Title & Document Type: 428B Clip-On DC Milliammeter
Manual Part Number: 00428-90003
Serial Prefixes: 995
Revision Date: Circa November 1970
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OPERATING AND SERVICE MANUAL
-hp- Part No. 00428-90003
MODEL 428B
CLIP-ON DC MILLIAMMETER
Serials Prefixed: 995- and above
Appendix A, Manual Backdating Changes
adapts this manual to instruments with
earlier serial prefixes.
Copyright Hewlett-Packard
Company 1970 P.O. Box 301,
Loveland, Colorado, 80537 U.S.A.
Printed: NOV 1970
Model 428B
TABLE OF CONTENTS
1-1. INTRODUCTION 2
1-7. INSTRUMENT AND MANUAL IDENTIFICATION.
2
INSTALLATION 3
2-1. UNPACKING AND MECHANICAL INSPECTION.
3
2-4. OPERATION CHECK. 3
2-6. INSTALLATION. 3
2-8. POWER REQUIREMENTS. 3
2-10. OPERATION ON 115 OR 230 VOLTS. 3
2-13. THREE CONDUCTOR POWER CABLE. 3
2-15. RACK MOUNT MODEL. 3
1-2. The -hp- Model 428B Clip-On Milliammeter measures
the magnetic field, which exists around the wire carrying dc
current. Operating the instrument is simple. After zero
setting, the two jaws of the probe are clamped around wire
(arrow on probe head indicates direction of conventional
current flow) and the meter will indicate the current.
1-3. There are nine current ranges starting from 1 mA to 10
amp full-scale deflection. The sensitivity can be increased
even further by looping the wire several times through the
opening in the probe. The current indication is virtually
insensitive to superimposed ac signals and the series
loading of the circuit is less than 0.5 pH. A large amount of
feedback provides great stability.
1-4. OTHER PROBE HEADS.
1-5. Other probe heads are available to extend the
usefulness of your Clip-On DC Milliammeter. Write to the
nearest Sales and Service Office (listed in Appendix C) for
further information. At the time of publication of this manual,
the following accessory probe heads were available:
a. -hp-Model 3528A Large Aperture (2-1/2
inch probe head).
b. -hp- Model 3529A Magnetometer (1
gauss = 1 amp).
c. -hp- Model C11-3529A Magnetometer
(1 gauss = 1 mA).
1-6. Write to the nearest Sales and Service Office
(listed in Appendix C) stating your complete
requirements for information concerning special
applications.
1-7. INSTRUMENT AND MANUAL
IDENTIFICATION.
1-8. Hewlett-Packard uses a two-section serial
number. If the first section (serial prefix) of the serial
number on your instrument does not agree with
those on the title page of this manual, change
sheets supplied with the manual will define the
differences between your instrument and the Model
428B described in this manual. Some serial
numbers may have a letter separating the two
sections of the number. This letter indicates the
country in which the instrument was manufactured.
2
Figure 1-1. Model 428B Clip-On Milliammeter
Model 428B
SECTION II
INSTALLATION
2-1. UNPACKING AND MECHANICAL INSPECTION.
2-2. Inspect instrument for signs of damage incurred in
shipment. This instrument should be tested as soon as
it is received. If it fails to operate properly, or is
damaged in any way, a claim should be filed with the
carrier. A full report of the damage should be obtained
by the claim agent, and this report should be forwarded
to us. We will then advise you of the disposition to be
made of the equipment and arrange for repair or
replacement. Include model number and serial number
when referring to this instrument for any reason.
2-3. Hewlett-Packard Company warrants each
instrument manufactured by them to be free from
defects in material and workmanship. Our liability under
this warranty is limited to servicing or adjusting any
instrument returned to the factory for that purpose and
to replace any defective parts thereof. Any damage to
the instrument upon receipt is due to the carrier. File a
claim with the carrier as instructed in the preceding
paragraph.
2-4. OPERATION CHECK.
2-5. This instrument should be checked as soon as it is
received to determine that its electrical characteristics
have not been damaged in shipment. Refer to the
In-Cabinet Performance Checks of Section V of this
manual.
