Showing posts with label astable. Show all posts
Showing posts with label astable. Show all posts

Wednesday, July 7, 2010

Astable Operation


555 astable operationWith the output high (+Vs) the capacitor C1 is charged by current flowing through R1 and R2. The threshold and trigger inputs monitor the capacitor voltage and when it reaches 2/3Vs (threshold voltage) the output becomes low and the discharge pin is connected to 0V.

The capacitor now discharges with current flowing through R2 into the discharge pin. When the voltage falls to 1/3Vs (trigger voltage) the output becomes high again and the discharge pin is disconnected, allowing the capacitor to start charging again.

This cycle repeats continuously unless the reset input is connected to 0V which forces the output low while reset is 0V.

An astable can be used to provide the clock signal for circuits such as counters.

A low frequency astable (<>

An audio frequency astable (20Hz to 20kHz) can be used to produce a sound from a loudspeaker or piezo transducer. The sound is suitable for buzzes and beeps. The natural (resonant) frequency of most piezo transducers is about 3kHz and this will make them produce a particularly loud sound.

Duty cycles

Duty cycle

The duty cycle of an astable circuit is the proportion of the complete cycle for which the output is high (the mark time). It is usually given as a percentage.

For a standard 555/556 astable circuit the mark time (Tm) must be greater than the space time (Ts), so the duty cycle must be at least 50%:

Duty cycle = Tm = R1 + R2
Tm + TsR1 + 2R2

555 astable circuit with diode across R2

555 Astable Multivibrator


555 astable output
555 astable output, a square wave
(Tm and Ts may be different)
555 astable circuit
555 astable circuit
An astable circuit using 555 produces a square wave. Figure shows a digital waveform with sharp transitions between low 0V and high. The durations of the low and high states may be different. The time period (T) of the square wave is the time for one complete cycle, but it is usually better to consider frequency(f) which is the number of cycles per second.

T = 0.7 × (R1 + 2R2) × C1 and f = 1.4
(R1 + 2R2) × C1

T = time period in seconds (s)
f = frequency in hertz (Hz)
R1 = resistance in ohms (ohm)
R2 = resistance in ohms (ohm)
C1 = capacitance in farads (F)

The time period can be split into two parts: T = Tm + Ts
Mark time (output high): Tm = 0.7 × (R1 + R2) × C1
Space time (output low): Ts = 0.7 × R2 × C1

Choosing R1, R2 and C1

555 astable frequencies
C1R2 = 10kohm
R1 = 1kohm
R2 = 100kohm
R1 = 10kohm
R2 = 1Mohm
R1 = 100kohm
0.001µF68kHz6.8kHz680Hz
0.01µF6.8kHz680Hz68Hz
0.1µF680Hz68Hz6.8Hz
1µF68Hz6.8Hz0.68Hz
10µF6.8Hz0.68Hz
(41 per min.)
0.068Hz
(4 per min.)
R1 and R2 should be in the range 1kohm to 1Mohm. It is best to choose C1 first because capacitors are available in just a few values.
  • Choose C1 to suit the frequency range you require (use the table as a guide).
  • Choose R2 to give the frequency (f) you require. Assume that R1 is much smaller than R2 (so that Tm and Ts are almost equal), then you can use:
    R2 = 0.7
    f × C1
  • Choose R1 to be about a tenth of R2 (1kohm min.) unless you want the mark time Tm to be significantly longer than the space time Ts.
  • If you wish to use a variable resistor it is best to make it R2.
  • If R1 is variable it must have a fixed resistor of at least 1kohm in series
    (this is not required for R2 if it is variable).