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DM-81
DIP METER
INTRODUCTION .............................................................................................................. 1
Inductive coupling (Fig. 1A)........................................................................................... 1
Capacitive coupling (Fig. 1B)......................................................................................... 1
FEATURES ........................................................................................................................ 3
SPECIFICATIONS............................................................................................................. 4
CONTROLS ....................................................................................................................... 5
PRECAUTIONS................................................................................................................. 6
Battery and Oscillation Coil Loading ............................................................................. 6
Obtaining a Dip Point ..................................................................................................... 6
Measuring Transistor Resonant Circuits......................................................................... 6
Caution in Measuring Transmitters ................................................................................ 6
Caution in Motor Pointer Deflection Change................................................................. 7
APPLICATIONS................................................................................................................ 7
Use as a Dip Meter.......................................................................................................... 7
Other Frequency Measurements ..................................................................................... 8
Resonant circuit measurement.................................................................................... 8
Use of the capacitive probe......................................................................................... 8
Antenna resonant frequency measurement............................................................... 10
Use as a Signal Generator......................................................................................... 11
Use as Crystal Checker and Marker Generator......................................................... 11
Use as an Absorption Frequency Meter.................................................................... 12
Use as a Field-Strength Meter................................................................................... 13
Capacitance and Inductance Measurements ............................................................. 14
ADJUSTMENT ................................................................................................................ 17
VR1: 01 Bias adj........................................................................................................... 17
VR2: Meter zero adj...................................................................................................... 17
VR3: Sensitivity adj...................................................................................................... 17
VR4: Battery voltage check adj.................................................................................... 17
PARTS AND SERVICE................................................................................................... 17
Ordering Spare Parts..................................................................................................... 17
Service........................................................................................................................... 17
PARTS LIST..................................................................................................................... 18
PRINTED CIRCUIT BOARDS ....................................................................................... 22
SCHEMATIC DIAGRAM ............................................................................................... 24
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KENWOOD DM-81
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KENWOOD DM-81
INTRODUCTION
A dip meter is used for adjustment of radio equipment and antennas. The DM-81 is a
self-excited oscillator designed for external coupling to the equipment being tested. It
features both inductive and capacitive coupling for measuring enclosed coils and toroidal
coils (patent pending). This is not possible with conventional testing instruments.
The DM-81 has the following two functions:
Inductive coupling
As shown (Figure 1A), place the coil unit of the dip meter in close proximity to
the circuit being measured.
Adjust the dial. When the dip meter oscillation frequency coincides with the
resonant frequency (tuned circuit), oscillating energy is absorbed by the circuit,
thus decreasing the oscillation strength.
This strength is indicated on the meter. The pointer swings back momentarily at
the resonant point. Since the meter pointer dips at a tuned point, this instrument is
called a dip meter.
Capacitive coupling
This is a special feature of the DM-81 which is not found in any other dip meter.
The resonant frequency can be checked simply by touching the capacitance probe
to the hot side of the resonant circuit under test, instead of coupling the DM-81's
coil and measuring inductively. The frequency is read directly on the dial. See
Figure 1B.
Radio equipment is miniaturized and most coils are enclosed in metal shields.
Also, toroidal coils are used in many types of radio equipment, and these coils do
not couple to conventional dip meters. The DM-81 has solved this problem.
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KENWOOD DM-81
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KENWOOD DM-81
FEATURES
1. Measurable frequency range is 700kHz to 25OMHz in seven bands.
2. All seven dip meter coils, capacitive probe, earphone and ground clip lead, can be
carried within the unit for easy transport and storage.
3. Convenient for both in indoor and outdoor measurements, all solid-state and builtin battery.
4. HC-25U and FT-243 sockets enable use as a crystal checker and marker
generator.
5. Amplitude modulation is convenient in aligning receivers when using your DM81 as a signal generator. Also, when used as the marker generator, amplitude
modulation is helpful in precisely calibrating the dial scale even for a receiver
having no BFO.
6. An FET and transistor are used in the meter circuit to provide extremely good
sensitivity.
7. As an absorption frequency meter, your DM-81 is used both to align transmitters
and measure field strength.