2-6. INSTALLATION.
2-7. See Paragraph 3-3 before operating this
instrument.
2-8. POWER REQUIREMENTS.
2-9. Power requirements are given in Specifications
table at t he front of this manual.
2-10. OPERATION ON 115 OR 230 VOLTS.
2-11. This instrument may be used with either a 115
volt or 230 volt supply with a frequency of 50 to 60 cps,
single phase. This instrument is shipped from the
factory ready for operation from a 115 volt source
unless otherwise indicated.
2-12. To operate from a 230 volt source, the 115-230
switch on the rear apron must be flipped to 230. First
turn the instrument off and pull the power cable from the
socket. Place a pointed tool, such as the sharpened end
of a pencil, in the slot of the switch and pull down.
Replace the fuse with the one given in Table 6-1 for 230
volt operation.
2-13. THREE CONDUCTOR POWER CABLE.
2-14. The three-conductor power cable supplied with
the instrument is terminated in a polarized, three-prong
male connector recommended by the National Electrical
Manufacturers' Association (NEMA). The third
conductor grounds the instrument chassis for the
PROTECTION OF THE OPERATING PERSONNEL.
When using a three-prong to two-prong adapter ground
third lead (green wire) externally.
2-15. RACK MOUNT MODEL.
2-16. This instrument is available in a rack mount
version in addition to the cabinet model shown in this
manual. The rack mount version is identical electrically
and similar physically except that the degausser has
been moved to the front panel for greater convenience.
2-17. PREPARATION FOR STORAGE AND SHIPMENT.
2-18. The best method for packing this instrument is in
the original shipping carton with the original fillers
packed in the same manner as when received from the
factory. Therefore, when unpacking, note carefully the
method of packing and save the original packing
material for possible future reuse.
2-19. If the original packing material is not available, and
it is desired to package the instrument for storage or
shipment, first wrap the instrument in heavy kraft paper
to avoid scratching the paint. Then pack in a cardboard
carton with a bursting strength of at least 150 lb per
square inch. Pad the instrument on all sides with at least
2 inches of rubberized hair or at least 4 inches of tightly
packed excelsior.
2·20. STORAGE.
2-21. No special precautions are necessary in storage
except the usual protection against mechanical damage,
salt air, etc.
3
Model 428B
4
Figure 3-1. Measurement Procedures
Model 428B
SECTION III
OPERATING INSTRUCTIONS
3-1. INTRODUCTION.
3-2. This section contains instructions and information
necessary for operation of the Model 428B clip-on
milliammeter.
3-3 OPERATING PRECAUTIONS.
CAUTION
a. BEFORE APPLYING OPERATING POWER TO
THE 428B, VERIFY THAT THE LINE VOLTAGE
SWITCH ON THE REAR PANEL INDICATES THE
LINE VOLTAGE TO BE USED AND THAT THE
INSTRUMENT IS PROPER L Y FUSED.
b. THE PROBE IS INSULATED TO WITHSTAND 300
VOLTS MAXIMUM. DO NOT USE THIS PROBE ON
A BARE WIRE WHICH IS MORE THAN 300 VOLTS
PEAK ABOVE GROUND.
c. DO NOT USE THE 428B PROBE IN THE
PRESENCE OF STRONG RF FIELDS.
d. DO NOT EXPOSE THE 428B PROBE TO
TEMPERATURES EXCEEDING 130° F (55°C). DO
NOT LAY THE PROBE ON TOP OF THE 428B
CABINET (OR ANY OTHER HOT SURFACE).
PROBE UNBALANCE AND EVENTUAL DAMAGE
WILL RESULT.
e. DO NOT DROP THE PROBE OR RELEASE THE
FLANGES ABRUPTLY SO THAT THE JAWS SNAP
TOGETHER.
f. DO NOT OPERATE THE DEGAUSSER FOR MORE
THAN THREE MINUTES CONTINUOUSLY.
g. BECAUSE THE 428B IS COOLED BY
CONVECTION" PLACE THE 428B WHERE AIR
CAN CIRCULATE FREELY THROUGH THE
INSTRUMENT.
h. DO NOT USE THE 428B TO MEASURE DC IN A
WIRE WHICH CARRIES MORE AC THAN
FULL-SCALE READING ON THE METER.
