March 1983
Thanks to John Day who provided this scanned copy
Title & Document Type:
Manual Part Number:
Revision Date:
HP References in this Manual
This manual may contain references to HP or Hewlett-Packard. Please note that HewlettPackard's former test and measurement, semiconductor products and chemical analysis
businesses are now part of Agilent Technologies. We have made no changes to this
manual copy. The HP XXXX referred to in this document is now the Agilent XXXX.
For example, model number HP8648A is now model number Agilent 8648A.
About this Manual
We’ve added this manual to the Agilent website in an effort to help you support your
product. This manual provides the best information we could find. It may be incomplete
or contain dated information, and the scan quality may not be idea l. If we find a better
copy in the future, we will add it to the Agilent website.
Support for Your Product
Agilent no longer sells or supports this product. You will find any other available
product information on the Agilent Test & Measurement website:
www.tm.agilent.com
Search for the model number of this product, and the resulting product page will guide
you to any available information. Our service centers may be able to perform calibration
if no repair parts are needed, but no other support from Agilent is available.
MET6LoGY
JAN 21 1986
thERATING
i
.
AND
SERVICE MANUAL
434.2A.
HEWLETT
I?!!
PACKARD
COPYRIGHT AND DISCLAIMER NOTICE
Copyright - Agilent Technologies, Inc. Reproduced with the permission of Agilent
Technologies Inc. Agilent Technologies, Inc. makes no warranty of any kind with regard
to this material including, but not limited to, the implied warranties of merchantability
and fitness for a particular purpose. Agilent Technologies, Inc. is not liable for errors
contained herein or for incidental or consequential damages in connection with the
furnishing, performance, or use of this material or data.
CERTI FI CATI 0 N,
The Hewlett-Packard Company certifies that this instrument was
thoroughly tested and inspected and found to meet its published
specifications when it was shipped
Packard -Company further
ments are traceable to the U.S. National Bureau
the extent allowed by the Bureau’s calibration facility.
certifies
from
the factory. The Hewlett-
that its calibration meusure-
of
Standards to
WARRANTY AND ASSISTANCE
All Hewlett-Packard products are warranted against defects in
materials and workmanship. This warranty applies for one year
from the date of delivery, or, in the case of certain major compo-
nents listed in the operating manual, for the specified period. We
will repair or replace products which prove to be defective during
the warranty period provided they are returned to Hewlett-
Packard. No other warranty is expressed or implied. We are not
liable for consequential damages.
Service contracts or customer assistance agreements are available
for Hewlett-Packard products that require maintenance and re-
pair on-site.
For any assistance, contact your nearest Hewlett-Packard Sales and
Service Office. Addresses are provided at the back of this manual.
OPERATING AND SERVICE
MODEL 4342A
Q METER
SERIAL NUMBERES COVERED
This manual applies directly to Model 43428 Q Meter
with serial prefixed 12125. Backdating changes in
SectionVII cover instruments with serials 12125-00590
and below. Instruments with higher serial prefix will
be covered in an Updating Manual Supplement at the
first of the manual.
MANUAL
This manual cover-es Option 001 instruments as well
as the standard instrument.
aCOPYRIGHT: YOKOGAWA-HEWLETT-PACKARD, LTD., 1970
9-1, TAKAKURA-CHO, HACHIOJI-SHI, TOKYO, JAPAN
Manual Part No. 04342-90009
Microfiche Part No. 04342-90059
laboratory, on the production line, or in QA
incoming inspection areas. The direct read-
ing,expanded scale of the 4342.4 permits measurement of Q from 5 to 1000 and the reading
of very small changes in Q resulting from
variation in test parameters. The long frequency dial scale and the pushbutton range
selector continuously cover the frequency
range of 22kHz to 7OPlHz (in seven - l/3 de-
cade steps) and permit setting the frequency
to an accuracy of 1.5% with 1% resolution.
The calibrated long-scale capacitance dials
permit reading the capacitance of the
tuning capacitor at an accuracy of 1% and
provides the capability for varying the
capacitance with O.lpF resolution on the
vernier scale. Inductance of sample can be
read directly from the inductance scale ad-
jacent to the capacitance scale at seven
specific frequencies by setting the frequency
dial to the "L" point on each frequency range.
Flat oscillator output, automatically levelcontrolled over the entire frequency ranges,
is a feature of the 4342A.
This advantage
obviates the necessity for frequent oscil-
lator level adjustments to maintain the out-
put level constant or the use of a
specially
matched fragile thermocouple level meter.
The high reliability of the instrument and
ease of operation are the direct results of
these measurement advancements in the 4342A.
For determing the resistance, reactance, or
quality factor of capacitance and inductance
samples in the high frequency region, the
4342A is a most versatile measuring instru-
ment. The 4342,1 can measure the dissipation
factor and dielectric constant of insulating
materials, coefficient of coupling, mutual
inductance, and the frequency characteristics
of transformers. Accessories which extend
the measurement capabilities, designed for
Figure l-l. Model 4342A Q Meter.
Section I
Paragraphs 1-3 to l-12
Model 4342A
user convenience, have broad applications
in testing components and electronic materials, in physical and chemical research, and
in related scientific fields.
Pushbutton operation of frequency range and
Q/AQ range selection provides for straight-
forward measurement.
meter scales,
multipliers are used,
and reading speed.
l-3. How The 4342A Measures.
l-4. The Q Meter is basically composed of a
stable, variable oscillator, a tuning circuit
for taking resonance with an unknown sample,
and a high input impedance RF voltmeter connected across the variable capacitor which is
a section of the tuning circuit.
To measure the quality factor of a sample, a
stable oscillator signal is injected into the
series tuning circuit composed of the vari-
able capacitor and the unknown (inductor).
