2.2.1 Open and Short Calibration...........................................................................................................................................................13
2.2.3 Range Hold....................................................................................................................................................................................13
2.2.4 DC Resistance Measurement........................................................................................................................................................14
2.2.5 AC Impedance Measurement........................................................................................................................................................14
The B&K Precision Corp. 889A Synthesized In-Circuit LCR/ESR Meter is a high accuracy test instrument used
for measuring inductors, capacitors and resistors with a basic accuracy of 0.1%. Also, with the built-in functions of
DC/AC Voltage/Current measurements and Diode/Audible Continuity checks, the 889A can not only help
engineers and students to understand the characteristics of electronics components but also being an essential
tool on any service bench.
The 889A is defaulted to auto ranging. However, it can be set to auto or manual ranging by pressing the Range Hold key. When LCR measurement mode is selected, one of the test frequencies, 100 Hz, 120 Hz, 1 KHz, 10
KHz, 100 KHz or 200 KHz, may be selected on all applicable ranges. One of the test voltages, 50mVrms, 0.25
Vrms, 1 Vrms or 1 VDC (DCR only), may also be selected on all applicable ranges. The dual display feature
permits simultaneous measurements. When DC/AC voltage/current measurement mode or the Diode/Audible
Continuity Check mode is selected, only the secondary display will be used to show the result of the
measurement.
The highly versatile 889A can perform virtually all the functions of most bench type LCR bridges. With a basic
accuracy of 0.1%, this economical LCR meter may be adequately substituted for a more expensive LCR bridge in
many situations. Also, with the basic accuracy of 0.4% in voltage and current measurements, the 889A performs
the functions of a general purpose Digital Multi-Meter and can be used to replace the DMM on a service bench.
The 889A has applications in electronic engineering labs, production facilities, service shops, and schools. It can
be used to check ESR values of capacitors, sort and/or select components, measure unmarked and unknown
components, and measure capacitance, inductance, or resistance of cables, switches, circuit board foils, etc.
The key features are as following:
1. Voltage Measurements:
l AC : True RMS, up to 600Vrms @ 40 ~ 1K Hz
l DC : up to 600V
l Input Impedance : 1M-Ohm
2. Current Measurements:
l AC : True RMS, up to 2Arms @ 40 ~ 1K Hz
l DC : up to 2A
l Current Shunt : 0.1 Ohm @ > 20mA; 10 Ohm @ ≤ 20mA
3. Diode/Audible Continuity Checks:
l Open Circuit Voltage: 5Vdc
l Short Circuit Current: 2.5mA
l Beep On: ≤ 25 Ω
l Beep Off: ≥ 50 Ω
l Measurement Parameters : Z, Ls, Lp, Cs, Cp, DCR, ESR, D, Q and ?
l Basic Accuracy : 0.1%
l Dual Liquid Crystal Display
l Auto Range or Range Hold
l RS-232 Interface Communication
l Open/Short Calibration
l Primary Parameters Display:
Z : AC Impedance
DCR : DC Resistance
Ls : Serial Inductance
Lp : Parallel Inductance
Cs : Serial Capacitance
(
)
Ω∠=+=
θ
(
)
θ
I
maginary Axis
Real Axis
Figure 1.1
Cp : Parallel Capacitance
l Second Parameter Display:
? : Phase Angle
ESR : Equivalence Serial Resistance
D : Dissipation Factor
Q : Quality Factor
l Combinations of Display:
Serial Mode : Z –?, Cs – D, Cs – Q, Cs – ESR, Ls – D, Ls – Q, Ls – ESR
Parallel Mode : Cp – D, Cp – Q, Lp – D, Lp – Q
1.2 Impedance Parameters
Due to the different testing signals on the impedance measurement instrument, there are DC and AC
impedances. The common digital multi-meter can only measure the DC impedance, but the 889A can do both. It
is very important to understand the impedance parameters of the electronic components.
When we analysis the impedance by the impedance measurement plane (Figure 1.1), it can be visualized by the
real element on the X-axis and the imaginary element on the y-axis. This impedance measurement plane can
also be seen as the polar coordinates. The Z is the magnitude and θ is the phase of the impedance.
X
s
Z
R
s
Z
jX
RZ
R
s
X
s
s
s
θ
()
Impedance
=
Z
()
Resistance
=
R
S
()
Reactance
=
X
S
()
Ohm
=Ω
sX,RZ
s
22
+==
RZCosZ
s
−
1
==
TanSinZ
θθ
X
s
X
s
R
s
There are two different types of reactance: Inductive (XL) and Capacitive (XC). It can bedefined as follows:
X
L
X
C
fLL
πω
2====
11
fCC
πω
2
L = Inductance (H)
C = Capacitance (F)
f = Frequency (Hz)
Also, there are Quality factor (Q) and the Dissipation factor (D) that need to be discussed. For component, the
Quality factor serves as a measurement of the reactance purity. In the real world, there is always some
associated resistance that dissipates power, decreasing the amount of energy that can be recovered. The Quality
factor can be defined as the ratio of the stored energy (reactance) and the dissipated energy (resistance). Q is
generally used for inductors and D for capacitors.
