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Oscillator blocking

The Armstrong oscillator on page 181 can be modified to produce only a single pulse, which would be half of a complete up-and-down sine wave. This is called a blocking oscillator or a one-shot oscillator, and it would be similar to the relay-operated pulse generator on page 134, using the NC contacts and [Pg.185]


In testing DC/DC converter transformer shorts, the could give information only on very crude faults. A more approach is when the ohm meter is connected into the circuit of a transistor (minimum beta - 45) in series primary of the transformer under testing. The secondary in the base circuit to form a "blocking oscillator", as Fig. 11.7. Note the correct coll connection directions with the dots. [Pg.248]

Another reason could be a short circuit in the transformer. This can be checked for with the previously described "blocking oscillator" test. [Pg.253]

If there is no detector voltage, first the blocking oscillator should be tested for operation. If the base of Q102 is driven from outside with a variable voltage from a helical potentiometers wiper, the operation of the amplifier stages could be easily checked. [Pg.254]

Fig. 1 shows the block diagram of the vibrometer, in which the most sensible to small phase variations interferometric scheme is employed. It consists of the microwave and the display units. The display unit consists of the power supply 1, controller 2 of the phase modulator 3, microprocessor unit 9 and low-frequency amplifier 10. The microwave unit contains the electromechanical phase modulator 3, a solid-state microwave oscillator 4, an attenuator 5, a bidirectional coupler 6, a horn antenna 7 and a microwave detector 11. The horn antenna is used for transmitting the microwave and receiving the reflected signal, which is mixed with the reference signal in the bidirectional coupler. In the reference channel the electromechanical phase modulator is used to provide automatic calibration of the instrument. To adjust the antenna beam to the object under test, the microwave unit is placed on the platform which can be shifted in vertical and horizontal planes. [Pg.655]

Structure of installation enter the source-receiver of acoustic oscillations, block of ultrasonic transducers, system of scanning, control system engines, block of the analysis and registration. [Pg.883]

The electronic block, which includes block of the analysis and registration and control system engines, and block of the source-receiver of acoustic oscillations are universal for any installations of this type. As the source-receiver of acoustic oscillations the ultrasonic flow detector is usually use. It s, as a rule, the serial devices for example y/f2-12. The electronic block contains the microprocessor device or PC, device of the power supply and management of engines... [Pg.883]

Note Because of its neglect of off-diagonal blocks, this optimizer can sometimes oscillate and fail to converge. In this case, use a conjugate gradicn t method. [Pg.60]

A typical large three-phase ferroalloy furnace using prebaked carbon electrodes is shown in Eigure 4. The hearth and lower walls where molten materials come in contact with refractories are usually composed of carbon blocks backed by safety courses of brick. In the upper section, where the refractories are not exposed to the higher temperatures, superduty or regular firebrick may be used. The walls of the shell also may be water-cooled for extended life. Usually, the furnace shell is elevated and supported on beams or on concrete piers to allow ventilation of the bottom. When normal ventilation is insufficient, blowers are added to remove the heat more rapidly. The shell also may rest on a turntable so that it can be oscillated slightly more than 120° at a speed equivalent to 0.25—1 revolution per day in order to equalize refractory erosion or bottom buildup. [Pg.123]

A. P. J. Jansen, R. M. Nieminen. A Monte Carlo study of CO oxidation with oscillations induced by site blocking. J Chem Phys 706 2038-2044, 1997. [Pg.434]

The assumption of independent oscillators allows us to study a simplified system containing only one atom, as illustrated in Fig. 14 where x and Xq denote, respectively, the coordinates of the atom and the support block (substrate). The dynamic analysis for the system in tangential sliding is similar to that of adhesion, as described in the previous section. For a given potential V and spring stiffness k, the total energy of the system is again written as... [Pg.173]

The ballistic mortar and lead block tests use only small amounts of explosive and are not applicable to slurry explosives which are too insensitive to detonate properly under such conditions. For these explosives it is useful to fire larger amounts of several kg under water and measure the period of oscillation of the gas bubble produced. The longer the period the greater the energy of the gas bubble and this part of the total energy of the explosive has been found to correlate well with the blasting effect of the explosive. [Pg.64]

Therefore, the strip was sticking out from the Cu top to avoid oscillations of the sample, the second copper block (D) was tied to a fibreglass stick (E) attached to the copper top by means of a thin PTFE wire (F) of negligible thermal conductance. The electrical connections of the thermometer (TH) and the heater (FI) was made by eight manganin wires (G), 100 xm in diameter. Another thermometer (Tc) was used to monitor the temperature of the cold end of the sample. An LR700 AC resistance bridge was used to read the resistance of the thermometers. [Pg.265]

Fig. 1. Typical a.c. plasma systems used for hydrogenation of semiconductor samples. A. In this aparatus, hydrogen is pumped through the quartz tube (Q) and a plasma excited by inductive coupling of 13.56 MHz r.f. power with a copper coil (c2). The sample rests on a graphite block (b) that is heated by 440 KHz power coupled by a second coil (cl). A pyrometer (P) measures the sample temperature. B. In this system, a high frequency oscillator is used for plasma excitation while the sample is heated in a tube furnace (Pearton et al., 1987). Fig. 1. Typical a.c. plasma systems used for hydrogenation of semiconductor samples. A. In this aparatus, hydrogen is pumped through the quartz tube (Q) and a plasma excited by inductive coupling of 13.56 MHz r.f. power with a copper coil (c2). The sample rests on a graphite block (b) that is heated by 440 KHz power coupled by a second coil (cl). A pyrometer (P) measures the sample temperature. B. In this system, a high frequency oscillator is used for plasma excitation while the sample is heated in a tube furnace (Pearton et al., 1987).

See other pages where Oscillator blocking is mentioned: [Pg.185]    [Pg.186]    [Pg.254]    [Pg.185]    [Pg.186]    [Pg.254]    [Pg.540]    [Pg.595]    [Pg.602]    [Pg.145]    [Pg.166]    [Pg.375]    [Pg.668]    [Pg.792]    [Pg.169]    [Pg.813]    [Pg.331]    [Pg.136]    [Pg.294]    [Pg.17]    [Pg.160]    [Pg.183]    [Pg.259]    [Pg.47]    [Pg.714]    [Pg.190]    [Pg.201]    [Pg.228]    [Pg.6]    [Pg.189]    [Pg.276]    [Pg.299]    [Pg.703]    [Pg.710]    [Pg.157]    [Pg.429]    [Pg.159]    [Pg.31]   
See also in sourсe #XX -- [ Pg.185 ]




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