At the tuned frequency, the RF voltmeter
(called Q voltmeter) indicates a peak value
in the signal level increase (resonance) and
is proportional to the quality factor of the
sample measured.
signal with a low output impedance and by
measuring the signal level of the series re-
sonant circuit with a high impedance volt-
meter, the quality factor of the unknown
samnle can be accurately determined at the
resonant frequency.
parameters of the sample can be measured
(directly and indirectly) as factors of the
resonant frequency and the tuning capacity
which can be read from their respective dial
scales.
l-5. For accurate measurements, the 4342A
employs a unique constant voltage injection
system and a low output impedance injection
transformer. The oscillator signal is automatically leveled by an ALC loop to provide
the constant injection voltage required by
the Q range in use.
of an oscillator level control or the fragile
thermocouple level meter (as used in tradi-
tional Q Meters).
transformer along with the high quality low
loss tuning capacitor contribute minimal additional loss to the measurement circuit (resonant circuit) and greatly improve the Q ac-
curacy in high Q measurements.
l-6. High stability of the Q voltmeter virtually eliminates the need for Q-zero adjustments in routine measurements. Troublesome
zero settings prior to each adjustment are
thus eliminated, ensuring simple and rapid operation. Accurate determination of Q changes
l-2
frequency dials, and frequency
Automatic indication of
adding to the simplicity
By injecting an oscillator
Additionally, various
This obviates the need
The unique injection
in delta-Q measurements can be obtained in all
Q ranges by using the expanded resolution
(X10) capability.
l-7. The unique Q Limit selector is especially useful in Go/No-Go checking on the
production line. The high response speed of
the Go/No-Go indicator (compared to using a
meter pointer deflection method) permits
faster Go/No-Go testing. For even easier
testing, external indicating devices may be
remotely controlled by the Go/No-Go output
signal (on the rear panel).
1-8. INSTRUMENTS COVERED BY MANUAL.
l-9. Hewlett-Packard uses a two-section
nine character serial number which is marked
on the serial number plate (Figure 1-2) attached to the instrument rear panel.
first four digits and the letter are the serial prefix and the last five digits are the
suffix. The letter placed between the two
sections identifies country where instrument
was manufactured.
all identical instruments; it changes only
when a change is made to the instrument.
suffix, however,
and is different for each instrument.
contents of this manual apply to instruments
with the serial number prefix(es) listed
under SERIAL NUMBERS on the title page.
l-10. An instrument manufactured after the
printing of this manual may have a serial
number prefix that is not listed on the title
page.
dicates that the instrument is different from
those described in this manual. The manual
for this new instrument may be accompanied by
a yellow Manual Changes supplement or have a
different manual part number. This supplement contains
plains how to adapt the manual to the newer
instrument.
l-11. In addition to change information, the
supplement may contain information for correcting errors (called Errata) in the manual.
To keep this manual as current and accurate
as possible, Hewlett-Packard recommends that
you periodically request the latest Manual
Changes supplement. The supplement for this
manual is identified with this manual's title
page.
are available from ltewlett-Packard. If the
serial prefix or number of an instrument is
lower than that on title page of this manual,
see Section VII Manual Changes.
1-12.
number prefix that is not listed on the title
page or in the Manual Changes supplement,
contact your nearest Hewlett-Packard office.
This unlisted serial number prefix in-
Complimentary copies of the supplement
For information concerning a serial
The prefix is the same for
is assigned sequentially
"change information" that ex-
The
The
The
Model 4342A
Paragraphs l-13 to l-22
Section I
1-13. SPECIFICATIONS.
1-14. Complete specifications of the Model
4342A Q Meter are given in Table l-1. These
specifications are the performance standards
or limits against which the instrument is
tested. The test procedures for testing the
instrument to determine if it meets its specifications are covered in Section V Mainte-
nance Paragraph 5-9 Performance Checks.
When the 4342A Q Meter is shipped from the
factory, it meets the specifications listed
in Table l-l.
l-15. ACCESSORIES SUPPLIED.
1-16. Fuses (HP Part No. 2110-0339 and 2110-
0044), the Operating and Service Manual, and
a power cord are furnished with the 4342A.
One of four types of power cords (HP Part No.
8120-1703, -0696, -1692 or -1521) is fur-
nished depending on the instrument destin-
ation. All accessories supplied are packed
in the instrument carton.
l-17. ACCESSORIES AVAIALABLE.
l-18.
devices which extend or enhance the measure-
ment capabilities of the 4342A.
ing accessories are available for use with
the 4342A Q Meter:
Accessories are specially designed
The follow-
16014A Series Loss Test Adapter:
The 16014A Series Loss Test Adapter is
a special terminal adapter designed
for measuring low impedance components,
low-value inductors and resistors, and
also high value capacitors.
adapter adds convenience in connecting
components in series with the test
circuit of the 4342A Q Meter.
sists of a teflon printed-circuit
base on which are mounted binding
posts to accept the supplemental inductors,
series terminals for the unknown.
16451A Dielectric Test Adapter (4342A-KOl):
The 16451A Dielectric Test Adapter is
a test fixture for measuring the dielectric constant or dielectric loss
angle (tan 6) of insulating materials.
The 16451A has a pair of precision
variable electrodes (one side is fixed)
which hold the sample and which op-
erate similar to a micrometer to per-
mit direct reading of electrode spac-
ing. This test adapter is directly
attached to 4342A measurement
terminals.
Typical performance, characteristics, and additional information regarding these accessories are given in Table l-2.
and a pair of low-inductance
The
It con-
16470 Series Supplemental Inductors:
A range of 20 inductors (model num-
bers 16471A to 1649OA), which can be
supplied separately or as a set, are
available for use with the 4342A Q
Meter.
reference devices when measuring the
RF characteristics of capacitors, re-
sistors, or insulating materials.
4342A option 001 instruments, the
Model 16465A Inductor is additionally
available.
terminals including a guard terminal
for stabilization of measurements.
16462A Auxiliary Capacitor:
The 16462A Auxiliary Capacitor is de-
signed to extend the Q and L measurement capabilities of the 4342A. It is
especially useful when measuring small
inductors at low frequencies.
These inductors are useful as
These inductors have three
For
1-19. OPTIONS.
l-20. An option is a standard modification
performed in the instrument to meet a special
requirement desired by a user.
strument model is ordered with an option number, the corresponding optional parts are
installed in/or packaged with instrument at
the factory.
lower measurement frequency range is avail-
able for installation in the 4342A.
l-21.
l-22.
frequency range, 1OkHz to 32MHz, instead of
the standard frequency range of 20kHz to
70MHz. All specifications that apply to Option 001 instruments are given in Table 1-1.
Option 001.
The 4342A Option 001 covers a lower
An Option for obtaining a
When an in-
1-3
Section I
Table l-l
Model 4342A
Table l-1. Specifications (Sheet 1 of 2).
FREQUENCY CHARACTERISTICS
Measurement Frequency Range:
22kHz to 70MHz in 7 bands (22 to
70kHz, 70 to 220kHz,
700 to 2200kHz, 2.2 to 7MHz, 7 to
22MHz, and 22 to 70MHz).
