resultant trace.
NOTE: If the input signals are in-phase, the amplitude
of the resultant trace will be the arithmetic difference of
the individual traces (e.g., 4.2div - 1.2div = 3.0div). If
the input signals are 180° out of phase, the amplitude of
the resultant trace will be the arithmetic sum of the
individual traces (e.g., 4.2 div + 1.2 div = 5.4 div).
6. If the peak-to-peak amplitude of the resultant trace is very
small, mm both VOLTS/DIV switches to increase the display
height. Make sure both VOLTS/DIV controls are set to the
same position.
2-3-7 Triple-trace Operation
A very useful feature of the LBO-516 is that the timebase
trigger can be displayed on the CRT screen along with the two
vertical inputs. The trigger signal appears as the third trace,
permitting continuous trigger view and/or a third input channel.
Trigger Display.
trigger signal and two input channels, proceed as follows:
1. Set the following controls as indicated below. Any
controls not mentioned here or in the following steps can be neglected.
PULL TRIPLE control (22) ......................... Pulled out
CH-2 INV switch (19) ................................. Out
VARIABLE VOLTS/DIV Fully CW, and
controls (11) pushed in
AC/GND/DC switches (16) .......................... AC
PULL QUAD control (23) ........................... Pushed in
A INTEN control (3) ................................... APS*
FOCUS control (5) ...................................... APS*
POWER switch (1) ...................................... Pushed in
HORIZ DISPLAY switches (31) .................. A
B TIME/DIV switch (25) ............................. 05/PS
A VARIABLE control (26) ......................... Fully CW, and
Horizontal POSITION control (29) .............. APS*
* As previously set.
** See Step 7.
2. Press the ALT or CHOP V MODE pushbutton (21). Press
ALT for relatively high-frequency displays (A TIME/DIV
switch set at .2 mS/div and faster); press CHOP for relatively
low-frequency displays (A TIME/DIV switch set at .5mS/div
and slower). If the CHOP pushbutton is pressed when fast
sweep speeds are used, the displayed traces will appear as
broken lines when signal is applied. Conversely, if the ALT
pushbutton is pressed when low sweep speeds are used, the
display will flicker excessively.
To continuously display the timebase
3. Use the vertical POSITION controls (17 and 18) to set the
CH- 1 trace near the 90% dotted graticule line, and the CH-2
trace on the center graticule line.
4. Use the PULL TRIPLE control (22) to set the third trace near
the 10% dotted graticule line.
5. Connect the signal to be observed to the CH-1 and CH-2 IN
connectors (14 and 15), and adjust the VOLTS/DIV switches
(10) so the displayed signals are totally on screen and clear
of each other.
6. Set the A TIME/DIV switch (24) so the desired number of
cycles is displayed. Be certain the display mode (ALT or
CHOP) selected is consistent with this switch setting (per
Step 2). If the signal you wish to observe is so high in fre-
quency that even the .02 PS position of the A TIME/DIV
switch results in too many cycles displayed, pull the A
VARIABLE (XI0 MAG) control (26). This increases the
effective sweep speed by a factor of 10, so .02 PS/div becomes 2 KS/div.
7. If CH-1 and CH-2 are both handling signals of the same
frequency, trigger from the channel haying the steepest
waveform. If the signals are different but harmonically-related frequencies, trigger from the channel carrying the
lowest frequency.
8. The third trace is the timebase trigger signal. With trigger
taken from either CH- 1 or CH-2, the trigger signal may appear to be the same as one of the vertical channels. However,
trigger COUPLING switch positions other than DC insert
frequency-selective networks into the CH-3 amplifier, so the
third trace may appear different at certain frequencies.
NOTE: If ALT trigger source is selected, the third trace
will resemble the CH-1 trace, not the composite trigger
channels, proceed as follows:
2-3-8 Four-trace Operation
displayed as the fourth trace in this mode of operation. To display
the CH-1 and CH-2 input signals, their algebraic sum, and the
signal triggering the timebase, proceed as follows:
17
signal.
Three Input Channels
1. Perform Steps 1 to 6 of the previous procedure.
2. Connect the third signal to be observed to the EXT
TRIG IN (CH-3) connector (35). If the three signals are
different but harmonically-related frequencies, apply the
lowest-frequency signal to this channel.
CAUTION: Do not apply a signal greater than 400 V
(DC + AC peak).
3. Set the SOURCE switch (34) to the 2 V/DIV position. If
the trace is less than one division high, external
amplification will be needed.
4. The third trace is the CH-3 input signal as well as the
timebase trigger, so do not use any trigger coupling
position other than AC or DC. The bandwidth-limiting
filters inserted at other positions of the COUPLING
switch (36) will distort the CRT display of the CH-3
input signal.
The algebraic sum of the CH-I and CH-2 input signals is
. To display three independent input
Page 21
1. Set the following controls as indicated. Any control not
mentioned here or in the following steps can be neglected.
