Kenwood_DM-81_user.pdf

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 KENWOOD DM-81 KENWOOD DM-81 1 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-81s 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. KENWOOD DM-81 2 KENWOOD DM-81 3 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 built- in 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 DM- 81 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. KENWOOD DM-81 4 SPECIFICATIONS Frequency range: 700kHz - 250MHz ( 3%) A band 0.7 - 1.6MHz ( 3%) B band 1.5 - 3.6MHz ( 3%) 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%) Modulation: 1 kHz (sine wave) Power requirements: Battery, 9V(006P) Power consumption: 9 mA Semi-conductors: 1 FET, 3 transistors, 3 diodes Crystal oscillator element to be used: HC-25U and FT-243 RF search terminal: For measuring resonant frequency (capacitive coupling) and checking RF voltage using the supplied probe. Earphone terminal: Accepts crystal earphone with 3.5 plug for monitoring modulated tone. Dimensions: 70W x 180H x 45D (mm) Weight: Approx. 690g (with accessories) Accessories: (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 CAUTION: Do not apply a voltage exceeding 500V (DC + AC peak) to the probe. KENWOOD DM-81 5 CONTROLS KENWOOD DM-81 6 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. KENWOOD DM-81 7 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. KENWOOD DM-81 8 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. KENWOOD DM-81 9 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. KENWOOD DM-81 10 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. KENWOOD DM-81 11 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. KENWOOD DM-81 12 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 a