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Index 128



Keyed_oscillator

Published:2009/7/24 6:03:00 Author:Jessie

Keyed_oscillator
In this circuit, one timer section of an XR-L556 is operated in the free-running mode, and is keyedon and off by the other section. The circuit output (timer 2) appears as a tone burst, whose frequency is set by RA, RB, and C2, and whose duration is set by R1 and C1. EXAR Corporation Databook, 1990, p. 5-222.   (View)

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Sequential_timing_delayed_one_shot

Published:2009/7/24 6:01:00 Author:Jessie

Sequential_timing_delayed_one_shot
In this circuit, the output of one timer section triggers the other section so that the output of T2 is delayed from the initial trigger at pin 6 by a time delay of T1. Both T1 and T2 are set by values of external components, as shown. EXAR Corporation Databook, 1990 , p. 5-221.   (View)

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Independent_time_delay

Published:2009/7/24 6:00:00 Author:Jessie

Independent_time_delay
This circuit uses both sections of an XR-L556 dual timer to produce two independent time delays. Each section is used separately in the monostable mode to produce respective time delays T1 and T2. EXAR Corporation Databook, 1990 , p. 5-221.   (View)

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Astable_free_running

Published:2009/7/24 5:59:00 Author:Jessie

Astable_free_running
This circuit uses one section of an XR-L556 dual timer. Output frequency and duty cycle are set by C and R (Fig. 5-12B). Notice that R=RA + 2RB (Fig. 5-12B). EXAR Corporaton Databook, 1990, p. 5-218/5-221.   (View)

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Monostable_one_shot

Published:2009/7/24 5:57:00 Author:Jessie

Monostable_one_shot
This circuit uses one section of an XR-L556 dual timer. Duration of the output pulse is set by C and RA (Fig. 5-11B). RL should equal the load being driven. EXAR Corporation Databook, 1990 , p. 5-218/5-220.   (View)

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Square_wave_oscillator

Published:2009/7/24 5:47:00 Author:Jessie

Square_wave_oscillator
This circuit uses only one section of an LP165/365 comparator, and produces square waves at a frequency that is determined by the values of R and C, as shown. Raytheon Linear Integrated Circuts, 1989, p. 5-42.   (View)

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Crystal_controlled_oscillator

Published:2009/7/24 5:46:00 Author:Jessie

Crystal_controlled_oscillator
This circuit uses only one section of an LP165/365 comparator,and produces pulses at 100 kHz using the values shown, with a single supply. Raytheon Linear Integrated Circuts, 1989, p. 5-42.   (View)

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Crystal_stabilized_relaxation_oscillator

Published:2009/7/24 7:50:00 Author:Jessie

Crystal_stabilized_relaxation_oscillator
This circuit shows an LT1011 connected as a simple relaxation oscillator with crystal control. Figure 5-28B shows the corresponding waveforms. Waveform A is taken from the inverting ( -) input of the LT1011, while waveform B is taken from the LT1011 output. Linear Technology Corporation. Linear Appications Handbook, 1990, p. AN12-3, -2.   (View)

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Simple_clock_oscillators

Published:2009/7/24 7:48:00 Author:Jessie

Simple_clock_oscillators
These circuits show four basic clock oscillators composed of digital IC gates, and a discrete-component oscillator, all of which are well suited as clock sources. Notice that the diodes used in the discrete-component oscillator can be 1N4148s or equivalent. Linear Technology Corporation, Linear Applications Handbook, 1990, p. AN12-2.   (View)

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High_purity_sine_wave_generator

Published:2009/7/24 7:46:00 Author:Jessie

High_purity_sine_wave_generator
By combining a MAX270 4th-order low-pass filter, a 74HC163 counter, and an 8-channel analog MUX, high-purity 1- to 25-kHz sine waves are generated with a THD of less than -80 dB. The low-pass filter is set to the desired frequency and a clock 8 times the sine frequency is applied to the 74HC163 counter. The MAX270 uncommitted op amp sets the filter output level. Gain accuracy is set by the MAC270 gain at the corner frequency, which is guaranteed between -2.4 and -3.6 dB at 1 kHz. The 100-kΩ potentiometer provides gain control if desired. Two resistor dividers provide the input voltages that are required at the MUX inputs. When the MUX switches through channels 0 to 7, an 8-times oversampled staircase approximation of a sine wave is generated. Compared with a square wave, the oversampled waveform greatly reduces smoothing-filter requirements by pushing the first significant harmonic out to 7 times the fundamental. All higher-order harmonics are filtered to below -80 dB by the MAX270. Maxim , 1992, Applications and Product Highlights, p. 7-7.   (View)

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15_V_powered_temperature_compensated_crystal_oscillator