PULL QUAD control (23) ........................... Pulled out
CH-2 INV switch (19) ................................. Out
VARIABLE VOLTS/DIV controls (11) Fully CW, and
pushed in
AC/GND/DC switches (16) ......................... AC
A INTEN control (3) ................................... APS*
FOCUS control (5) ...................................... APS*
POWER switch (1) ...................................... Pushed in
B TIME/DIV switch (25) .............. . 05P S
HORIZ DISPLAY switches (31) ..... A
A VARIABLE control (26) ........... Fully CW, and
pushed in
SOURCE switch (34) .................. CH-1 or CH-2**
COUPLING switch (36) ............... AC
SWEEP MODE switches (37) ........ AUTO
HOLDOFF control (42) ................ Pulled out
(PRESET level)
Horizontal POSITION control (29) .. APS*
* As previously set. ** See Step 6.
2. Press the ALT or CHOP V MODE pushbutton (21). Press
ALT for relatively high-frequency displays (A TIME/ DIV
switch set at .2 mS/div and faster); press CHOP for relatively
low-frequency displays (A TIME/DIV switch set at .5mS/div
and slower). If the CHOP pushbutton is pressed when fast
sweep speeds are used, the displayed traces will appear as
broken lines when signal is applied. Conversely, if the ALT
pushbutton is pressed when low sweep speeds are used, the
display will flicker excessively.
3. Use the vertical POSITION controls (17 and 18) to set the
CH-1 trace two graticule divisions from the bottom of the
CRT screen. This will set the sum trace (CH- 1 + CH-2) near
the center graticule line.
NOTE: The position of the sum trace is not separately
controllable.
4. Use the PULL TRIPLE control (22) to temporarily set the
CH-3 trace off screen.
5. Connect the signals to be observed to the CH-1 and CH-2 IN
connectors (14 and 15), and adjust the VOLTS/DIV switches
(10) so the displayed traces are totally on screen and well
clear of each other. Make sure both VOLTS/ DIV switches
are set to the same position, and their VARIABLE controls
(11) are detented in their CAL'D positions. If the signal
levels are very different, set both VOLTS/DIV switches to
the position suitable for the higher-level signal.
6. Set the trigger SOURCE switch (34) to match the channel
with the higher-amplitude signal.
7. Set the A TIME/DIV switch (24) so the desired number of
cycles is displayed. Be certain the display mode (ALT or
CHOP) selected is consistent with this switch setting (per
Step 2). If the signal you wish to observe is so high in
frequency that even the .02 p3 position of the A TIME/ DIV
switch results in too many cycles displayed, pull the A
VARIABLE (XI0 MAG) control (26). This increases the
effective sweep speed by a factor of I0, so .02PS/div
becomes 2 KS/div.
8. The CH-2 INV switch (19) can be pushed in to display the
difference signal between the CH-1 and CH-2 input signals
instead of their sum.
9. If your primary reason for selecting the four-trace display
mode is to view the sum or difference signal while simultaneously viewing the two signals from which it is derived,
leave the CH-3 trace off screen. If you need to see the timebase trigger trace as well, use the PULL TRIPLE control to
move the CH-3 trace to a relatively vacant spot on screen.
10. If the CH-3 trace is used as a third input channel, set the
trigger SOURCE switch to 0.2 V/DIV or 2 V/DIV, as befits
the input-signal amplitude. Since this trace is also the
timebase trigger signal, some positions of the trigger
COUPLING switch (36) will distort the trace because of the
limited-bandwidth filters they insert. Therefore, use either
the DC or AC COUPLING settings in this application.
2-3-9 Delayed-timebase Operation
The LBO-516 contains two timebases, arranged so one (the
A timebase) may provide a delay between a trigger event and the
beginning of sweep by the second (B) timebase. This allows any
selected portion of a waveform, or one pulse of a pulse train, to be
spread over the entire screen. Moreover, the CRT can be
alternately swept by the two timebases, so both the full waveform
and the selected portion appear across the full CRT screen width.
The aforementioned dual-timebase displays can be used with
any of the vertical display modes (single trace, dual trace, triple
trace, or quad). The procedure is the same regardless of the
number of traces displayed.
Basic Delayed Sweep
follows:
1. Set up the LBO-516 as directed for whatever vertical mode
you desire.
2. Make sure the START pushbutton (32) is out.
3. Press the INTEN BY B pushbutton (31). A section of the
trace(s) will intensify (brighten).
NOTE: The intensified portion will be quite small if there is
a large difference between the settings of the A and B
TIME/DIV switches. 4. Turn the B TIME/DIV control (25)
until the intensified portion of the trace widens to an amount
equal to the portion of the trace you wish to magnify (see
Figure 2-12b).
5. Turn the DLY TIME MULT control (28) to position the
intensification over the portion of the trace you wish to
magnify.
6. Press the B HORIZ DISPLAY pushbutton (31). That portion
of the trace intensified in Step 5 now appears spread over the
full width of the CRT screen. The trace now displayed is
being swept by the B timebase (Figure 2-12c).
7. If needed, additional enlargement is possible by palling the A
VARIABLE (X10 MAG) control (26) outward.
. For delayed sweep, proceed as
18
Page 22
B Intensity Adjustment.
relative to A trace brightness as the difference in A and B
TIME/DIV switch setting varies. The B INTEN control (4) allows
compensatory adjustment for the brightness difference. This
control can be rotated clockwise for increased brightness.
The B trace brightness varies
Alternate Sweep Mode.
main (A) and delayed (B) timebase traces for each vertical
channel used. The total number of traces is always doubled. Since
up to eight traces may appear in the alternate sweep mode, most
of the effort in this procedure involves adjusting trace amplitudes
and positions to get an understandable display.
