ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING
Propeller speed control. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Electric motors When working out propeller installations of snowmobiles, motor hang gliders, airplanes, as well as aircraft models, the designer needs to know the exact values of a number of parameters. And most importantly - the speed of the propeller. This is necessary both when boosting engines and when choosing a propeller. The rotational speed is also one of the main parameters during the operation of the motor: by the value of this parameter, one can objectively judge the reliability of the engine. In many cases, it is simply impossible to “attach” any of the standard tachometers to a propeller-driven installation: Well, when it comes to model engines, contact measurements can distort their operation so much that any subtleties of adjustment are out of the question. I bring to the attention of readers a non-contact electronic tachometer designed to measure the speed of the propeller without using any mechanical connections between the sensor and the engine shaft. The tachometer consists of two main parts - a sensor and a frequency counter (Fig. 1).
The sensor generates pulse signals that follow with a frequency that is a multiple of the speed of rotation of the propeller. The multiplicity is determined by the number of blades. Two types of sensors can be used for this tachometer: electrostatic and optical. An electrostatic sensor designed specifically for the described device converts the charge accumulated on the blades of a rotating propeller during friction against air into a pulsed voltage. To do this, the sensor has a sensitive element (Fig. 2) - a narrow antenna made of a metal plate or wire, installed parallel to the plane of rotation of the screw.
When the charged blades pass by the antenna, an alternating voltage will be induced in it, the frequency of which will be determined by the expression (K * N) / 60, where K is the number of propeller blades, N is the propeller speed (rpm). The electrostatic sensor antenna is a source of low (on the order of millivolts) voltage with a very high internal resistance equal to the insulation resistance. To ensure the normal operation of the frequency meter, this voltage is supplied to an amplifier with a high input impedance (Fig. 3).
High input impedance is achieved by using a matching stage, which is a combination of a flux follower on a field effect transistor VT1 and an emitter follower on a bipolar transistor VT2. Operational amplifier DA1 provides signal amplification to a level sufficient to operate the frequency counter. An optical sensor consists of a light source, a sensitive element - a photodiode or a photoresistor - and an amplifier. The light source and the sensing element are positioned so that the beam passes through the plane of the screw. During rotation, the blades periodically cross the beam incident on the sensitive element connected between the base and the emitter (Fig. 4), periodically changing its resistance and thereby forming an alternating voltage on the base of the transistor.
The received pulses are amplified by a two-stage amplifier to a value sufficient for the operation of the frequency meter. The frequency meter converts the pulses received by the transmitters into a direct current proportional to the pulse repetition rate. Its main element is a waiting multivibrator on transistors VT5 and VT6 (Fig. 5).
When signals from sensors arrive at the waiting multivibrator, it generates pulses of constant duration, determined only by the values of the resistors and capacitances of the circuit. When the screw rotates, a sequence of pulses with a constant amplitude and duration is formed at the output of the waiting multivibrator, the repetition rate of which is proportional to the speed of rotation of the screw. The resulting pulse sequence contains a constant component, the value of which depends on the so-called duty cycle - the ratio of the pulse repetition period to their duration, that is, on the speed of rotation of the screw. The DC component is extracted by integrating the pulse sequence. The integrating element is the RA1 pointer device, which simultaneously serves to indicate the speed of rotation of the propeller. In this case, a 100 μA magnetoelectric head was used with an additional resistor R22. A coarser instrument may also be used. Variable resistor R21 is used when calibrating the tachometer. An emitter follower on a VT7 transistor is used to decouple the integrator and the waiting multivibrator. The device is powered from batteries or from a 9,5 V rectifier. In the manufacture of a tachometer, any design can be adopted, but the most appropriate is the design in the form of two blocks - a sensor and a frequency meter with an indicator, interconnected by a three-wire cable. An electrostatic sensor must be carefully shielded. The sensor antenna can be made of a piece of copper wire, a narrow strip of brass or foil fiberglass. During measurements, it should be parallel to the plane of rotation of the screw at a distance that ensures normal operation of the device. To improve the accuracy of measuring the speed of rotation of the propeller, before starting work, it is necessary to calibrate the tachometer, for which a calibrator (built-in or remote) is included in its composition. The calibrator is a multivibrator (Fig. 6) that generates short pulses, the repetition rate of which is determined by the values of resistors R24, R25 and capacitances C6, C7 and is selected based on the range of measured speeds. For sufficient measurement accuracy, calibration should be carried out at two or three points in the velocity range. In this case, the required pulse repetition rates for a two-blade propeller are determined by the expression f=N/30.
The table (see Fig. 6) shows the values of resistors R24 and R25 for various screw speeds. Precise frequency setting is carried out by a tuning resistor R30, while the frequency setting is controlled using a high-precision digital frequency meter. You can get several frequencies by stepping resistors R24 and R25 or by using several generators. Author: V.Evstratov See other articles Section Electric motors. Read and write useful comments on this article. Latest news of science and technology, new electronics: Machine for thinning flowers in gardens
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