Frequency Dial Accuracy:
21.5% at 22kHz to 22MHz,
22%
at 22MHz to 70MHz,
-cl%
at "L" point on frequency dial.
Frequency Dial Resolution:
Approximately 21%.
Q MEASUREMENT CHARACTERISTICS
Q Range:
5 to 1000 in
to 100, 50 to 300, and 200 to 1000).
Q Tolerance:
quency 22kHz - 30MHz 30MHz - 70MHz
:
5 - 300
300 - 600
600 - 1000
Q Resolution:
Upper scale: 1 from 20 to
Lower scale: 0.5 from 5 to
AQ Range:
0 to 100 in 4 ranges, 0 to 3, 0 to
10, 0 to 30, 0 to 100.
4 ranges (5 to 30, 20
% of indicated value
(at 25'C)
27% 210%
210% 215%
215% ?20%
220 to 700kHz,
100,
30.
AQ Tolerance:
210% of full scale.
AQ Resolution:
Upper scale:
Lower scale:
I
NDUCTANCE MEASUREMENT CHARACTERISTICS
L Range:
0.09nH to 1.2H, direct reading for
seven specific frequencies as marked
at the frequency dial "L" scale point
and selected by the frequency range
switches.
L Accuracy:
?3%
after compensation for residual
inductance (approx. 1OnH).
TUNING CAPACITOR CHARACTERISTICS
Capacitance Range:
Main dial capacitor: 25 to 470pF
Vernier dial capacitor:
Capacitance Dial Accuracy:
Main dial: *l% or 1pF whichever is
Vernier dial: +O.lpF.
Capacitance Resolution:
Main dial: 1pF from 25 to 30pF,
Vernier d ial: O.lpF.
0.1 from 0 to 10,
0.05 from 0 to 3.
-5 to +5pF
greater.
2pF from 30 to 200pF,
5pF from 200 to 470pF.
1
l-4
Model 4342A Section I
Table l-1
Table 1-l.
REAR PANEL OUTPUTS
Frequency Monitor:
17OmVrms min. into SOR.
Q Analog Output:
1V +-50mV dc at full scale, proportional to meter deflection, output
impedance approx. 1kR.
Over Limit Signal Output:
Single pole relay contact output,
one side grounded, relay contact
capacity 0.5.4/15VA.
Over Limit Display Time:
Switch-selectable, lsec. or
continuous.
GENERAL
Operating Temperature Range:
o"c to 50°C.
Warm-up Time: 30 minutes.
Power: 115 or 230V +lO%,
approx. 25VA.
Weight: Approx. 31 lbs (
Specifications (Sheet 2 of 2).
48 - 440Hz,
4kd.
OPTION 001:
This option covers a frequency range
of 10kHz to 32MHz. Specifications
are identical with those of the
standard model except as noted below.
Oscillator Frequency Range:
1OkHz to 32MHz in 7 bands (10 to
32kHz, 32 to lOOkf-Iz, 100 to 320kHz,
320 to lOOOkHz, 1 to 3.2MHz, 3.2 to
IOMHz, and 10 to 32MHz).
Frequency Accuracy:
i-1.5%
at 1OkHz to 1OMllz.
+_2% at 1OMllz to 32MHz.
21% at "L" point on frequency dial.
Q Tolerance: % of indicated value
(at 25'C)
1 5 - 300 1 300 - 600 1 600 - 1000 1
I 27% I ?lO% I
?15%
DIMENSIONS:
NOTE :
DLL(ENSIW IN INCHES AND OALLIYETERSI.
I
:& (41
Accessories Furnished:
Power Cord
Accessories Available:
16471A through 16490A,
and 16465A
Supplemental
16462A Auxiliary Capacitor.
16014A Series Loss Test Adapter.
16451A Dielectric Test Adapter.
* The frequency in parentheses indicates frequency at which maximum Q factor is obtained
(for the respective inductor).
** Approx. resonant frequency for tuning capacitance of 450pF.
*** For 43426 Option 001 only. use
16462A
16014A Series Loss Test Adapter
Auxilialy
Capacitance Range: 300pF to 2700pF in steps
of 300pF. 10 ranges including OFF position.
Capacitance Accuracy: +l% on all ranges.
5000 at 20kHz on all ranges.
Q:
Residual inductance: approx. O.luH.
Residual capacitahce at OFF position:
approx. 23pF.
Useable Frequency Range: 1OkHz to 10MHz.
Capacitor
Measurable Capacitance Range: 450pF to 0.225uF
Measurable Resistance Range: 1Om.Q to 80R at
lOMHz, 4R to 8kR
Stray Capacitance Between Unknown Terminals:
approx. 3pF.
Insulation Resistance between Unknown Terminals
approx. 1OMR at 1MHz.
Residual Inductance: approx. 30nH
16451A Dierectric Test Adapter
(refer to Page 3-21 Table 3-2).
at
1OkHz.
4
3
2
9
l-6
Model 4342A
Section II
Paragraphs 2-l to 2-16
SECTION II
INSTALLATION
2-l. INTRODUCTION
2-2. This sectioncontains informationfor unpacking,
inspection, repacking, storage, and installation of the
Model 4342A.
2-3. INITIAL INSPECTION
2-4. MECHANICAL CHECK
2~5. If damage to the shipping carton is evident, ask
that the carrier’s agent be present when the instrument
is unpacked. Inspect the instrument for mechanical
damage. Also check the cushioning material for signs
of severe stress.
2-6. PERFORMANCE CHECKS
2-7. The electrical performance of the Model4342A
should be verified upon receipt. Performance checks
suitable for incoming inspectionare given in Section
V, Maintenance.
2-8. DAMAGE CLAIMS
2-9. If the instrument is mechanically damaged in
transit, notify the carrier and the nearest Hewlett-
Packard field office immediately. A list of field offices
is on the backof this manual. Retain the shipping carton andpadding material for the carrier’s inspection.
The fieldoffice will arrange for replacement or repair
of your instrument without waiting for claim settle-
ments against the carrier.
2-10. Before shipment this instrument was inspected
and found free of mechanical and electrical defects.
If there is any deficiency, or if electrical performance
is not within specifications, notify your nearest
Hewlett-Packard Sales and Service Office.
sq in. bursting test) with a layer of excelsior
about 6 inches thick packed firmly against all
surfaces of the instrument.