3-4. OPERATING CONSIDERATIONS.
3-5. INTERCHANGING PROBE HEADS.
3-6. Each probe is calibrated at the factory with a
particular instrument and carries the serial number of that
instrument (serial number appears on probe
connector) (NOTE: if your buying one with the probe,
make sure you verify this. The numbers are scribed
with a vibrating pen. Not very HP). If a probe has to be
replaced, a realignment and recalibration of the
instrument is necessary (see also Section V
Maintenance).
3-7. EFFECT OF MEASUREMENT ON CIRCUIT.
3-8. Reflected Impedance.
3-9. The probe will add a small inductance to the
circuit of less than 0.5 microhenries due to the
magnetic core and magnetic shield. This makes it
ideal for measuring current in very low impedance
paths such as ground loops where other instruments
would disturb the circuit.
3-10. Induced Voltage.
3-11. The gating signal, driving the core in and out of
saturation, will induce a voltage in the wire carrying
the dc current. This induced voltage is less than 15
millivolts peak. If more than one loop is passed
through the probe the induced voltage will be
multiplied by the number of loops.
3-12. EFFECT OF CIRCUIT ON MEASUREMENT.
3-13. Circuit Impedance.
3-14. The impedance of the circuit being measured
has practically no effect on the dc current
measurement. A shorted loop inserted along with a
wire carrying dc current will decrease the reading by
only 0.2% of full scale.
3-15. AC Fields & Superimposed AC Current.
3 -16. The instrument is designed to allow a high
amount of ac ripple in the dc being measured. The
presence of ac whose peak value equals full-scale
reading (limited to 4 amperes peak on 10-ampere
range) will cause less than 2% error in the dc reading.
Examples of such high ac currents are found in the
input of dc filter sections of power supplies.
3-17. Ac currents having frequency components of 40
kHz or harmonics thereof will cause error, as such
signals will interfere with the 40 kHz output signal of
the probe. The meter will indicate a beat reading if the
interfering frequency is within approximately 15 cycles
of 40 kHz or its harmonics. Although this situation is
very improbable, accurate dc current readings can be
obtained by shifting the frequency of the external ac
signal slightly.
3-18. The instrument as well as the pro be
head .should not be used in strong ac stray fields.
Such fields may exist in the vicinity of open core
power transformers, or large dc filter chokes, etc.
5
Model 428B
3-19. Magnetic Fields.
3-20. If the jaws of the probe are incompletely closed,
the magnetic shielding and the magnetic circuit will have
an air gap. The result is that dc fields, not associated with
the dc current being measured, will cause a shift in the
meter reading.
3-21. However, there will be an indication of a strong
external dc field even with the jaws perfectly closed.
Usually zero setting with the ZERO control compensates
such residual readings for a particular probe location.
3-22. EARTH'S MAGNETIC FIELD. The earth's magnetic
field will affect the reading if the jaws of the probe are not
completely shielded (jaws partially open). The effect of this
field is relatively strong - comparable to deflection due to
about 500 mA of current. Complete closure of the jaws
can be checked by switching to the 1 mA range with no dc
current input. If the jaws mate properly, the zero set
should stay within 0.1 mA while rotating the probe head
with respect to the earth's magnetic field.
3-23. If the zero shift is greater, the mating surfaces of the
jaws need to be cleaned or the probe wiring may be open
(see Section V).
3-24. FIELDS OF PERMANENT MAGNETS. Meter
magnets have strong stray fields, which can cause shift in
the current indication. Such fields are detected by bringing
the closed probe in the area where the measurement is to
be made and observing the zero shift (1 mA range).