To simultaneously display the A and B timebase traces,
proceed as follows:
1. Adjust the vertical VOLTS/DIV control(s) (10) so each trace
displayed does not exceed the number of divisions indicated
in Table 2-2. This is simply to insure that there is room for
all traces when switching to alternate sweep.
2. For the same reason, position the trace(s) so there is room
each
near
equal amplitude.
3. Display the B timebase as described in the preceding paragraph,
4. Press the ALT HORIZ DISPLAY pushbutton (31). The B
timebase trace(s) will now be displayed below its corresponding A timebase trace(s).
trace currently displayed for an additional trace of
Basic Delayed Sweep.
This sweep mode displays both
5. If necessary, adjust the A/B TRACE SEP control (33) so the
B timebase trace(s) do not overlap the A timebase traces.
Some adjustments with the vertical POSITION,
VOLTS/DIV, and A/B TRACE SEP controls may be necessary if the display is crowded (as in triple-trace and fourtrace operation).
NOTE:
Positioning eight traces can be difficult at first. The
suggested layout is to set the CH-1 baseline two graticule
divisions down from the top, and the CH-2 baseline two divisions up from the bottom. This puts the sum or difference
trace on the center graticule line. For positive-logic signals
(TTL, CMOS, etc.), set the CH-3 baseline on the bottom
graticule line, and later set the alternate B-sweep display
above
the A-sweep traces. For negative-logic signals (such
as ECL), set the CH-3 baseline on the top graticule line, and
later set the alternate B-sweep display
traces.
6. In measurement situations where the B sweep is very dim
(even with the B INTEN control (4) fully clockwise), you
can greatly increase the B sweep brightness by rotating the
HOLDOFF control (42) clockwise until it clicks into its B
ENDS A position. However, this will eliminate the A trace
from the intensified position onward. (See Figure 2-13).
19
below
the A-sweep
Page 23
Triggered B Sweep
is not triggered by a signal event; it begins when the main sweep
(A timebase) ends. This is readily seen in the alternate sweep
mode. The only problem with this is that main timebase jitter
becomes apparent in the B sweep when at high ratios of A to B
TIME/DIV switch settings (100:1 and up). To circumvent this, the
B sweep can be triggered by the signal itself or a time-related
trigger signal. The DLY TIME MULT control then determines the
minimum
time will be that plus the additional time until the next available
trigger. The result is that actual delay time is variable only with
step resolution, in increments of the interval between triggers.
get-signal supplied to the A timebase. For triggered B sweep,
proceed as follows:
1. Set up the scope for basic delayed or alternate sweep as
2. Press in the START pushbutton (32). The B timebase is now
2-3-10 Single-shot Operation
photograph a non-recurrent or transient event. The operation itself
is simple, but requires some preparation to ensure its success. To
set up for single-shot operation, proceed as follows:
1. Connect the CH-1 IN connector (14) to a signal source (a
2. Adjust the LBO-516 controls for the desired display, pref-
3. Press the NORM SWEEP MODE pushbutton (37), set the
4. Adjust the LEVEL control (40) for a stable trace.
delay time between A and B sweeps; the actual delay
The B timebase is triggered internally, using the same trig-
described in the preceding paragraphs.
triggering on a signal related in time to the A timebase
trigger. The start of the B sweep will always be a leading or
trailing edge of the trigger signal, turning the DELAY TIME
control will not change this.
NOTE:
V, the B timebase trigger signal will be filtered by the
TV-H filter. This facilitates inspection of complex
signals containing composite sync, such as VITS, VIRS,
and various coding signals found in the vertical interval.
Single-shot or single-sweep operation is used to observe or
pulse generator, for example) adjusted to produce recurrent
output pulses having the same polarity, amplitude, and pulse
width expected of the transient pulse to be observed. Keep
the repetition rate low (10 Hz or less) to get an idea of what
trace brightness will be like when observing the transient.
erably single-channel. Ensure that the channel 1 trace
amplitude is at least 2 divisions.
NOTE:
Multichannel operation is possible, but the CHOP
vertical mode must be used regardless of the sweep speed.
Because of the dim and broken trace resulting from CHOP
operation at high sweep speeds, a single channel is
recommended for single-shot observation of fast transients.
COUPLING switch (36) to DC, and the SOURCE switch (34)
to CH-1.
. In basic delayed sweep, the B timebase
If the COUPLING SWITCH (36) is set to TV-
5. Disconnect the substitute signal source, then connect the
CH- 1 IN connector to the transient to be observed.
6. Press the SINGLE SWEEP MODE pushbutton (37) twice.
After the second time, the READY lamp (38) will light.
7. The LBO-516 is now ready to display the transient. When it
occurs, the TRIG'D lamp (41) will flash, and the timebase
will sweep once, displaying the transient. When the sweep
starts, the READY lamp will go out. The sweep cannot be
retriggered by another transient until the SINGLE SWEEP
MODE pushbutton is pushed again.
2-3-11 X-Y Operation
The internal timebase of the LBO-516 is not utilized in X-Y
operation. Deflection in both the horizontal and vertical directions
is via external signals. One of the vertical input channels serves as
the X-axis (horizontal) signal processor, so horizontal and vertical
axes have identical control facilities.