2-13. ENVIRONMENT. Conditions during storage
and shipment should normally be limited as follows:
a. Maximum altitude, 20,000 feet
b. Minimum temperature, -40” F (-40” C)
C.
Maximum temperature, 167” F (75°C)
2-14.
2-15.
from
and Line frequency from 50 to 400Hz. A slide
switch on the rear panel permits quick conversion for
operating from either voltage. Insert a narrow- blade
screwdriver in the switch slot and slide the switch
the right for 115-volt operation (“115” marking exposed) or to the left for 230-voltoperation (“230” marking exposed). The Model 4342A is supplied with 115volt fuse; for 230-volt operation, be sure to replace
this fuse with that listed in Table 2-I.
POWER CONNECTION
LINE VOLTAGE. The Model 4342Aoperates
either 115 or 230 volt (*lo%) ac line voltage
Table 2-l. AC Line Fuse
Conversion 115-volt
Slide Switch Right
(“115’)
AC Line Fuse 0.6 amperes
Slow-Blow
2110-0339
230-volt
Left
(“230”)
0.3 amperes
Slow-Blow
21 lo-0044
to
2-11. STORAGE AND SHIPMENT
2-12. PACKAGING. To protect valuable electronic
equipment during storage or shipment always use the
best packaging methods available,
Packard field office can provide packing material such
as that used,for original factory packaging. Contract
packaging companies in many cities can provide dependable custom packaging on short notice. Here are
a few recommended packaging methods :
a. RUBBERIZED HAIR.
of instrument with protective wrapping paper.
Pack instrument securely in strong corrugated
container (350 lb/sq in. bursting test) with 2inch rubberized hair pads placed along all surfaces of the instrument. Insert fillers between
pads and container to ensure a snug fit.
b. EXCELSIOR. Cover painted surfaces of instru-
ment with protective wrapping paper. Pack in-
strument in strong corrugated container (350 lb/
Cover painted surfaces
Your Hewlett-
CAUTION
To avoiddamage to theinstrument, before
connecting the power cable, set the 115/
230-volt switch for the line voltage to be
used.
2-16. POWER CABLE, To protect operating personnel, the National Electrical Manufacturers Association (NEMA) recommends that instrument panels and
cabinets be grounded. Accordingly, the Model 4342A
is equipped with a detachable three.-conductor power
cable which, when plugged into an appropriate recepta-
cle, grounds panel and cabinet. The offset pin of the
three-prong connector is the ground pin. Proceed as
follows for power cable installation.
a. Connect flatplug (3-terminal connector) to LINE
jack at rear of instrument.
b. Connect plug (a-blade with round grounding pin)
to J-wire (grounded) power outlet. Exposed
2-l
Section II
portions of instrument are grounded through the
round pin on the plug for safety; when only 2blade outlet is available, use connector adapter
(HP Part No. 1251-0048). Then connect short
wire from slide of adapter to groundto preserve
the protection feature.
Model 4342A
2-2
Model 4342A
Section III
Paragraphs 3-1 to 3-9
SECTION III
OPERATION
3-1. INTRODUCTION.
3-2.
quality factor of inductors from 5 to 1000
and,
resistance, and the dielectric constant of
insulating materials over the frequency range
of 22kHz to 70MHz.
instructions and information necessary for
operating the 4342A Q Meter.
Fundamental operating procedures and general
techniques for measuring various parameter
values of the unknown directly and indirectly
by using accessories appropriate to the
characteristics of the unknown are also
outlined in this section.
3-3. PANEL CONTROLS, CONNECTORS AND
3-4. Control panel, top terminal deck, and
rear panel features of the 4342A are described in Figures 3-1 and 3-2. The numbers
in the illustrations are keyed to the descriptive items for each figure. Other detailed information about the functions of the
panel controls and connectors is provided in
paragraphs 3-8 through 3-11.
3-5. Q MEASUREMENT-GENERAL.
3-6. To complete the measuring circuit, the
Model 4342A requires the connection of an inductor to the measurement COIL terminals.
This circuit is then used to establish a
resonance, either by setting the frequency
controls to a predetermined frequency and
varying the tuning capacitor, or by presetting the tuning capacitor to a desired value
and adjusting the frequency controls. Reso-
nance is indicated by maximum deflection of
the panel Q meter. The Q value of the sample
is proportional to Q meter deflection at the
resonant frequency.
3-7. The "indicated Q" which is the Q meter
reading at resonance is called the "circuit
Q" because it includes all the additive
losses inherent in the instrument including
The 4342A Q Meter can measure the
in addition, capacitance, inductance and
This section provides the
INDICATORS.
those in the tuning capacitor, the Q volt-
meter input resistance, output resistance of
the oscillator signal injection circuit, and
contact resistances of the measurement termi-
nals.
ing or "circuit Q" is called "indicated Q"
throughout the balance of this manual. The
"effective Q", which is dependent only on the
inherent loss of the sample and can be meas-
ured only by an ideal measuring circuit, is
somewhat greater than the "indicated Q".
However, the "indicated Q" can
the "effective Q", by reducing instrument
losses as much as is possible. So, in most
instances, these Q values can be deemed to be
the same. The 4342A employs a Constant Voltage Injection System obviating the use of a
thermocouple level meter (the resistance of
thermocouple device would contribute additional losses to the measuring circuit) and
the coupling resistor used in traditional Q
meters.
jection transformer, the improved operating
performance of the Q voltmeter, and the pre-
cision tuning capacitor which has extremely
low loss over a wide frequency range minimize
the difference between the "indicated Q" and
"effective Q".
3-8. GO/NO-GO FUNCTION.
3-9. The 4342.4 Go/No-Go function provides
an annunciation when the measured Q value exceeds a reference value.
outputs, the OVER LIVIT lamp display and a
relay contact output (rear panel) are available. The OVER LIMIT indicator lamp lights
and the relay is energized when the measured
Q value is over the reference value set by
the front panel Q LIMIT control. Annunciation time can be selected to occur at either
1 second intervals or to be continuous by the
rear panel OVER LIMIT DISPLAY TIME switch,
When the switch is set to its 1 set position
and the Q meter indication goes over the pre-
set Q limit control value, the OVER LIMIT
lamp lights once for 1 second. In the con-
tinous mode,
during the entire time that the Q value meter
deflection exceeds the preset value. Relay
contact output follows in the same manner.