8. An earphone plug allows you to monitor transmitted signals.
9. A capacitive probe allows measurements without removing coil shields.
10. It is possible to measure resonant circuit frequencies of toroidal coils. This is not
possible with conventional dip meters.
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KENWOOD DM-81
SPECIFICATIONS
700kHz - 250MHz (± 3%)
A band 0.7 - 1.6MHz (± 3%)
B band 1.5 - 3.6MHz (± 3%)
Frequency range:
Modulation: 1 kHz (sine wave)
Power requirements: Battery, 9V(006P)
Power consumption: 9 mA
Semi-conductors: 1 FET, 3 transistors, 3 diodes
C band 3.0 - 7.4MHz (± 3%)
D band 6.9 - 17.5MHz (± 3%)
E band 17 - 42MHz (± 3%)
F band 41 - 110MHz (± 3%)
G band 83 - 250MHz (± 3%)
Crystal oscillator element
to be used:
RF search terminal:
Earphone terminal:
Dimensions: 70W x 180H x 45D (mm)
Weight: Approx. 690g (with accessories)
Accessories:
CAUTION: Do not apply a voltage exceeding 500V (DC + AC peak) to the probe.
HC-25U and FT-243
For measuring resonant frequency (capacitive coupling) and
checking RF voltage using the supplied probe.
Accepts crystal earphone with 3.5ø plug for monitoring
modulated tone.
(1) Coils, A-G bands — 7 pieces
(2) Probe — 1 piece
(3) Ground clip — 1 piece
(4) Crystal earphone — 1 piece
(5) Battery, 006P — 1 piece
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CONTROLS
KENWOOD DM-81
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KENWOOD DM-81
PRECAUTIONS
Battery and Oscillation Coil Loading
Taking the coil compartment out, you will find a battery snap connector inside the unit.
Fit the snap to the battery. First lay the battery take-out ribbon into the battery holder,
then install the battery in place. Place the supplied oscillation coils into the coil
compartment and reinstall into the dip meter main body.
Verify that the battery is serviceable before operating your DM-81. First, turn the
POWER switch on. Set the FUNCTION switch to "BATT CHECK". The battery is
usable as long as the meter pointer is within the "B.C" zone. A low battery results in
weak or unstable oscillation, no oscillation, or frequency error. Replace the battery when
weak.
After use, be sure to turn the POWER switch off. If your DM-81 will not be used for a
long period of time, remove the battery. You can easily remove it by pulling the take-out
ribbon toward you. Never remove the case screws.
Obtaining a Dip Point
The closer the dip meter is brought to the resonant circuit being checked, the tighter the
two are coupled and the deeper the dip point. However, the tuning point becomes so
broad that you cannot find the correct resonant frequency. Therefore, it is advisable to
move the dip meter a little away from the circuit.
Note that the A band has a large pull-in effect and therefore the dip point is broad.
Measuring Transistor Resonant Circuits
There is no load problem in measuring vacuum tube resonant circuits. In measuring some
resonant (tuning) circuits in transistorized transmitters and receivers, the resonant point
cannot always be found by the dipping load. In this event, temporarily disconnect the
transistor or operate the given resonant circuit with power on and measure by absorption.
Caution in Measuring Transmitters
Your DM-81 is usable as an absorption frequency meter in measuring transmitter power
amplifier tank circuits and similar stages producing high RF energy. In rneasurement, do
not abruptly bring the dip meter close to the circuit as the transistors and other parts in the
dip meter could be destroyed by excess RF energy. Bring it near the circuit slowly while
observing the meter pointer.
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KENWOOD DM-81
Caution in Motor Pointer Deflection Change
The meter pointer may swing slightly as if indicating a dip, This results from a variation
in oscillation signal strength while tuning the oscillator variable capacitor. Move the dip
meter coil away from the circuit under measurement. The meter pointer will return to full
scale for a real dip.
APPLICATIONS
Use as a Dip Meter
1. Select an oscillation coil covering the desired frequency range.
2. Install the coil into the socket on top of the dip meter.
3. Set the FUNCTION switch to "OSC".
4. Turn the power on.
5. Turn the SENSITIVITY control until the meter pointer reads at division 0.7. If not to
division 0.7, turn the control fully counter-clockwise.