All of the V MODE, HORIZ DISPLAY, trigger SOURCE
and COUPLING, and SWEEP MODE switches, as well as their
associated controls and connectors are inoperative in the X-Y
mode.
To set up the LBO-516 for X-Y operation, proceed as fol-
lows:
1. Push in the X-Y pushbutton (20).
CAUTION:
undeflected spot is very bright, or you may damage the CRT
phosphor screen
2. Apply the vertical signal to the CH-2 or Y IN connector (15),
and the horizontal signal to the CH-1 or X IN connector (14).
Once the trace is deflected, adjust the A INTEN control (3)
for suitable brightness.
3. Adjust the trace height with the CH-2 VOLTS/DIV switch
(10), and the trace width with the CH-1 VOLTS/DIV switch
(10). The VARIABLE VOLTS/DIV controls (11) and their
associated X10 MAG switches can also be used to adjust
trace amplitude along either axis.
4. Adjust the trace position vertically (Y axis) with the CH2
vertical POSITION or Y control (18). Adjust the trace
position horizontally (X axis) with the horizontal POSITION
control (29) and X FINE control (30); the CH-1 vertical
POSITION control has no effect during X-Y operation.
5. The vertical (Y-axis) signal can be inverted via the CH-2
INV pushbutton (19).
2-3-12 Intensity Modulation
Intensity modulation, also known as Z-axis modulation, is a
rarely-used operational mode wherein an external signal controls
the brightness of the CRT trace. Its main applications are in video
display and time or frequency marking. When so used, it is
usually in conjunction with X-Y operation (described in paragraph
2-3-11).
20
Reduce the trace intensity immediately if the
.
NOTE:
The X10 MAG switch on the A VARIABLE
control is operative, but should not be used. Keep this
knob pushed in.
Page 24
To intensity modulate the CRT, simply connect the modulating signal to the Z AXIS INPUT connector (43) on the back
panel. The modulating signal must exceed + 2 volts DC to
completely blank the trace at any brightness setting. At low
brightness levels, blanking may occur at signal voltages as low as
0.5 volt. A blanking signal in the range of + 2 to + 5 volts DC
(TTL high) is recommended.
CAUTION: Do not apply a signal greater than
50 V (DC + AC peak).
2-4 MEASUREMENT APPLICATIONS
This section contains instructions for using your LBO-516
for specific measurement procedures. However, this is but a small
sampling of the many applications possible for this oscilloscope.
These particular applications were selected to demonstrate certain
controls and features not fully covered in BASIC OPERATING
PROCEDURES, to clarify certain operations by example, or for
their importance and universality.
2-4-1 Amplitude Measurement
The modern triggered-sweep oscilloscope has two major
measurement functions. The first of these is amplitude. The
oscilloscope has an advantage over most other forms of amplitude
measurement in that complex as well as simple waveforms can be
totally characterized (i.e., complete voltage information is
available).
Oscilloscope voltage measurements generally fall into one of
two types: peak-to-peak or instantaneous. Peak-to-peak (p-p)
measurement simply notes the total amplitude between extremes
without regard to polarity reference. Instantaneous voltage
measurement indicates the exact voltage from from each and
every point on the waveform to a ground reference. When making
either type of measurement, ensure that the VARIABLE controls
(11) are rotated fully clockwise and de-tented in their CAL'D
position.
Peak-to. Peak Voltages
proceed as follows:
1. Set up the LBO-516 for the vertical mode desired per the
instructions in 2-3 BASIC OPERATING PROCEDURES.
. To measure peak-to-peak voltage,
2. Adjust the TIME/DIV switch (24) or (25) for two or three
cycles of waveform, and set the VOLTS/DIV switch (10) for
the largest possible totally on-screen display.
3. Use the appropriate vertical POSITION control (17) or (18)
to position the negative signal peaks on the nearest horizontal
graticule line below the signal peaks, per Figure 2-14.
4. Use the horizontal POSITION control (29) to position one of
the positive peaks on the central vertical graticule line. This
line has additional calibration marks equal to 0.2 major
divisions each.
5. Count the number of divisions from the graticule line
touching the negative signal peaks to the intersection of the
positive signal peak with the central vertical graticule line.
Multiply this number by the VOLTS/DIV switch setting to
get the peak-to-peak voltage of the waveform. For example,
if the VOLTS/DIV switch were set to 2 V, the waveform
shown in Figure 2-14 would be 11.2Vp-p (5.6 div X 2V).
6. If X10 vertical magnification is used, divide the Step 5
voltage by 10 to get the correct voltage. If 10X attenuator
probes are used, multiply the voltage by 10. However, if X
10 vertical magnification and 10X attenuator probes are
used, their effects cancel and the Step 5 voltage can be used
without correction.
7. If measuring a sine wave below 100 Hz, or a rectangular
wave below 1000 Hz, flip the AC/GND/DC switch to DC.
CAUTION:
a higher-amplitude DC voltage.
Instantaneous Voltages.
proceed as follows:
1. Set up the LBO-516 for the vertical mode desired per the
instructions in 2-3 BASIC OPERATING PROCEDURES.
2. Adjust the applicable TIME/DIV switch (24) or (25) for one
complete cycle of waveform and set the VOLTS/DIV switch
for a trace amplitude of 4 to 6 divisions (see Figure 2-15).