To avoid ambiguity, the Q meter read-
approximate
The low output impedance of the in-
Two annunciation
the lamp stays continuously lit
3-l
Section III
Figure 3-l
Model 4342A
3-2
LINE PUSH ON/OFF Switch:
1.
power on/off switch.
FREQUENCY RANGE Selector: These push- The frequency is read from FREQHENCY
2.
buttons select the desired measurement scale @and the multiplier indicator
frequency range from among the seven
ranges covering 22kHz to 7OMllz (10kHz
to 32MHz for Option 001). The inductance range which may be measured
directly at the "L" scale frequency
point on the selected frequency range
is labeled on the panel adjacent to
the pushbuttons.
Figure 3-l.
Instrument
Front Panel Controls (Sheet 1 of 2).
3. FREQUENCY Dial Control: This dial
wheel varies the measurement frequency
as well as the FREQUENCY dial scale@.
0
Q LIMIT Control:
4.
sets the low limit of the Q value for
Go/No-Go checks. The Q LIMIT setting
dial scale numbers are related to
meter deflection (% of full scale).
This dial control
Model
4342A
Section III
Figure 3-l
Frequency Multiplier Indicator: The
5.
Frequency multiplier indicators, ad-
jacent to the frequency dial scale,
light and correspond with the settings
of the frequency range selector @
pushbuttons.
6.
FREQUENCY Scale:
The Frequency scale
comprises two scales with ranges of
2.2 to 7.0 and 7 to 22 (1.0 to 3.2 and
3.2 to 10 for Option 001). One or the
other of the scales is automatically
illuminated depending on the FREQUENCY
RANGE selector @ setting.
OVER LIMIT Display: The letters "OVER
7.
LIMIT" are displayed when the measured
Q value exceeds the limit value set by
the Q LIMIT control 0.
Measurement Terminals: These binding
8.
post terminals facilitate connection
of the unknown and the various measurement aid accessories. A simplified
terminal circuit schematic is provided
by the top panel label.
9.
Q Meter:
At
maximum meter pointer de-
flection, this meter indicates the Q
value of the sample or of the measuring circuit as well as the optimum
tuning point. The outer two scales (0
to 100 and 0 to 30) are the Q readings.
The inner two reverse scales (10 to 0
and 3 to 0) provide hQ readings when
making AQ measurements. Meter scale
indicators at the left end of scale
automatically light to indicate the
appropriate scale (to read) on the se-
lected
Meter Pointer Adjustment Screw:
10.
Q/hQ
range.
adjustment screw zero-sets the meter
pointer so it is exactly over the zero
calibration mark when the instrument
is off.
AQ ZERO Controls:
11.
These coarse and
fine controls adjust the meter indication for zero (reference) scale in AQ
measurements.
This function applies
only to AQ measurements.
This
L Scale: This dial scale allows di-
12.
rect reading of inductance sample
values at the "L" frequency. An "L"
scale frequency point, common to and
useable on all frequency ranges, is
labeled with a blue letter on the FRE-
QUENCY scale 0.
The L scale indi-
cates the inductance value of the un-
known when resonated with the tuning
capacitance at the "L" frequency.
13. AC Scale: This dial scale permits the
reading of the capacitance of a
vernier tuning capacitor from -5pF to
+5pF in O.lpF steps. The actual tuning capacitance is sum of the C Scale
@ and the AC Scale readings. A small
change in the tuning capacitance ad-
justment point resulting from a
variation in test parameters can be
accurately read from the spread AC
scale.
14. C Scale:
This dial scale is for reading the capacitance of the main tuning
capacitor which may be varied from
25pF to 470pF.
A
C scale reading is
exact (calibrated) when the AC scale@
is set to OpF.
15.
AC Dial Control: This dial wheel
varies the vernier tuning capacitor
and moves the AC Scale 0. The control employs a string drive mechanism
which facilitates easy adjustment of
vernier capacitor.
L/C Dial Control: This dial wheel
16.
varies the main tuning capacitor as
well as moving the C scale @ and L
scale 0.
Q/ AQ RANGE Selector: These push-
17.
buttons select the desired Q range
(either 30, 100, 300 or 1000 full
scale).
AQ button enables AQ measure-
ment and expands Q resolution by ten
times (3, 10, 30 or 100 full scale).
Figure 3-l. Front Panel Controls (Sheet 2 of 2).
3-3
Section III
Figure 3-2
Model 4342A
1
METER ZERO AD<J: This trimmer adjust-
1.
ment electrically zero-sets the meter
pointer so that it is exactly over the
zero calibration mark when the instru-
ment is on.
FUSE: Instrument power fuse is in-
2.
stalled in this fuse holder. Appropriate current rating for the fuse required is labeled on the rear panel.
VOLTAGE SELECTOR: This slide switch
3.
selects the appropriate ac operating
power voltage (115V or 230V +lO%).
Selection of the ac voltage must be
made before the instrument is connected to power line.
LINE Receptacle: Male ac power line
4.
receptacle with center ground pin for
powering the instrument from a 115V or
23OV, 48 - 440Hz line. Before con-
necting power cord (furnished), VOLTAGE SELECTOR @ should be properly set.
OVER LIMIT DISPLAY TIME Switch: This
5.
slide switch sets "OVER LIMIT" annunciation time for Go/No-Go checks to
either 1 second (1 set) or to contin-
ous (00).
OVER LIMIT SIC. OUTPUT Connector:
6.
Relay contact output for Go/No-Go
checks. Center and outer conductors
of this BNC connector are internally
short-circuited when measured Q value
exceeds the limit value set by the Q
LIMIT control.
7.
Q .4NALOG OUTPUT Connector: 0 to 1v
analog output proportional to meter
deflection.
Output impedance is ap-
proximately 1kR.
FREQUENCY MONITOR Connector:
8.
connector provides a portion of inter-
nal oscillator output for monitoring
oscillator frequency with external e-
quipment (such as a frequency counter).
Output level is 17OmVrms min. and
output impedance is 50R.
9.
Measurement Terminals: These six
binding post terminals, including the
two shield terminals, provide the con-
nection capabilities for attaching the
unknown sample as well as supplemental
inductors, auxiliary capacitors, and
other devices and accessories used in
making measurements.
This BNC
3-4
Figure 3-2. Rear Panel Controls and Connectors.
Model 4342A
Section III
Paragraphs 3-10 to 3-17
3-10. MEASUREMENT TERMINALS.