Published:2009/7/24 7:44:00 Author:Jessie

15_V_powered_temperature_compensated_crystal_oscillator
This fully temperature-compensated oscillator is operated from a 1.5-V source (single battery) and draws only 230-μA current, making the circuit ideal for portable high-accuracy clocks, survival radios, and secure communications. Linear Technology Corporation, 1991, AN45-14.   (View)

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Quartz_stabilized_4_kHz_oscillator_with_9_ppm_distortion

Published:2009/7/24 7:40:00 Author:Jessie

Quartz_stabilized_4_kHz_oscillator_with_9_ppm_distortion
A spectrally pure sine-wave oscillator is required for data converter, filter, and audio testing. This oscillator has less than 9 ppm (0.0009%) distortion in the 10-Vpp output. The circuit is adjusted for minimum distortion by adjusting the 50-kΩ potentiometer while monitoring the A3 output with a distortion analyzer. This trim sets the voltage across the photocell to the optimum value for lowest distortion. Linear Technology Corporation, 1991, AN45-12.   (View)

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HIGH_DRIVE_OSCILLATOR_FLSHER

Published:2009/6/30 23:34:00 Author:May

HIGH_DRIVE_OSCILLATOR_FLSHER
The driver in the package is connected as a Schmitt trigger oscillator (A) where R1 and R2 are used to generate hysteresis. R3 and C are the inverting feedback timing elements and R4 is the pull-down load for the first driver. Because of its current capability, the circuit can be used to drive an array of LEDs or lamps. If resistor R4 is replaced by an LED (plus a current limiting resistor), the circuit becomes a double flasher with the 2 LEDs flashing out of phase (B).   (View)

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LOW_FREQUENCY_OSCILLATOR_FLASHER

Published:2009/6/30 23:29:00 Author:May

LOW_FREQUENCY_OSCILLATOR_FLASHER
Electrolytic capacitors are unnecessary to generate a 1 cps frequency. As an scs triggers on, the 0.2 μF commutating capacitor turns off the other one and charges its gate capacitor to a negative potential. The gate capacitor charges towards 24 volts through 20 M retriggering its scs. Battery power is delivered to the load with 88% efftciency.The 20 M resistors can be varied to change prf or duty fact   (View)

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2_MHz_CRYSTAL_USING_CMOS_PAIR

Published:2009/6/30 23:13:00 Author:May

2_MHz_CRYSTAL_USING_CMOS_PAIR
One CMOS transistor pair from CA3600E array is connected with feedback pinetwork to glve sta-ble oscilIator performance with 2-MHz crystal.Low power drain makes circuit ideal for use in digital clocks and watches.- Linear Integrated Circuits and MOS/FET's, RCA Solid State Divi-sion, Somerville, NJ, 1977, p 280.   (View)

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Vpp_GENERATOR_FOR_EPROMS

Published:2009/6/30 22:34:00 Author:May

Vpp_GENERATOR_FOR_EPROMS
  (View)

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RE_OSCILLATOR

Published:2009/6/30 3:05:00 Author:May

RE_OSCILLATOR
This rf oscillator is useful up to 30 MHz.An SK 3007 PNP transistor is recommended.   (View)

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COLPITTS_OSCILLATOR

Published:2009/6/30 3:04:00 Author:May

COLPITTS_OSCILLATOR
When calculating its resonan frequency,use C1C2/C1+C2 for the total capacitance ofthe L-C circuit.   (View)

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27_MHz_AND_49_MHz_RE_OSCILLATOR_TRANSMITTER

Published:2009/6/30 3:00:00 Author:May

27_MHz_AND_49_MHz_RE_OSCILLATOR_TRANSMITTER
The modulator and oscillator consist of two NPN transistors. The base of the modulator transistor is driven by a bidirectional current source with the voltage range for the high condition limited by a saturating PNP collector to the pin 4 VREG voltage and low condition limited by a saturating NPN collector in series with a diode to ground. The crystal oscillator/transmi tter transistor is configured to oscillate in a class C mode. Because third overtone crystals are used for 27 MHz or 49 MHz applications a tuned collector load must be used to guarantee operation at the correct frequency.   (View)

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Feedback_measurement

Published:2009/7/24 20:36:00 Author:Jessie

Feedback_measurement
Because op-amp circuits usually include feedback, it is sometimes necessary to measure feedback voltage at a given frequency with given operating conditions.The basic feedback-measurement connections are shown in Fig. 10-A. Although it is possible to measure the feedback voltage, as shown in Fig. 10-Aa, a more accurate measurement is made when the feedback lead is terminated in the normal operating impedance(Fig.10-Ba).If an input resistance is used In thecircuit,and this resistance is considerably lower than the IC inputimpedance,usethe resistance value.If In doubt, measure the input impedance of the IC(asdescribed In chapter 1). Then,terminate the feedback lead In that value(tomeasure open-loop feedback voltage). Remember that open-loop voltage gammust be substantially higher than the closed-loop voltage gam for most Op-ampcircuits to perform properly.   (View)

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