6. Bring the dip meter coil about 1 cm from the tuned circuit to be measured and slowly
turn the dial. The oscillator signal energy will be absorbed by the tuned circuit at the
resonant point and the meter will dip abruptly. See Figure 3.
Note: At first, couple the dip meter coil tightly to the given tuned circuit so that you
can easily find the dip point. Then, bring the oscillation coil away until the dip is as
narrow as possible, and readjust the dial precisely for an accurate dip point. Now read
the correct frequency on the dial.
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KENWOOD DM-81
Other Frequency Measurements
Resonant circuit measurement
A basic measurement with your DM-81 is a frequency check of resonant (tuned)
circuits comprised of coils and capacitors. In practice, the dip meter is brought
near the coil to be measured as shown in Figure 1A. This illustrates a standard
method of resonant frequency measurement.
Use of the capacitive probe
If a coil to be measured is located in a narrow place and cannot be coupled to the
dip meter coil, or if a coil is enclosed in a shield, the probe can be used for
accurate measurement. See Figure 4.
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KENWOOD DM-81
The dip point can be obtained by using the ground clip and probe for frequencies
of about 50MHz or lower, and the probe only for about 5OMHz and higher.
Toroidal coils can be measured in the same manner. Note that the probe should be
connected to the hot side (not the ground side) of the circuit. See connections (a)
through (e) in the illustration. The dip point is sometimes critical depending on
the circuit or frequency to be measured. An accurate dip point can be obtained by
turning the dial slowly.
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KENWOOD DM-81
Antenna resonant frequency measurement
Any antenna can be regarded as a kind of resonant circuit. Its resonant frequency,
therefore, can be measured as illustrated in Figure 5. For measurement, connect a
one-turn coil to the feed point at the center of the antenna.
Couple it with the dip meter coil. Now, you can obtain the antenna resonant
frequency in a similar manner to APPLICATIONS Section A. For a vertical
antenna or similar antennas for which the other feeder lead is grounded, place the
one-turn coil between the antenna and ground.
Couple the one-turn coil to the dip meter until a dip point is obtained. Then,
slowly separate the coil to measure the resonant frequency accurately.
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KENWOOD DM-81
Use as a Signal Generator
Your DM-81 can be used as a signal generator for aligning receivers and similar
equipment. Couple the dip meter to the antenna circuit of the receiver as
illustrated in Figure 6. The dip meter output carrier will enter the receiver. For
aligning an AM receiver, set the FUNCTION switch to "MOD". The receiver will
sound a 1kHz tone. Aligning SSB and CW receivers can be achieved by leaving
the switch at "OSC" for no modulation. Adjust the capacitor trimmers and
inductor cores for maximum receiver "S" meter reading or maximum speaker
output.
Use as Crystal Checker and Marker Generator
Your DM-81 car, be modified as a crystal checker by installing a crystal in Place
of the oscillation coil (see Figure 7).
You may use either HC-25U or FT-243 crystals. Also, an HC-6U crystal can be
checked if plugged into the FT-243 socket. The oscillation signal strength may
vary depending on the type and frequency of the crystal used. Adjust the dial for
most stable oscillation.
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KENWOOD DM-81
In addition, your DM-81 is applicable as a marker generator by installing a
marker crystal of 1MHz, 3.5MHz, or the like. The marker generator is useful for
calibrating a receiver dial.
Use as an Absorption Frequency Meter
Install an oscillation coil covering the desired frequency range into the socket.
Turn the SENSITIVITY control ON and adjust to the minimum meter deflection
(just before the OFF position of the control), and set the FUNCTION switch to
OSC. You can now use your DM-81 as an absorption frequency meter to receive
external energy and indicate its frequency on the meter.
Figure 8a shows how to measure oscillator frequency. The oscillator coil is
coupled with, or brought near, the absorption frequency meter coil. Adjust the dial
for maximum meter deflection and read the oscillation frequency. Figure 8b
shows the absorption frequency meter coupled to a transmitter tank coil. Its
radiated energy can be measured in a similar manner to that of Figure 8a.
CAUTION:
A transmitter power amplifier stage produces high RF energy. The
absorption frequency meter should be brought near the tank coil slowly so the
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KENWOOD DM-81
meter pointer does not deflect off scale. The earphone ahows you to monitor
modulation.
