HP 428B Instruction Manual

Errata
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
2-17. PREPARATION FOR STORAGE AND SHIPMENT.
3
2·20. STORAGE. 3
OPERATING INSTRUCTIONS 5
3-1. INTRODUCTION. 5 3-3 OPERATING PRECAUTIONS. 5
3-4. OPERATING CONSIDERATIONS. 5 3-5. INTERCHANGING PROBE HEADS. 5
3-7. EFFECT OF MEASUREMENT ON CIRCUIT. 5 3-12. EFFECT OF CIRCUIT ON MEASUREMENT. 5
3-19. Magnetic Fields. 6 3-26. OPERATING PRACTICES. 6
3-27. MECHANICAL OPERATION OF PROBE. 6 3-29. DEGAUSSING OF PROBE HEAD. 6
3-33. ELECTRICAL ZERO SET. 6 3-37. POLARITY OF CURRENT. 6
3-39. INCREASING THE ABSOLUTE SENSITIVITY 7 3-41. CURRENT CHECK LOOPS.
3-44. NULLING CURRENTS. 3-46. USE OF OUTPUT JACK.
3-48. With Oscilloscope. 3-50. With Recorder.
THEORY OF OPERATION
4-1. INTRODUCTION. 4-3. THEORY OF OPERATION.
4-9. CURRENT PROBE. 4-19. 20 kHz OSCILLATOR.
4-23. HEAD-DRIVE AMPLIFIER. 4-25. DETECTOR GATE AMPLIFIER.
4-28. 40 kHz INPUT/AMPLIFIER CIRCUIT. 11 4-30. SYNCHRONOUS DETECTOR AND FILTER (C24).
4-36. DC AMPLIFIER. 12 4-43. NEGATIVE FEEDBACK CURRENT CIRCUIT. 12
4-45. 40 kHz PHASE SHIFTER. 12 4-48. POWER SUPPLY. 12
7 7
7 7
7
9
9 9
9 11
11 11
11
MAINTENANCE 14 GENERAL INFORMATION 2
5-1. INTRODUCTION. 14 5-3. TEST EQUIPMENT REQUIRED. 14
5-5. IN-CABINET PERFORMANCE CHECKS. 14 5-7. CLEANING OF PROBE JAWS. 14
5-10. ELECTRICAL ZERO SET. 14 5-13. RANGE CHECK. 15
5-15. METER TRACKING. 15 5-17. OUTPUT CALIBRATION. 15
5-19. FREQUENCY RESPONSE. 15 5-21. AC OVERLOAD. 16
5-23. NOISE CHECK. 16 5-25. ADJUSTMENT PROCEDURE. 16
5-27. POWER SUPPLY. 16 5-29. MECHANICAL ZERO SET. 16
5-31. DC AMPLIFIER BALANCE. 16 5-34. ALIGNMENT. 17
5-35. OSCILLATOR BALANCE. 17 5-37. OSCILLATOR FREQUENCY. 17
5-39. OSCILLATOR LEVEL. 17 5-41. DETECTOR GATE. 17
5-43. TUNED AMPLIFIER. 17 5-44. Equipment Setup. 17
5-46. Input Alignment. 17 5-48. Interstage Alignment. 17
5-50. DETECTOR PHASE ADJUSTMENT. 17 5-53. Preliminary Adjustment. 18
5-54. Preset the controls as follows: 18 5-55. Drive Balance Adjustment. 18
5-59. TROUBLESHOOTING. 19 5-60. FRONT PANEL TROUBLESHOOTING. 19
5-63. DETAILED TROUBLESHOOTING. 19 5-64. Probe Check. 19
5-66. Power Supply Check. 19 5-71. Oscillator - Buffer Amp. Check. 21
5-80. Synchronous Detector. 21
REPLACEABLE PARTS 23
6-1. INTRODUCTION. 23 6-4. ORDERING INFORMATION. 23
6-6. NON-LISTED PARTS. 23
CIRCUIT DIAGRAMS 29
7-1. INTRODUCTION. 29 7-3. BLOCK DIAGRAM. 29
7-5. SCHEMATIC DIAGRAMS. 29 7-7. COMPONENT LOCATION DIAGRAMS. 29
MANUAL BACKDATING CHANGES 36
Model 428B
LIST OF TABLES
Table 1-1 Specifications 1 Table 5-1. Recommended Test Equipment. 13
LIST OF ILLUSTRATIONS
Figure 1-1. Model 428B Clip- On Milliammeter 2 Figure 3-1. Measurement Procedures 4 Figure 3-2. Polarity of Current. 6 Figure 3-3. Increasing The Absol ute Sensitivity. 7 Figure 4-1. Block Diagram 8 Figure 4-2. Simplified Block. 9 Figure 4-3. Magnetic Mechanical Analogy. 10