3-11. Six binding post terminals, including
two shield terminals, mounted on the instrument top deck, facilitate connection of unknown samples and accessories to the measuring circuit. Figure 3-3 illustrates the
measurement terminals circuit configuration.
Shield terminals 3 and 6, and binding post 4
are directly connected to instrument chassis
(grounded). Binding posts 1 and 2 are the LO
and HI COIL terminals, respectively, to which
an inductor is connected to compose the circuit to be resonated. Inductors can be meas-
ured by connecting them to the COIL terminals
(1 and 2) and by taking resonance with the
tuning capacitor.
injected into the measuring circuit between
LO COIL terminal 1 and GND terminal 4. Bind-
ing posts 4 and 5 are CAPACITOR terminals
which are used for doing parallel connection
measurements (outlined in paragraph 3-19).
Shield terminals 3 and 6 are used for connec-
tion to the shield terminal of an inductor or
to the guard terminal of the device connected
between HI COIL terminal 5 and GND terminal 4.
3-12. HOW TO CONNECT UNKNOWN.
3-13. There are three basic methods of connecting unknown sample to the measuring cir-
cuit of the Q Meter. The characteristics of
the unknown, the parameter value to be measured, and the measurement frequency are the
factors which guide the selection of an appropriate connection method. The fundamental
operating procedures for each individual connection method are outlined in Table 3-l.
The oscillator signal is
3-14. MEASUREMENT PARAMETERS AND CONNECTION
METHODS.
3-15. The connection to the measuring circuit of the 4342A, when measuring quality
factor, inductance, capacitance, resistance
or dielectric constant, may be either a di-
rect, parallel, or a series connection and
depends upon the sample. As the sample
values and measurement parameters are the
guidelines for selecting an appropriate connection method, a discussion of the measurement capabilities unique to each connection
method will help you to make straight-forward
measurements. The measurement range limits
of the individual connection methods and
associated reasoning are outlined in the
paragraphs which follow.
3-16.
3-17.
method in taking Q meter measurement parameters, only the quality' factor, inductance,
equivalent series resistance, and distributed
capacitance of the inductor can be read from
Q meter indications. In addition, the quality factor and the inductance measurement
ranges covered by the direct connection
method are dependent on sample inductance and
measurement frequency. This is because the
sample value and measuring frequency must
satisfy the following mathematical relationship so as to resonate with the measuring
circuit:
can be measured directly by the 4342A is approximately 54uH to 1.2mH. And, for a given
inductance, the measurement frequency range
is indicated. For example, a 1OuH inductor
can be measured over a frequency range of ap-
proximately 2.3MHz to 11MHz. Additionally,
the quality factor of sample must be below
1000 (upper range limit). Figure 3-4 sh/ows
the relationships between the measurement fre-
quency and the inductance limits measurable
with the 4342A alone (without using any supplemental equipment). In Figure 3-4, the
shaded area denotes the applicable induct-
ances and useable frequencies. The seven
bold lines in the shaded area indicate the "L"
frequencies and the ranges of inductance
which can be read from the L/C dial L scale
3-5
Section III
Paragraphs 3-18 to 3-23
Model 4342A
at these particular L frequencies. The induc-
tance at a measurement frequency other than
the "L" frequency can be determined by substi-
tuting frequency and L/C dial (C scale) read-
ings in equation 3-l.
3-18. Expansion of measurement ranges.
3-19.
For higher or lower value inductances
(above or below the shaded area in Figure
3-4), a parallel or series connection of the
unknown to the measuring circuit enables the
measurement to be made. To obtain the value
of the desired parameter, these methods em-
ploy a comparison of the Q meter indications.
The Q meter measuring circuit is first resonated with a reference inductor.
Then the
sample is connected in parallel or in series
with the measuring circuit and the circuit
again resonated.
The sample value is calcu-
lated from the difference in Q meter indica-
tion measurements made before and after connecting the sample. In the equation from
which the sample values are obtained, the
values inherent in the reference inductor are
subtracted from the measurement quantities.
Consequently, the characteristics of the reference inductor do not (theoretically) affect
measurement results.
In addition to their expanded measurement
ranges,
the parallel and series methods have
some measurement capability advantages which
do not appear when using direct methods.
A detailed description of these advantages is
given in the discussion in paragraph 3-58.
3-20. Capacitance Measurement.
3-21. For capacitor samples, either a paral-
lel or series connection method may be used
when measuring either the capacitance or the
Q value. The criteria for selecting the ap-
propriate connection method concerns only the
sample value and is irrespective of the measurement frequency. Capacitances higher than
approximately 450pF (up to approximately
0.2uF) are normally measured by the series
method and lower capacitances are easily
measured by the parallel method. Generally,
capacitors can be measured at the desired
frequency by using an appropriate inductor as
a measurement aid.
3-22. Resistance Measurement.
3-23. Resistance values are fundamentally
calculated from measured Q values. Thus, the
connection method selected depends upon the
sample value and the measurement frequency.
Figure 3-5 shows approximate limits for both
parallel and series measurements.
The upper
shaded area indicates the combinations of frequency and measurable resistance values for
parallel measurements. Similarly, the lower
shaded area indicates the values for series
measurements. For sample values between the
upper and lower shaded areas, it is difficult
3-6
I I I III I I III I I III I I III
IOK lOOK
Figure 3-4.
FREQUENCY (Hz)
Inductance Measurement Ranges
IM IOM l3OM
vs. Frequency (direct method).
Model 4342A
Section III
Paragraphs 3-24 to 3-29
to measure with either connection method.
These limits are based on the use of a reference inductor having a Q value of 280.
Parallel measurement low limits can be ex-
tended by using an external capacitor connected to the measurement CAPACITOR (HI and
GND)
terminals.
3-24. High Q Measurement.
3-25. Measurement of high quality factors up
to 10000 can also be made by the parallel or
series connection methods. These methods
enable the measurement of low loss samples
and are especially useful in the measurement
of high Q capacitors.
As
inherent losses in
the instrument will cause larger incremental
measurement errors in higher Q measurements,
these residual loss factors should be taken
into consideration in the accuracies of measured values. In high Q measurements, the
measured Q should be deemed to be only a
rough approximation of the sample Q value.
A
detailed discussion on parallel and series
connection measurement errors is provided in
paragraph 3-60 and those which follow.
3-26.
Supplemental Equipment Used in
Parallel and Series Methods.