Make certain the waveform is not riding on
To measure instantaneous voltages,
21
Page 25
3. Position the AC/GND/DC switch (16) to GND.
4. Use the appropriate vertical POSITION control (17) or
(18) to set the baseline on the central horizontal graticule line.
However, if you know the signal voltage is to be positive,use
the 0% or bottom-most graticule line. If you know the signal
voltage is to be negative, use the 100% or uppermost graticule
line.
NOTE:
The vertical POSITION controls must not be
touched again until the measurement is completed.
5. Position the AC/GND/DC switch to DC. The polarity of all
points above the ground-reference line is positive; all points
below the ground-reference line are negative.
CAUTION:
on a high-amplitude DC voltage before positioning the
AC/GND/DC switch.
6. Use the horizontal POSITION control (29) to position any
point of interest on the central vertical graticule line. This line
has additional calibration marks equal to 0.2 major divisions
each. The voltage relative to ground at any point selected is
equal to the number of divisions from that point to the ground reference line multiplied by the
Make certain the waveform is not riding
VOLTS/DIV setting. In the example used for Figure 2-15,
the voltage for a 0.5 V/div scale is 2.5 V (5.0 div X 0.5 V).
7. If XI0 vertical magnification is used, divide the Step 6
voltage by 10 to get the correct voltage. If 10X attenuator
probes are used, multiply the voltage by 10. However, if X10
vertical magnification and 10X attenuator probes are used,
their effects cancel and the Step 6 voltage can be used
without correction.
2-4-2 Differential Measurement Techniques
Differential measurement techniques allow direct mea-
surement of the voltage drop across "floating" components (both
ends above ground), and measurement of very small signals in
electrically noisy environments (such as exist near high-power AC
machinery).
The control manipulations for differential operation were
explained in paragraph
Operation.
are shown in Figure 2-16. Figure 2-16a shows the simple
technique perfectly satisfactory for measuring high-level signals
on floating signals. In this example, the AC voltage drop (ripple)
across a power choke is observed
The technique for making the physical connections
2-3-6 Additive and Differential
22
Page 26
and measured. The ground terminals from the two probes or
cables are simply connected to the chassis or ground bus of the
circuit under observation. Figure 2-16b shows the connection
technique needed for low-level signals in a noisy environment
(strong AC fields). Using a separate ground connection and
connecting the probe or cable shields to the circuit under test
avoids ground loops and EMI pickup. This setup allows fullest
utilization of the CMRR (common-mode rejection ratio) of the
LBO-516's differential facility.
2-4-3 Time Interval Measurements
The second major measurement function of the triggeredsweep oscilloscope is the measurement of time interval. This is
possible because the calibrated timebase results in each division
of the CRT screen representing a known time interval.
Basic Technique
interval is described in the following steps. This same technique
applies to the more specific procedures and variations that follow.
1. Set up the LBO-516 as described in
Operation.
2. Set the A TIME/DIV switch (24) so that the interval you
wish to measure is totally on screen and as large as possible.
Make certain the A VARIABLE control (26) is rotated fully
clockwise and detented in its CAL'D position. If the UNCAL
lamp (27) is lit, any time interval measurements made under
this position will be inaccurate.
3. Use the vertical POSITION control (17) or (18) to position
the trace so the central horizontal graticule line passes
through the points on the waveform between which you want
to make the measurement.
4. Use the horizontal POSITION controls (29) and (30) to set
the left-most measurement point on a nearby vertical
graticule line.
5. Count the number of horizontal graticule divisions between
the Step 4 graticule line and the second measurement point.
Measure to a tenth of a major division. Note that each minor
division on the central horizontal graticule line is 0.2 major
division.
6. To determine the time interval between the two measurement
points, multiply the number of horizontal divisions counted
in Step 5 by the setting of the A TIME/DIV switch. If the A
VARIABLE control (26) is pulled out (X10 MAG), be
certain to divide the TIME/DIV switch setting by 10.
Period, Pulse Width, and Duty Cycle.
described in the preceding paragraph can be used to determine
pulse parameters such as period, pulse width, duty cycle,etc.
The period of a pulse or any other waveform is the time it
takes for one full cycle of the signal. In Figure 2-17, the distance
between points (A) and (C) represent one cycle; the time interval
of this distance is the period. The time scale for the CRT display
of Figure 2-17a is 10 mS/div, so the period is 70 milliseconds in
this example.
Pulse width is the distance between points (A) and (B). In
our example it is conveniently 1.5 divisions, so the pulse
. The basic technique for measuring time
2-3-2 Single-trace
The basic technique
not
width is 15 milliseconds. However, 1.5 divisions is a rather small
distance for accurate measurements, so it is advisable to use a
faster sweep speed for this particular measurement. Increasing the
sweep speed to 2 mS/div as in Figure 2-17b gives a large display,
allowing more accurate measurement. An alternative technique
useful for pulses less than a division wide is to pull the A
VARIABLE (X10 MAG) control (26) outward, and reposition the
pulse on screen with the horizontal POSITION control (29). Pulse
width is also called
between points (B) and (C) is then called
measured in the same manner as pulse width.
When pulse width and period are known, duty cycle can be
calculated. Duty cycle is the percentage of the period (or total of
on and ofttimes) represented by the pulse width (on time).
