Keithley 2182A/E Digital-Multimeter, DMM, 2182A/E Datenbogen
Produktcode
2182A/E
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www.keithley.com
1.888.KEITHLEY
(U.S. only)
A Greater Measure of Confidence
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optional accessory: Model 2187-4 low Thermal
Test lead Kit
The standard cabling provided with the Model
2182A Nano volt meter and Model 622X Current
Sources provides everything normally needed
to connect the instruments to each other and to
the DUT . The Model 2187-4 Low Thermal Test
Lead Kit is required when the cabling provided
may not be sufficient for specific applications,
such as when the DUT has special connection
requirements . The kit includes an input cable
with banana terminations, banana extensions,
sprung-hook clips, alligator clips, needle probes,
and spade lugs to accommodate virtually any
DUT . The Model 2187-4 is also helpful when the
DUT has roughly 1G
W impedance or higher .
In this case, measuring with the Model 2182A
directly across the DUT will lead to loading
errors . The Model 2187-4 Low Thermal Test Lead Kit provides a banana cable and banana jack
extender to allow the Model 2182A to connect easily to the Model 622X’s low impedance guard
output, so the Model 2182A can measure the DUT voltage indirectly . This same configuration also
removes the Model 2182A’s input capacitance from the DUT, so it improves device response time,
which may be critical for pulsed measurements .
Three Ways to Measure Nanovolts
DC nanovoltmeters. DC nanovoltmeters
DC nanovoltmeters. DC nanovoltmeters
and sensitive DMMs both provide low noise
DC voltage measurements by using long
integration times and highly filtered readings
to minimize the bandwidth near DC .
Unfortunately, this approach has limitations,
particularly the fact that thermal voltages
develop in the sample and connections vary,
so long integration times don’t improve
measurement precision . With a noise
specification of just 6nV p-p, the Model 2182A
is the lowest noise digital nanovolt meter
available .
AC technique. The limitations of the long
integration and filtered readings technique
have led many people to use an AC technique
for measuring low resistances and voltages .
In this method, an AC excitation is applied
to the sample and the voltage is detected
syn chronously at the same frequency and
an optimum phase . While this technique
removes the varying DC component, in many
experiments at high frequencies, users can
experience problems related to phase shifts
caused by spurious capacitance or the L/R
time constant . At low frequencies, as the
AC frequency is reduced to minimize phase
shifts, amplifier noise increases .
The current reversal method. The Model
2182A is optimized for the current reversal
method, which combines the advantages of
both earlier approaches . In this technique,
the DC test current is reversed, then the
difference in voltage due to the difference
in current is determined . Typically, this
measure ment is performed at a few hertz (a
frequency just high enough for the current
to be reversed before the thermal voltages
can change) . The Model 2182A’s low noise
performance at measurement times of a
few hundred milliseconds to a few seconds
means that the reversal period can be set
quite small in comparison with the thermal
time constant of the sample and the con-
nections, effectively reducing the impact of
thermal voltages .
180
185
190
195
200
205
210
215
220
0
8
17 25 33 42 50 58 67 75 83 92 100 108 117 125
Voltage
(nV)
Temperature
(
°C)
Minutes
–10
–5
0
5
10
15
20
25
30
figure 5. The Model 2182a’s delta mode provides extremely stable results, even in the pres-
ence of large ambient temperature changes. In this challenging example, the 200nV signal
results from a 20µa current sourced by a Model 6221 through a 10m
W test resistor.
2182a
Nanovoltmeter
figure 7. Model 2182a rear panel
figure 6. Model 2187-4 Test lead Kit