3-27. For use with the 4342A as reference
inductors, the Model 16470A series supple-
mental inductors are available. The
16470A
series inductors have various inductances
(from 0.07pH to 630mH) and totally cover the
frequency range of 1OkHz to 70MHz when used
with the 4342A as measurement aids. The reference inductor must be resonated alone
(before connecting unknown) at the desired
measurement frequency to take its inherent
values for reference. And, of course, the
useable frequency range of each individual
supplemental inductor depends upon the inductance of the individual coil. This frequency range is indicated on a label attached
to the case of each inductor. Detailed data
and information on the supplemental inductors
is tabulated in Table 1-2.
3-28. Inductor samples whose inductance is
somewhat lower than the low limits of the
measurement range of the 4342A may be meas-
ured by using an external high Q capacitor to
extend the available tuning capacitance range.
The external capacitor is connected between
HI and GND measurement terminals; its capacitance, thereby, adds to the tuning capacitance. For this special purpose, the HP
16462A Auxiliary Capacitor is available.
This capacitor module combines nine capacitors from 300pF to 2700pF (in 300pF steps) and,
when used with the 4342A, allows measurement
of low inductances to approximately l/6.7 of
the measurement
low limit
of the instrument.
IOK 22K IOOK IM IOM 70M
Figure 3-5.
MEASURING FREQUENCY IN Hz
Ranges of Measurable Resistance.
3-29.
Dielectric constant of an insulating
material is calculated from the capacitance
value of the sample held between a pair of
electrodes whose dimensions are accurately
known. Model 16451A Dielectric Test Adapter
is the test fixture which is specially designed for measuring dielectric constant
(E)
and dielectric loss angle (tan 6) and is directly attached to the 4342A measurement
terminals. The 16451A has a pair of variable
precision electrodes which can hold materials
measuring up to a maximum of 1Omm in thick-
ness. The electrodes operate similar to a
micrometer permitting direct reading of elec-
trode spacing (0 to 1Omm) with 0.02mm resolution.
The diameter of the electrodes has
been designed so as to simplify the associat-
ed calculations. Measurement time is thus
greatly shortened.
3-7
Section III
Figure 3-6
Model 4342A
3-8
I I
1
Figure 3-6.
1
Zeroing Procedure (sheet 1 of 2).
J’
Model 4342A
Mechanical zero adiustment
The meter is properly zero-set when the pointer sets exactly over
the zero calibration scale mark and the instrument is in its normal
operating environment.
To check the meter mechanical zero, turn the
instrument off and allow 30 seconds to completely deenergizethe z
strument.
the meter is not over zero,
Rotate meter pointer adjustment screw @ clockwise until meter
a.
To obtain maximum accuracy and mechanical stability, if
zero-set the meter as follows:
is moving toward zero in an upscale direction.
b. Continue rotating screw clockwise and stop when pointer is
exactly at zero. If the pointer overshoots, continue rotating
the adjustment screw clockwise to do steps a and b once again.
C.
When the pointer is exactly over zero, rotate adjustment screw
slightly counterclockwise to relieve tension on pointer suspension. If pointer moves off zero, repeat steps a, b and c, but
rotate less counterclockwise.
Section
Figure 3-6
TTT
Electrical zero adiustment
The meter pointer should set exactly over the zero scale mark when instrument is
turned on and nothing is connected to measurement terminals.
Turn the instru-
ment on and allow at least 15 minuts warm-up time to let the instrument reach a
stable operating condition. If meter pointer is not over zero, zero-set the
meter as follows:
Set FREQUENCY RANGE selector @to 22k - 70k (10k - 32k for Option
a.
001) and Q RANGE@ to 1000.
Adjust rear panel METER ZERO ADJ control@ so that the meter
b.
pointer is exactly over zero.
Figure 3-6. Zeroing Procedure (sheet 2 of 2).
3-9
Section III
Table 3-l
Model 4342A
Table 3-1.
Direct Connection.
HI HI
osc frequency.
Parallel Connection.
LO
osc -
(Bl
I
E
HI
-
v-
UNKNOWN
b
ON0
Methods of Connecting Unknown.
Inductors can usually be measured by connecting
them directly to the COIL terminals as shown in
Figure A. The measuring circuit is resonated by
adjusting either the L/C dial or the FREQUENCY
dial controls. The quality factor (indicated Q) of
0
the sample is read at maximum deflection of the Q
Meter. Setting the FREQUENCY dial to the "L"
scale point and taking resonance with the L/C dial
control permits reading the inductance of the
sample directly from the inductance scale (adjacent
to the tuning capacitor scale). Otherwise the
0
GND
inductance can be calculated from the frequency and
capacitance dial readings at the desired resonant
The parallel connection is suitable for high imped-
ance measurements. High inductances, high resist-
ances, and small capacitances can be measured by
connecting the samples to the CAPACITOR terminals
as shown in Figure B. Before connecting a sample,
the measuring circuit is resonated with a stable
inductor (such as a 16470 series supplemental
inductor) connected to the HI and LO COIL terminals
to obtain a reference Q reading and a capacitance
dial reading. The measuring circuit is again re-
sonated with the sample connected to the CAPACITOR
terminals by re-adjusting the L/C dial for maximum
Q meter deflection.
sample are derived from the Q meter readings and
the L/C dial readings obtained before and after
connecting the unknown sample. The derivation of
parameter values related to the unknown are detailed in paragraphs 3-64 through 3-72.
The parameter values of the
Series Connection.
3-10
HI
h
osc
(Cl
HI
0
GND
The Series connection is suitable for low impedance
measurements. Low inductances, low resistances and
high capacitances can be measured by connecting the
sample in series with a stable inductor as shown in
Figure C.
The 16014A Test Adapter is useful for
making the series connection to the unknown sample.
First,
a shorting strap is attached to the unknown
connection terminals in parallel with the sample
and the measuring circuit resonated with the L/C
control. For reference, the Q meter and capacitance dial readings are noted. The shorting strap
is then disconnected (or removed) and resonance of
the measuring cicuit is again taken by adjusting
the L/C dial.
The parameter values of the unknown
can be derived from the Q meter and capacitance
dial readings obtained before and after disconnecting the shorting strap. The derivation of the
parameter values related to the unknown are described in paragraphs 3-73 through 3-81.
Model 4342A
Section III
Paragraphs 3-30 to 3-34
Direct Connection Measurements
3-30. BASIC Q METER MEASUREMENTS.
3-31. QUALITY FACTOR AND INDUCTANCE
MEASLREMENT~ (DIRECT C~NNK-U~N).