PW(100)
Duty cycle (%) = Period = A
Duty cycle of example = 70 mS = 21.4%
Lead and Lag Time.
quency, but not the same phase, one signal is said to be
and the other
follows:
1. Set up the LBO-516 as described in
eration
and the other to the CH-2 IN connector (15).
NOTE:
compensated probes, or equal lengths of the same type
of coaxial cable to ensure equal delay times.
2. Position the trigger SOURCE selector (34) to the channel
with the leading signal (CH- 1 in the Figure 2-18 example).
3. Use the A TIME/DIV switch (24) to display the time
difference as large as possible (Figure 2-18b).
4. Use the CH- l vertical POSITION control (17) to drop the
bottom of the channel 1 trace a little below the central hori-
zontal graticule line, and the CH-2 vertical POSITION
control (18) to raise the top of the channel 2 trace a little
above the line.
5. Use the horizontal POSITION controls (29) and (30) to align
the left-most trace edge (of channel I in this case) with a
nearby vertical graticule line. The horizontal distance
between this line and the point at which the leading edge of
the other trace crosses the central horizontal graticule line
represents the time difference between the two signals. The
channel 1 signal may be said to he leading the channel 2
trace, or the channel 2 trace may be said to be lagging the
channel 1 trace, depending on the point of view.
6. Make sure the A VARIABLE timebase control (26) is ro-
tated fully clockwise and detented in its CAL'D position.
Then, count the number of horizontal divisions between the
leading edges of the traces and multiply this number by the
setting of the A TIME/DIV switch to determine the time
difference. For example, the time difference in Figure 2-18b
is l0 microseconds (5.0 div X 2/PS).
"on"
time in some applications. The distance
off
time. This can be
A
5mS X 100
When two signals have the same fre-
lagging
. To measure this lead/lag time, proceed as
, connecting one signal to the CH-1 IN connector (14)
At high frequencies use identical and correctly
>>>>
B(100)
>>>>
C
leading
2-3-5 Dual-trace Op-
1
,
23
Page 27
If the points between which the time difference exists are less
than 1 major division apart and located in the middle of complex
waveforms that are otherwise in phase, use the delayed (B)
timebase as described in
select and expand that section of the complex waveform. After
doing that, follow the same technique as described in the
preceding paragraph. As an alternative, pull the A VARIABLE
(X10 MAG) control to expand the traces, and reposition the
section with the time difference on screen with the horizontal
POSITION controls.
If the points between which the time difference exists are
more than 1 but less than 5 major divisions apart, the HighAccuracy Technique described next will yield the greatest
accuracy.
High-accuracy Techniques
complex waveform can be measured using the DLY TIME MULT
control. The linearity error of this control is only a fraction of a
percent, far less than the error possible over a small portion of the
timebase sweep.
The delay-time technique can be used with single-trace time
measurements (pulse width, period, etc.) or dual-trace
measurements (lead and lag time). The technique, after the trace
or traces are set up according to the desired procedure, is as
follows:
2-3-9 Delayed Timbase Operation
. Closely spaced points within a
to
1. Set the B TIME/DIV switch (25) to a position 50 to 100
times (5 to 6 positions) faster than the A TIME/DIV switch
setting.
2. Press the INTEN BY B HORIZ DISPLAY pushbutton (31),
then position the intensified area over the first measurement
point by means of the DLY TIME MULT control (28).
3. Press the B HORIZ DISPLAY pushbutton (31) and carefully
adjust the DLY TIME MULT control to position the first
measurement point exactly over the central vertical graticule
line. Record the DLY TIME MULT dial reading.
4. Rotate the DLY TIME MULT control to position the second
measurement point over the central vertical graticule line.
Record the DLY TIME MULT dial reading.
5. Subtract the Step 3 reading from the Step 4 reading. For
example, if the DLY TIME MULT control setting was 4.86
in Step 3, and 7.38 in Step 4, the difference is 2.51.
6. Multiply the Step 5 number by the A TIME/DIV switch
setting to find the time difference.
2.4-4 Phase Difference Measurements
Phase difference or phase angle between two signals can be
measured using the dual trace feature of the oscilloscope or by
operating the oscilloscope in the X-Y mode. When
24
Page 28
measuring phase shift of signal-processing devices, the test setup
shown in Figure 2-22 can be used.
Dual-trace Method.
waveform (sine, triangle, rectangular, complex pulse, etc.). In
fact, it will usually work even if different waveforms are being
compared. This method and its variations are effective in
measuring small or large differences in phase, at any frequency up
to 100 MHz.
To measure phase difference by the dual-trace method,
proceed as follows:
1. Set up the LBO-516 as described in
Operation,
(14) and the other to the CH-2 IN connector (15).
2. Position the trigger SOURCE selector (34) to the channel
with the cleanest and most stable trace. Temporarily move
the other channel's trace off the screen by means of its vertical POSITION control.
3. Center the stable (trigger source) trace with its vertical
POSITION control, and adjust its amplitude to exactly 6
vertical divisions by means of its VOLTS/DIV switch (10)
and VARIABLE control (11).
4. Use the LEVEL control (40) to ensure the trace crosses the
central horizontal line at or near the beginning of the sweep.
(See Figure 2-19.)