WARNING:
Tube type power amplifiers operate at high RF and DC potentials.
Transistorized power amps also produce high RF levels. Observe normal safety
procedures for high RF and DC circuits.
Use as a Field-Strength Meter
Your DM-81 can be used to measure the field strength of a transmit antenna. Set
up as directed in APPLICATIONS: "Use as Absorption frequency meter". In
addition, couple to an antenna as in Figure 9. You can now measure field strength.
This application is convenient for transmit antenna matching, radiation pattern
adjustments, and similar uses.
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KENWOOD DM-81
Capacitance and Inductance Measurements
The value of an unknown inductor can be obtained in combination with a known
capacitor by their resonant frequency, as illustrated in Figure 10. Likewise the
value of an unknown capacitor can be calculated. The inductance (L), capacitance
(C), and resonant frequency (f) are related as:
f = 1 / (2π √(LC))
This formula can be rewritten as
L = 25,400 / (f² C)
C = 25,400 / (f² L)
Where
L = inductance in µH
C = capacitance in pF
f = frequency in MHz
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KENWOOD DM-81
An inductance or capacitance can easily be calculated by substituting the known
values into the above equations.
The oscillation coils supplied with your DM-81 are useful as the known inductor.
Their inductances are
BAND INDUCTANCE
A 1250 µH
B 160 µH
C 39 µH
D 8.4 µH
E 1.2 µH
F 0.22 µH
G 0.047 µH
In addition to all these applications, your DM-81 is usable in place of a receiver
local oscillator in repairing or alignment, and is effective in other services as well.
Also, your DM-81 can serve as a BFO for a receiver without one in receiving a
CW or SSB signal. It is useful in a wide variety of situations. By fully
understanding the principles of operation your DM-81's capabilities may be
extended to other applications.
For an additional source of general information, the radio amateur's handbook is
recommended.
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ADJUSTMENT
VR1: 01 Bias adj.
By using G band, adjust VR1 so that the meter pointer deflection is
maximum at 83MHz.
VR2: Meter zero adj.
Adjust VR2 so that the meter deflection is zero when the sensitivity
control/power switch is set to just before the OFF position of the control.
VR3: Sensitivity adj.
Optimum position.
VR4: Battery voltage check adj.
KENWOOD DM-81
Adjust VR4 so that the meter deflection comes to the left edge of the
"B.C" zone at 7V when the FUNCTION switch is set to "B.C" position.
PARTS AND SERVICE
Ordering Spare Parts
When ordering replacement or spare parts for your equipment, be sure to specify the
following:
Model and serial number.
Schematic number of the parts.
Printed circuit board number on which the part is located.
Part number and name, if known, and quantity desired.
Service
Should it ever become necessary to return this equipment for repair, pack in its original
boxes and packing, and include a full description of the problems involved. Also include
your telephone number. You need not return accessory items unless directly related to the
service problem. Tag all returned items with your call for easy I.D.
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KENWOOD DM-81
Please mention the model and serial number of your unit in any correspondence, whether
phone or written. For future reference, record this information in the space provided on
the back cover of this manual.
NOTE:
When claiming warranty service, please include a photocopy of the bill of sale, or other
proof of purchase showing the date of sale.
PARTS LIST
MAIN CHASSIS
Ref.
#
A01-0859-08 Case top
A01-0860-08 Case bottom
A09-0506-08 Coil case
A10-0471-28 Chassis
A29-0502-08 Top panel
B20-0918-28 Dial scale
B23-0602-08 Front glass
B31-0719-08 Meter
Part # Description
AMP UNIT (X73-1350-00)
Ref.