3-32. This paragraph and those which follow
describe the fundamental operating procedures
for quality factor and inductance measurements which are typical applications of the
Q Meter. An inductor usually has some
distributed capacitance (Cd).
resonant frequency (fo) of the inductor is
determined by its self-inductance and the Cd.
The 4342A measuring circuit consideration of
distributed capacitance is shown in Figure
3-7. If the Q meter indication is Qt when Cd
is zero, then the presence of Cd will influence the voltage across the resonating induc-
tor such that the Q meter will actually indicate a Q value lower than Qt. The indicated
Q value (Qi) and the Qt can be correlated by
a correction factor (which is a function of
Cd and the tuning capacitance) each with the
other. A similar correction factor also
applies to difference of inductance readings
resulting from the presence of Cd.
tailed discussion of correction factors is
given in paragraph 3-50. When the Cd is less
than l/20 of the tuning capacitance, the
difference between Qi and Qt (Li and Lt are
similar in meaning) is within 5%.
The self-
A de-
Adjust L/C dial control for maximum
C.
panel Q meter deflection on the
instrument.
Note
Alternatively, the resonance may be
taken by setting the L/C dial to a
desired position and adjusting the
FREQUENCY dial for maximum Q meter
deflection.
Depress Q RANGE button as appropriate
d.
for obtaining a Q meter deflection
more than one-third of full scale and
less than full scale.
Re-adjust L/C dial (or FREQUENCY dial)
e.
control for maximum deflection. If
panel meter deflection exceeds full
scale,
up-range the Q RANGE and continue the adjustment. For easily obtaining a precise resonance, use the
AC dial control.
Note
The AC dial control facilitates
accurate adjustment for establishing resonance especially in high Q
measurements.
rI
I
Cd +
I
I
L,
GND
Figure 3-7.
Distributed Capacitance in
Direct Connection.
3-33. Q Measurement.
3-34.
To read the quality factor of an in-
ductance sample directly from the Q meter
indication, proceed as follows:
a. Connect unknown to measurement COIL
(HI and LO) terminals.
Depress an appropriate FREQUENCY RANGE
b.
button and set FREQUENCY dial control
to the desired frequency.
0
Read panel Q meter indication on the
f.
meter scale designated by the appro-
priate scale lamp indicator lit.
Note
The measured Q value corresponds to
the "indicated Q" of the sample.
To derive series equivalent resistance
g*
of the sample, substitute the Q meter
FREQUENCY, C dial, AC dial, and Q
readings in the following equation:
Rs = l/wCQWO.l59/fCQ . . . . . (eq. 3-2)
Where, Rs: equivalent series resist-
ance in ohms.
f: frequency dial reading in
hertz.
0: 2~r times the frequncy
(2wf).
c: sum of C and AC dial read-
ings in farads.
panel Q meter reading.
Q:
3-11
Section III
Paragraphs 3-35 to 3-38
Direct Connection Measurements
AQ
3-35.
3-36.
cal,
accurately on the normal Q scale.
Measurement.
When two Q values are nearly identi-
the difference is difficult to read
The AQ
feature of the 4342A provides accurate read-
ings for changes in Q on all Q ranges by providing ten times resolution, namely: 0 to 3,
0 to 10, 0 to 30, and 0 to 100.
To make a AQ
measurement, proceed as follows:
Connect the sample inductor to the
a.
measurement COIL (HI and LO) terminals
Resonate the inductor using the
b,
same
procedure as described in Q Measurement (para. 3-34) steps b, c, d and e.
c. Note panel Q meter reading.
Depress AQ button and set AQ COARSE
d.
and FINE controls so that meter pointer indicates zero (full scale) on AQ
scale.
Check for correct resonance by slight-
e.
ly rotating AC dial control.
If
Q
meter deflection is not at peak, re-
adjust AC dial and AQ controls.
Make the desired change in the sample
f.
or in the measuring circuit.
Adjust L/C dial control for maximum Q
g.
meter deflection.
Use AC dial control
for easily taking a precise resonance.
If meter pointer scales out at the
left end of the scale (AQ full scale),
reset the function to normal Q
meas-
urement and skip steps h and i.
h. Read panel Q meter indication on AQ
scale.
The AQ reading is the difference in Q resulting from the change
made in step f.
Model 4342A
3-37. Inductance Measurement.
3-38.
The inductance of a coil can be
meas-
ured directly from the Q meter inductance
scale at specific "L" frequencies. The in-
ductance range which
may
be measured directly
at the "L" scale frequency point on the selected frequency range is labeled on the
panel adjacent to the FREQUENCY RANGE pushbuttons. To measure inductance at the "L"
frequency, proceed as follows:
Connect unknown to measurement COIL
a.
(HI and LO) terminals.
b.
If the approximate value of inductance
is known, select an appropriate
measuring frequency range. Refer to
the chart in Figure 3-4 or the inductance multiplier label adjacent to the
FREQUENCY RANGE pushbuttons. For the
samples whose values are quite unknown,
select a trial frequency range. Depress the selected frequency range
pushbutton.
Set FREQUENCY dial control for the "L"
C.
scale frequency designated by the mark
"-L-" (shown in blue) on the FREQUENCY
scale.
Set Q RANGE to 100. Rotate L/C dial
d.
control and verify that panel Q meter
indicates peak deflection.
If a peak
meter deflection can not be recognized,
change to another trial FREQUENCY
RANGE setting and repeat the procedure
until a peak is verified.
Set AC dial to zero scale (OpF).
e.
1.
.
1.
3-12
The differential Q value (after
change) is given by the following
equation:
Qz = Q1 - AQ
where, Q1:
. . . . . . . . . . . . . . . (eq. 3-3)
Q meter reading in step c
(before change).
present Q value (after
Q2:
change).
AQ: Q meter reading from AQ
scale in step h.
When the change in Q exceeds AQ full
scale, the difference is given by the
following equation:
AQ = QI - Qz
. . . . . . . . . . . . . . .
(eq. 3-4)
Adjust L/C dial control for maximum Q
f.
meter deflection (change Q RANGE setting as necessary).
Read L/C dial L scale indicated by the
g.
fixed scale pointer. To calculate the
inductance value,
multiply the L scale
reading by the factor for the selected
inductance range.
Note
The measured value corresponds to
the "indicated L" including meas-
uring circuit residual factors
(similar to "indicated Q" value).
Loading...
+ 146 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.