5. Use the A TIME/DIV switch (24), A VARIABLE control
(26), and the horizontal POSITION control (29) to display
one cycle of trace over 7.2 divisions. When this is done, each
major horizontal division represents 50°, and each minor
division represents 10
connecting one signal to the CH-1 IN connector
NOTE:
At high frequencies use identical and correctly
compensated probes, or equal lengths of the same type
of coaxial cable to ensure equal delay times.
This method works with any type of
2-3-5 Dual-trace
°.
25
Page 29
6. Move the off-screen trace back on the CRT with its vertical
POSITION control, precisely centering it vertically. Use the
associated VOLTS/DIV switch (10) and VARIABLE control
(11) to adjust its amplitude to exactly 6 vertical divisions.
7. The horizontal distance between corresponding points on the
waveform is the phase difference. For example, in the Figure
2-19 illustration the phase difference is 6 minor divisions, or
°.
60
You can use the X FINE control (30) to align one of the
mid-cycle zero crossings with a graticule calibration to
facilitate this measurement.
8. If the phase difference is less than 50° (one major division),
pull the A VARIABLE (X10 MAG) control (26) outwards
and use the horizontal POSITION control (if needed) to
position the measurement area back on screen. With 1 OX
magnification, each major horizontal division is 5% and each
minor division is 1
Lissajous Pattern Method.
with sine waves. Measurements are possible at frequencies up to 3
MHz, the bandwidth of the horizontal amplifier. However, for
maximum accuracy, measurements of small phase differences
should be limited to below 100 kHz.
To measure phase difference by the Lissajous pattern
method, proceed as follows:
1. Depress the X-Y switch (20).
CAUTION:
undetected spot damage the CRT phosphor.
2. Ensure that the CH-2 INV switch (19) is out. This will introduce a 180° error if pushed in.
3. Connect one signal to the CH-1 or X IN connector (14), and
the other signal to the CH-2 or Y IN connector (15).
4. Center the trace vertically with the CH-2 vertical POSITION
control (18), and adjust the CH-2 VOLTS/DIV switch (10)
and VARIABLE control (I1) for a trace height of exactly 6
divisions (the 100% and 0% graticule lines tangent to the
trace).
5. Adjust the CH- 1 VOLTS/DIV control (10) for the largest
possible on-screen display.
Precisely
6.
POSITION control (29) or X-FINE control (30).
center the trace horizontally with the horizontal
°.
This method is used primarily
Reduce the trace intensity, lest the
7. Count the number of divisions subtended by the trace along
the central vertical graticule line (dimension B in Figure 220a). You can now shift the trace vertically with the CH-2 or
Y POSITION control to a major division line for easier
counting.
T
8. The phase difference (angle
equal to the arc sine of dimension B÷A (the Step 7 number
divided by 6). For example, the Step 7 value of the Figure 220a pattern is 2.0. Dividing this by 6 yields .3334, whose arc
sine is 19.5 degrees.
9. The simple formula in Figure 2-20a works for angles less
than 90°. For angles over 90° (leftward tilt), add 90° to the
angle found in Step 7. Figure 2-20b shows the Lissajous
patterns of various phase angles; use this as a guide in de-
termining whether or not to add the additional 90
10. The sine-to-angle conversion can be accomplished by using
trig tables or a trig calculator. However, if the sine is
between 0.1 and 1.0, you can use the Figure 2-21
nomograph. Simply lay a ruler on the nomograph so its edge
passes through the cross mark and the number of divisions
measured in Step 7 (B dimension). When this is done the
edge will also intersect the phase-angle column.
2-4-5 Distortion Comparison
The dual-trace feature of the LBO-516 offers a quick method
of checking for distortion caused by a signal-processing device
(such as an amplifier). To do this, proceed as follows:
1. Connect the output of the signal generator (of frequency
suitable to the device under test) to the CH- 1 IN
connector (14) and the input of the device under test
(DUT).
2. Connect the CH-2 IN connector (15) to the output of the
device or its load (see Figure 2-22)
3. Increase the signal to the DUT until the channel 2 trace
or an RMS AC voltmeter indicates the desired output
level.
4. If the DUT has reversed the phase, press the CH-2 INV
pushbutton (19).
) between the two signals is
26
°.
Page 30
5. Superimpose the two traces with the vertical POSITION
controls (17) and (18), and use the VARIABLE VOLTS/
DIV control (11) of the larger trace to achieve the best trace
match.
6. Any
2-4-6 Frequency Measurements
frequency counter is obviously the first choice. However, an
oscilloscope can be used in either of two ways to measure
frequency when a counter is not available, or modulation and/or
noise makes the counter unusable.
Simply measure the period "t" of the unknown signal as instructed
in
frequency "f" using the formula f = 1/t. If a calculator is available,
simply enter the period and press the 1/x key. Period in seconds
(S) yields frequency in hertz (Hz); period in milliseconds (mS)
yields frequency in kilohertz (kHz); period in microseconds (PS)
yields frequency in megahertz (MHz). The accuracy of this technique is limited by the timebase calibration accuracy (see Table of
Specifications).
frequency-ratio method, the unknown frequency is compared to a
known frequency (from a calibrated signal generator). The two
signals are fed to the oscilloscope operating in its X-Y mode, and
the signal generator frequency is varied until a recognizable
Lissajous pattern appears. The pattern shape indicates the ratio
between the two frequencies. When the generator frequency is
multiplied by this ratio, the unknown frequency will be
determined. This method is usable for frequencies up to 3 MHz.
follows:
1. Set up the LBO-516 for X-Y operation (paragraph 2-3-11).
2. Connect the output of a signal generator having accurate
3. Adjust the CH- 1 VOLTS/DIV switch (10) for about 6 divi-
4. Connect the signal with the unknown frequency to the CH-2
5. Adjust the CH-2 VOLTS/DIV switch (10) for about 6 divi-
6. Vary the frequency of the signal generator until the scope
uniform horizontal
phase difference (described in paragraph 2-4-4). Any other
differences in shape indicate distortion caused by the DUT,
such as slew rate or frequency distortion, ringing, etc.
