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Attenuating the input signal extends the common mode
range by the same factor as the attenuation. Pressing the
+10 ATTENUATOR button increases the common mode
range to ±155 volts, and using a probe with a +10 attenuation factor will too. The effect of the internal ÷10 AT-
TENUATOR and the attenuation factor of probes is multi-
plied just as the signal is attenuated. For example, using
the amplifier’s ÷10 ATTENUATOR with a probe having a
+100 attenuation factor (total attenuation of + 1000) results
in a common mode range of 15,500 volts. In this case, the
probe’s maximum voltage rating probably limits the maxi-
mum common mode input voltage.
The gain setting of the amplifier has no effect on common
mode range; it is the same in XI0 GAIN as it is in XI.
When making measurements on circuits that are line referenced, use enough total attenuation to keep the peak voltage at the amplifier input below 15.5 volts. The US
power-line can exceed 170 peak volts and therefore at
least a total attenuation of ÷100 should be used. Line
voltages in some other countries are larger but their peak
voltages do not exceed the 1550 volt common mode range
that a +100 attenuation factor provides.
MOVING THE OSCILLOSCOPE POSITION SETTING
AWAY FROM CENTER SCREEN
When operating the 1850A/1855A with a scope, it is very
important to set the oscilloscope’s position and/or offset
control to center screen, There are a couple of reasons for
this.
First, the linear portion of the 1850A/1855A’s ±500mV
output range is centered around zero volts. As the
1850A/1855A approaches its limits, the output signal will
be distorted. Moving the oscilloscope’s position control
way from center screen can allow these distortions to
appear on the oscilloscope’s screen where they may be
mistaken for part of the displayed signal.
Second, proper operation of the 1855A’s Precision Voltage
Generator (PVG) depends on the operator knowing the
location of zero volts on the display. The readout in the
PVG is designed to display the voltage of the signal as it
crosses the center line of the oscilloscope screen. If the
oscilloscope’s position or offset control has been moved,
incorrect readings could result.
When the 1855A is controlled with the ProBus interface
(using the REMOTE connector on the 1850A/1855A rear
panel), the offset control on the oscilloscope controls the
1855A PVG. The PVG display will read the offset set from
the oscilloscope front panel.
When the 1850A is controlled with the ProBus interface, an
external source must be used to control the vertical trace
position:
03/10/99
General Operating Information -- 1850A11855A
USING SCOPE AT GREATER THAN 50mV/div (e.g.
200m V/div)
"I know the input to the 1850A/1855A is a sinewave, but I
am seeing a squarewave on the oscilloscope." This comment is the result of the operator setting the oscilloscope
sensitivity to something less than 50mV/div. If the oscilloscope sensitivity ’is set to 200mV/div, the 1850A/1855A
will limit at 2%_ divisions above and below center screen
(zero volt point if the oscilloscope’s position control is
properly set). Thus, a sinewave large enough to overdrive
the 1850A/1855A will appear as a squarewave on the os-
cilloscope.
The 1850A/1855A is designed to cleanly limit the output
signal to ±500inV. The 1850A/1855A is designed to recover very quickly once its input signal level decreases
sufficiently to allow the amplifier to return to its linear
range. The 1850A/1855A will recover from overdrive to
its full accuracy much more quickly than most oscillo-
scopes.
If the 1850A/I 855A did not limit the signal at +_.500mV, it
would be of no help to the oscilloscope in viewing large
signals.
Keeping the oscilloscope’s position at center screen and
using oscilloscope sensitivities between 50mV/div and
l mV/div (or the oscilloscope’s most sensitive setting) will
insure good signal integrity. When the displayed signal
contains mostly low frequency components, the operator can use the oscilloscope’s 100mV/div setting to allow
large signals to he completely shown on screen.
FAILURE TO TERMINATE THE AMPLIFIER IN 50
OHMS
"All the signals displayed on my oscilloscope seem to be
twice as large as they should be." This comment results
from not having the output of the 1850A/1855A properly
terminated into 50 ohms. The 1850A/1855A output impedance is 50 ohms. The cable connecting the
1850A/1855A to the oscilloscope or spectrum analyzer
should be 50 ohms and be terminated with a 50 ohm load.
If the termination at the end of the connecting coaxial cable
is missing, the amplifier will not be properly terminated.
Several things occur if the external termination is missing.
First, the output isn’t properly terminated for all frequencies resulting in poor frequency and transient response. For
most signals this distortion will be minor, except when the
1855A’s 1 MHz and 20 MHz bandwidth limit filters are
used. These filters will ring when not properly terminated.
Failure to use a 50 ohm coaxial cable will adversely affect
the transient response of the 20MHz filter even though the
termination impedance is 50 ohms.
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