Figure 4-5. 428B Flux Gate. 10 Figure 4-4. Basic Flux Gate. 10 Figure 4-6. Waveforms. 10 Figure 4-7. Detector Bridge. 11 Figure 4-8. Negative Feedback 12 Figure 4-9. 90° Phase Shift 12 Figure 5-1. Cleaning Probe Jaws. 14 Figure 5-2. Electrical Zero Set. 14 Figure 5-3. Range Check. 15 Figure 5-4. AC Overload. 16 Figure 5-5. Oscillator Balance Probe. 17 Figure 5-6. Detector Phase Adjustment. 17
Table 6-1. Replaceable Parts 24
Figure 5-7. Detector Phase Display. 18 Figure 5-9. Detailed Troubleshooting Tree. 20 Figure 6-1. Parts Breakdown, current probe. 28 Figure 7-1. Block Diagram. 30 Figure 7-2. Component Locator For Circuit Board Part
No. 00428-66501 31
Figure 7-3. Front Panel Component Locator. 31 Figure 7-4 Rear Panel Component Locator. 31
Figure 7-5. Power Supply. 32 Figure 7-6. Block Diagram. 33 Figure 7-7. Component Locator for Circuit Board Part
No. 00428-66501 34 Figure 7-8. Front Panel Component Locator. 34 Figure 7-9 Rear Panel Component Locator. 34 Figure 7-10. Metering Circuit 35 Figure A-1. 428B Side Views. 37 Figure A-2 Backdating Schematics for 428B 38 Figure A-3 Backdating Schematics for 428B 39
Model 428B
428B SPECIFICATIONS
Table 1-1 Specifications
Current Range:
1 mA to 10 A full-scale, nine ranges.
Accuracy:
± 3% of full-scale ± 0.15 mA, from 0°C to 55°C. (When instrument is calibrated to probe).
Probe Inductance:
Less than 0.5 µH.
Probe Induced Voltage:
Less than 15 mV peak (worst case at 20 kHz and harmonics).
Output:
Variable linear output level with switch position for calibrated 1 V into open circuit (corresponds
to full-scale deflection). 1.5 V Max. into open circuit in uncalibrated position.
0.73 ± .01 V into 1 kΩin calibrated position.
Noise:
1 mA Range, < 15 mV rms across 1 kΩ. 3 mA Range, < 5 mV rms across 1 kΩ.
10 mA thru 10 A Ranges, <2 mV rms across 1 kΩ.
Frequency Range:
DC to 400 Hz (3 dB point).
AC Rejection:
Signals above 5 Hz with peak value less than full-scale affect meter accuracy less than 2%. (Except at 40 kHz carrier frequency and its
harmonics). On the 10 A range, ac peak value is limited to 4 A.
Probe Insulation:
300 V Max.
AC Power:
115 or 230 V ±10%, 50 to 60 Hz, 71 W.
Operating Temperature:
- 20°C to + 55°C.
Cabinet Mount:
7½" wide, 11½" high, 14½" deep (190,5 x 292,1 x 368,3 mm).
Weight:
Cabinet Mount: Net 19 lbs (8,6 kg); shipping 24 lbs (10,9 kg).
Rack Mount: Net 24 lbs (10,9 kg); shipping 35 lbs 15,9 kg).
Accessories Available:
-hp- Model 3528A Large Aperture Probe
-hp- Model 3529A Magnetometer Probe
-hp- Model 11035A Output Cable
-hp- Model 10110A Output Adapter
Dimensions:
Rack Mount
1
Model 428B
SECTION I
GENERAL INFORMATION
1-1. INTRODUCTION
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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