When a precise determination of frequency is needed, a
Reciprocal Method. Frequency is the reciprocal of period.
2-4-3 Time Interval Measurements
Comparison Method. In the frequency-comparison or
To measure frequency by the comparison method, proceed as
frequency calibration to the CH-1 or X IN connector (14).
sions horizontal deflection.
or Y IN connector (15).
sions vertical deflection.
display resembles a circle, an ellipse, or a diagonal line.
When this occurs the unknown frequency is the same as the
signal generator frequency (which can be read from its dial).
The accuracy of this technique depends on the signal
generator's calibration accuracy.
displacement of the traces is simply
, and calculate the
NOTE: While many other ratios are theoretically possible, drift in
either signal frequency makes more complex Lissajous patterns
nearly impossible to read.
2-4-7 Risetime Measurement
Risetime is the time required for the leading edge of a pulse
to rise from 10% to 90% of the total pulse amplitude. Falltime is
the time required for the trailing edge of a pulse to drop from 90%
of total pulse amplitude to 10%. Risetime and falltime, which may
be collectively called transition time, are measured in essentially
the same manner.
To measure rise and fall time, proceed as follows:
1. Connect the pulse to be measured to the CH- 1 IN connector
(14) and set the AC/GND/DC switch (16) to AC.
2. Adjust the A TIME/DIV switch (24) to display about 2 cycles
of the pulse. Make certain the associated VARIABLE control
(11) is rotated fully clockwise and de-tented in its CAL'D
position.
3. Center the pulse vertically with the channel 1 vertical
POSITION control (17).
4. Adjust the channel 1 VOLTS/DIV switch (10) to make the
positive pulse peak exceed the 100% graticule line, and the
negative pulse peak exceed the 0% line, then rotate the
VARIABLE control (11) counterclockwise until the positive
and negative pulse peaks rest exactly on the 100% and 0%
graticule lines. (See Figure 2-23).
5. Use the horizontal POSITION (29) and X-FINE (30) controls
to shift the trace so the leading edge passes through the
intersection of the 10% and central vertical graticule lines.
6. If the risetime is slow compared to the period, no further
control manipulations are necessary. If the risetime is fast
(leading edge almost vertical), pull the A VARIABLE (X10
MAG) control (26) and reposition the trace as in Step 5. (See
Figure 2-23b.)
7. Count the number of horizontal divisions between the central
vertical line (10% point) and the intersection of the trace with
the 90% line.
8. Multiply the number of divisions counted in Step 7 by the
setting of the A TIME/DIV switch to find the measured
risetime. If Xl0 magnification was used, divide the
TIME/DIV setting by 10. For example, if the A timebase
setting in Figure 2-23 was .1/PS (100 KS), the risetime would
be 36 nanoseconds (100 KS ÷ 10 = 10 KS; 10 KS x 3.6 div =
36 KS).
9. To measure falltime, simply shift the trace horizontally until
a trailing edge passes through the 10% and central vertical
graticule lines, and repeat Steps 7 and 8.
10. The rise and fall times measured thus far include the 3.5 KS
transition times of the LBO-516 (about 5 KS with probe).
These errors are negligible if the measured rise and fall times
are 20 KS or longer. For shorter transition times, correct the
measured rise and fall times using one of the following
formulas:
27
Page 31
2-4-8 -- 3 dB Bandwidth Measurement
Bandwidth measurement usually involves finding the -3 dB
response point in the frequency-response curve of a circuit or
device. This can easily be determined without the need for
calculations or dB conversions by using the following "trick":
1. Connect the output of a constant-amplitude signal generator
(of appropriate frequency range) to the input of the de-vice-
under test (DUT). Connect the output of the DUT to the
CH-1 IN connector (14).
2. Set the generator to a frequency
the DUT, then adjust the generator output level to produce
the desired DUT output level.
3. Set the CH-1 VOLTS/DIV control (10) to the
that produces
4. Use the CH-1 VARIABLE VOLTS/DIV control (11) and
CH-1 vertical POSITION control (17) to make the trace
height
and bottom-most graticule lines.
5. Increase the generator frequency until the trace height de-
creases to exactly 5 divisions. This is the upper -3 dB re-
sponse point. The frequency can be determined from the
signal-generator dial, or with a frequency counter connected
to the CH-1 OUTPUT connector (13).
6. Restore the generator to its Step 2 frequency, then decrease
the generator frequency until the trace height decreases to
exactly 5 divisions. This is the lower -3 dB response point.
over 7 divisions
exactly
7 divisions, and touching the second highest
well within
trace height.
the passband of
highest setting
28
Loading...
+ hidden pages
You need points to download manuals.
1 point = 1 manual.
You can buy points or you can get point for every manual you upload.