3-25. FERROUS WIRE. Wires made out of magnetic
materials can cause a current reading of 2-3 mA without
any connection to the wire. This fact is important as leads
of most transistors are made out of magnetic material.
may be necessary after measuring current on the
1 thru 10 AMP RANGE.
3-32. Normally, it takes about 10 seconds to degauss
the probe when using the above method (see
Caution, Paragraph 3-3f).
3-33. ELECTRICAL ZERO SET.
3-34. If the instrument cannot be zero set electrically
(with ZERO control) there are two probable causes:
1) Incomplete closure of probe jaws, 2)
Magnetization of probe head.
3-35. Dust deposits on the lapped surfaces of the
probe jaws create an air gap. If the jaws are not
completely closed, the earth's magnetic field will
affect the reading. With the RANGE switch at 1 mA,
rotation of the closed probe should not vary the zero
set more than 0.1 mA. Cleaning of the jaws will
restore proper operation conditions (see Section V,
Cleaning of Probe Jaws).
3-36. Magnetic shields protect the probe head from
stray magnetic fields. However, excessive dc
currents (such as short circuit discharge currents
from electrolytic capacitors, etc.) will magnetize the
probe. For demagnetization of probe head, see
Paragraph 3-29, Degaussing of Probe Head.
3-37. POLARITY OF CURRENT.
3-38. The arrow on the probe head indicates the
direction of the conventional current flow for upscale
reading. Reversal of the current flow direction will
reverse the indication on the meter (see Figure 3-2).
3-26. OPERATING PRACTICES.
3-27. MECHANICAL OPERATION OF PROBE.
3-28. The probe jaws are opened by simply squeezing
together the two flanges on the probe body. An internal
spring returns the jaws to their proper position when the
flanges are released. (See Paragraph 3-3e.).
3-29. DEGAUSSING OF PROBE HEAD.
3-30. To demagnetize the probe, proceed as follows:
a. Insert probe into degausser at the rear of the
instrument (located on front panel of rackmount
models) with arrow on probe in same position as
arrow marked on chassis.
b. Depress degausser switch S3 to energize degausser.
c. Withdraw probe very slowly for the first few inches
while depressing the degausser switch until probe is
removed approximately one foot.
d. Zero instrument on 1 mA range with ZERO control
3-31. Under normal operating conditions, degaussing
Figure 3-2. Polarity of Current.
6
Model 428B
3-39. INCREASING THE ABSOLUTE SENSITIVITY
3-40. The sensitivity of the instrument can be increased by
looping the wire (carrying the dc current) several time
through the opening of the probe (see Figure 3-3). For
example, three turns increase the sensitivity three times.
With an increased sensitivity, however, the induced voltage
between the probe and the circuit under measurement will
increase also.
Figure 3-3. Increasing The Absolute Sensitivity.
3-41. CURRENT CHECK LOOPS.
3-42. In restricted situations such as printed circuit boards,
wire loops for the probe can be built into the circuit to allow
convenient current measurements with the Model 428B.
Here, currents can then be measured under operating
conditions with the same ease as voltage measurement.
3-43. Circuits can also be modified to accept an impromptu
loop for testing. As an example, to measure the collector
current of a transistor for troubleshooting purposes, the
collector lead can be removed from the board and a loop of
fine wire soldered between the collector lead and the board.
To measure current through a resistor, lift one lead and
install a series loop, clip the 428B probe around the loop and
measure current through the resistor. As an alternative, an
equivalent resistor with long leads can be installed to replace
the resistor in question.
3-44. NULLING CURRENTS.
3-45. The resolution of the 428B can be increased by nulling
one current against another and measuring the difference
between the two. To null the reading, clip the probe over
both wires at once with the wires so arranged that the
currents are going in opposite directions. The considerations
mentioned in Paragraph 3-39 also apply to current nulling.
For example, assume that a 0.6 A current source is to be
tested against a 0.4 A standard. The 0.6 A supply should be
looped twice through the probe jaws and the 0.4 A supply
should be looped three times through the jaws such that the
7
two currents oppose each other. It should be
remembered when making such a measurement,
that the absolute value of any deviations observed
have been multiplied. If, in the above example, the
0.6 A supply wavered by .01 A, the change would
be read as .02 A on the meter.