#
Part # Description
RESISTOR
Carbon resistor
R11 RD14BB2E563J
R12 RD14BB2E124J
R13 RD14BB2E683J
56KΩ ±5%
¼W
Carbon resistor
120KΩ ±5%
¼W
Carbon resistor
68KΩ ±5%
¼W
B40-0772-08
B50-2920-00
C01-0191-08
E11-0061-08 Pin jack
E13-0101-05 Phone jack
E18-0207-08
E18-0402-08
18
Name plate
(serial #)
Instruction
manual
Variable
capacitor
Crystal socket
(FT-243)
Crystal socket
R14 RD14BB2E472J
R15 RD14BB2E222J
R16 RD14BB2E561J
VR2 R12-2506-08
VR3 R05-3002-08
Carbon resistor
4.7KΩ ±5%
¼W
Carbon resistor
2.2KΩ ±5%
¼W
Carbon resistor
560Ω ±5% ¼W
Semi-fixed
resistor 5KΩ
Variable
resistor (with
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KENWOOD DM-81
E29-0524-08 Probe
E30-1839-08 Ground clip
E91-0401-08 Battery snap
F20-0619-08
H01-2914-08
H12-0533-08
Insulating
plate
Packing case
(inside)
Pad (formed
styrene)
H19-0507-08 Accessory box
H25-0165-08
H25-0166-08
Polyethylene
bag
Polyethylene
bag
J19-0477-08 Battery holder
J21-1460-08
Coil mounting
hardware
CAPACITOR
C11 CE04W1C100
Electrolytic
10µF 16WV
SEMI-CONDUCTOR
FET 2SK19
(GR)
Transistor
2SA719
Zener diode
RD-6, 2EB
MISCELLANEOUS
K29-0256-08 Knob
J25-2888-08
Printed circuit
board
HIGH FREQUENCY UNIT (XB4-1040-
00)
Variable
J21-1461-08
capacitor
mounting
hardware
J25-1279-08
Printed circuit
board
K29-0254-08 Push-button
K29-0255-08 Dial
L37-0017-08 Coil A
L37-0018-08 Coil B
L37-0019-08 Coil C
L37-0020-08 Coil D
L37-0021-08 Coil E
L37-0022-08 Coil F
Ref. # Part # Description
RESISTOR
Carbon
R1 RD14BB2E562J
resistor
5.6KΩ ±5%
¼W
Carbon
R2,6,7 RD14BB2E124J
resistor
120KΩ ±5%
¼W
Carbon
R3 RD14BB2E222J
resistor
2.2KΩ ±5%
¼W
Carbon
R4 RD14BB2E471J
resistor 470Ω
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KENWOOD DM-81
Battery 006P
9V
Ceramic
C12 CC45SL2H050C
capacitor 5pF
500WV
Ceramic
C13 CK45D1H103M
capacitor
0.01µF ±20%
Carbon resistor
R17 RD14BB2E393J
39KΩ ±5%
¼W
Semi-fixed
VR4 R12-3513-08
resistor
20KΩB
T18-0052-08 Earphone
S32-2001-15 Slide switch
X73-1350-00 AMP unit
X84-1040-00
High
frequency unit
R5,8 RD14BB2E103J
R9 RD14BB2E472J
R10 RD14BB2E221J
VR1 R12-3511-08
CAPACITOR
C1 CC45SL1H470J
C2 CC45SL1H030C
C3 CC45SL1H010C
Carbon
resistor
10KΩ ±5%
¼W
Carbon
resistor
4.7KΩ ±5%
¼W
Carbon
resistor 220Ω
±5% ¼W
Semi-fixed
resistor
20KΩB
Ceramic
47pF ±5%
Ceramic 3pF
±0.25pF
Ceramic 1pF
±0.25pF
C4 CK45D1H103M
C5,7 CK45D1H102M
C6 CC45SL1H101J
C8-10 CQ92M1H472K
C14 CC45SL1H050C
SEMI-CONDUCTOR
Q1
Ceramic
0.01µF ±20%
Ceramic
0.001µF
±20%
Ceramic
100pF ±5%
Mylar
4700pF
±10%
Ceramic 5pF
±0.25pF
Transistor
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KENWOOD DM-81
Q2
Transistor
2SC945 (K)
D1,2 Diode 1SS16
MISCELLANEOUS
L33-0262-08
J25-2887-08
Feri-inductor
2mH
Printed
circuit board
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PRINTED CIRCUIT BOARDS
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KENWOOD DM-81
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KENWOOD DM-81
SCHEMATIC DIAGRAM
Unless otherwise specified, resistors are ¼W and ±5%. Also, the circuit elements may be changed without
notice owing to a technical innovation.
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