Figure 1.2
Real and imaginary components are serial
+
=
Real and imaginary components are parallel
G=1/R
jB=1/jX
jB
+
=
jXp R
Q
D
X
B
=
G
11
==
δ
tan
L
ω
s
R
s
R
p
X
p
s
R
s
R
p
L
ω
p
1
===
C
ω
===
sRs
R
C
ω
p
p
There are two types of the circuit mode, the series mode and the parallel mode. See Figure 1.2 to find out the
relationship of the series and parallel modes.
Rs jX
s
p
p
jXRZ
ss
1
1
Y+=
jX
R
P
P
p
GY
1.3 Specification
lMeasuring Range:
Parameter Range
Z 0.000 Ωto 500.0 MΩ
L 0.030 µH to 9999 H
C 0.003 pF to 80.00 mF
DCR 0.000 Ω to 500.0 MΩ
ESR 0.000 Ω to 9999 Ω
D 0.000 to 9999
Q 0.000 to 9999
? -180.0 ° to 180.0 °
Voltage/Current Measurements
V 0.0 mV to +/- 600 V
A 0.000 mA to +/- 2 A
lAccuracy (Ae):
1. DC Voltage Measurement:
Range : 2V, 20V, 200V, and 600V
Resolution : 1mV, 10mV, 100mV, and 1V
Accuracy : +/- (0.4% + 3 digits)
Input Impedance : 1 M-Ohm
2. AC Voltage Measurement (True RMS):
10M
Range : 2V, 20V, 200V, and 600V
Resolution : 1mV, 10mV, 100mV, and 1V
Accuracy : +/- (0.8% + 5 digits)
Input Impedance : 1 M-Ohm
3. DC Current Measurement:
Range : 2mA, 20mA, 200mA, and 2000mA
Resolution : 1uA, 10uA, 100uA, and 1mA
Accuracy : +/- (0.4% + 3 digits)
Current Shunt : 0.1 Ohm @ >20mA, 10 Ohm @ ≤20mA
4. AC Current Measurement (True RMS):
Range : 2mA, 20mA, 200mA, and 2000mA
Resolution : 1uA, 10uA, 100uA, and 1mA
Accuracy : +/- (0.8% + 5 digits)
Current Shunt : 0.1 Ohm @ >20mA, 10 Ohm @ ≤20mA
Note:
The accuracy of DC/AC voltage/current measurements is only applied when in 5% - 100% of the range.
CAe = Ae of C
f : Test Frequency (Hz)
Cx : Measured Capacitance Value (F)
|Zx| : Measured Impedance Value (Ω)
Accuracy applies when Dx (measured D value) ≤ 0.1
When Dx > 0.1, multiply CAe by
Example:
Test Condition:
Frequency : 1KHz
Level : 1Vrms
DUT : 100nF
Then
=
Zx
=
π
Refer to the accuracy table, get CAe=±0.1%
L Accuracy:
LAe = Ae of L
f : Test Frequency (Hz)
Lx : Measured Inductance Value (H)
|Zx| : Measured Impedance Value (Ω)
Accuracy applies when Dx (measured D value) ≤ 0.1
1
πCxf
⋅⋅⋅
2
1
−
3
102
9
⋅⋅⋅⋅
10100
LxfZx⋅⋅⋅=π2
1590
1Dx+
Ω=
2
When Dx > 0.1, multiply LAe by
Example:
Test Condition:
Frequency : 1KHz
Level : 1Vrms
DUT : 1mH
Then
⋅⋅⋅=
πLxfZx
−
3
3
⋅⋅⋅=
10
Refer to the accuracy table, get L
1022π
Ω=
283.6
1Dx+
= ±0.5%
Ae
2
ESR Accuracy:
100
100
100
100
Ae
ESR⋅±=
Ae
ESRAe = Ae of ESR
f : Test Frequency (Hz)
Xx : Measured Reactance Value (Ω)
Lx : Measured Inductance Value (H)
Cx : Measured Capacitance Value (F)
Accuracy applies when Dx (measured D value) ≤ 0.1
Example:
Test Condition:
Frequency : 1KHz
Level : 1Vrms
DUT : 100nF
Xx
2
Then
=
Zx
=
Refer to the accuracy table, get
CAe=±0.1%,
ESR
Ae
D Accuracy:
D±=
Ae
DAe = Ae of D measurement value
Accuracy applies when Dx (measured D value) ≤ 0.1
When Dx > 0.1, multiply Dx by (1+Dx)
Example:
Test Condition:
Frequency : 1KHz
Level : 1Vrms
DUT : 100nF
1
πCxf
102
3
Ae
1
Xx
⋅⋅⋅
1590
−
9
⋅⋅⋅⋅
10100
Ae
Ω=
Ω±=⋅±=59.1
2
π
LxfXx
=⋅⋅⋅=ππ
1
Cxf
2
⋅⋅⋅
Then
=
Zx
=
Refer to the accuracy table, get
CAe=±0.1%,
D
Ae
1
πCxf
102
⋅⋅⋅
1
3
Ae
⋅⋅⋅⋅
10100
±=⋅±=
1590
−
9
002.0
2
π
Ω=
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