3-46. USE OF OUTPUT JACK.
3-47. The OUTPUT jack enables the 428B to be
used as a dc coupled: amplifier/I-E transducer
/isolator. The basic action of the 4 28B (considered
as an input/output device) is to sense the magnetic
field around a current carrying wire and deliver a
proportional voltage at the OUTPUT jack. The
value of the output can be varied by using the
OUTPUT LEVEL control to produce as much as 1
1/2 volts at 1 mA. While the 428B meter registers
average dc (ignoring ac), the output at the
OUTPUT jack contains both the dc and ac
components of the signal being measured.
3-48. With Oscilloscope.
3-49. To display the output of the 428B on an
oscilloscope:
a. If the oscilloscope is dc coupled, it can be
calibrated as in Paragraph 3-51.
b. Clip the probe around the wire which varies the
signal to be displayed.
c. Connect the oscilloscope input to the 428B
OUTPUT jack.
d. Adjust the 428B RANGE switch to the
appropriate range.
3-50. With Recorder.
3-51. To record the output of the 428B on a graphic
recorder:
a. Insure that the recorder's input impedance
exceeds 1400 ohms.
b. Connect the recorder input to the 428B
OUTPUT jack.
c. Zero the 428B on the 1 mA Range, turn
OUTPUT LEVEL to minimum output.
d. Zero the recorder.
e. Adjust the 428B ZERO control for full-scale on
the 428B meter.
f. Adjust the 428B OUTPUT LEVEL control for
full scale on the recorder.
g. Zero the 428B, switch to the appropriate range
and clamp the 428B probe around the wire
which carries the signal to be measured.
3-52. When recording current variations with the
428B, it should be borne in mind that the 428B
displays some long term zero drift. The 428B zero
drift normally amounts to about 300 µA (indicated)
per clay so periodic checks should be made to
determine whether or not the ZERO controls need
adjustment.
Model 428B
8
Figure 4-1. Block Diagram
Model 428B
SECTION IV
THEORY OF OPERATION
4-1. INTRODUCTION.
4-2. This section describes the overall operation of the Model 428B, the operating principle of the current probe and
the function of the different circuits of the instrument.
4-3. THEORY OF OPERATION.
4-4. The simplified block diagram of Figure 4-2 shows the basic operation of the Model 428B Clip-ON Milliammeter.
4-5. The probe clips around a wire carrying dc current and delivers a 40 kHz output signal which is proportional to the
dc current. For transducing the dc current into a 40 kHz signal, the probe requires a 20 kHz gating signal, as described
in detail under Paragraph 4-9, Current probe.
4-6. The 40 kHz output signal of the probe is amplified, detected and fed back as negative feedback current to the
probe head cancelling the effect of the measured dc current and thus reducing the 40 kHz output signal almost to zero.
The negative feedback current, being proportional to and magnetically almost equal to the dc current of the inserted
wire, is used to indicate the measured dc current.
4-7. The 20 kHz oscillator has two functions: First, it supplies a 20 kHz signal for driving the probe head, and also
provides a 40 kHz (second harmonic) signal for gating the 40 kHz Synchronous Detector.
4-8. Due- to slight unbalances, the probe head output contains a small 40 kHz signal, even with no dc current being
measured. A 40 kHz phase-shifter output cancels such residual 40 kHz signal (zero-set controls).
4-9. CURRENT PROBE.
4-10. The probe head is a specially designed second harmonic flux gate type of a magnetometer used to measure the
magnetic field around a wire carrying direct current.
4-11. The flux gate principle is easily understood by referring to the mechanical model shown in Figure 4-3.
4-12. Coil A (representing wire through probe), is energized with dc, producing a dc flux in the core. Armature is
rotating at a constant rate (F), gating the flux 2F times per second inducing a voltage of 2 F frequency in coil B. The
amplitude is determined by the dc in coil A.
9
Figure 4-2. Simplified Block.
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