The 555 timer IC is an amazingly simple yet versatile device. It has
been around now for many years and has been reworked into a number of
different technologies. The two primary versions today are the original
bipolar design and the more recent CMOS equivalent. These differences
primarily affect the amount of power they require and their maximum
frequency of operation; they are pin-compatible and functionally
interchangeable.
This page contains only a description of the 555 timer IC itself.
Functional circuits and a few of the very wide range of its possible
applications will be covered in additional pages in this category.
The figure to the right shows the functional block diagram of the 555
timer IC. The IC is available in either an 8-pin round TO3-style can or an
8-pin mini-DIP package. In either case, the pin connections are as
follows:
- Ground.
- Trigger input.
- Output.
- Reset input.
- Control voltage.
- Threshhold input.
- Discharge.
- +VCC. +5 to +15 volts in normal use.
The operation of the 555 timer revolves around the three resistors that
form a voltage divider across the power supply, and the two comparators
connected to this voltage divider. The IC is quiescent so long as the
trigger input (pin 2) remains at +VCC and the threshhold input
(pin 6) is at ground. Assume the reset input (pin 4) is also at
+VCC and therefore inactive, and that the control voltage input
(pin 5) is unconnected. Under these conditions, the output (pin 3) is at
ground and the discharge transistor (pin 7) is turned on, thus grounding
whatever is connected to this pin.
The three resistors in the voltage divider all have the same value (5K
in the bipolar version of this IC), so the comparator reference voltages
are 1/3 and 2/3 of the supply voltage, whatever that may be. The control
voltage input at pin 5 can directly affect this relationship, although
most of the time this pin is unused.
The internal flip-flop changes state when the trigger input at pin 2 is
pulled down below +VCC/3. When this occurs, the output (pin 3)
changes state to +VCC and the discharge transistor (pin 7) is
turned off. The trigger input can now return to +VCC; it will
not affect the state of the IC.
However, if the threshhold input (pin 6) is now raised above
(2/3)+VCC, the output will return to ground and the discharge
transistor will be turned on again. When the threshhold input returns to
ground, the IC will remain in this state, which was the original state
when we started this analysis.
The easiest way to allow the threshhold voltage (pin 6) to gradually
rise to (2/3)+VCC is to connect it to a capacitor being allowed
to charge through a resistor. In this way we can adjust the R and C values
for almost any time interval we might want.
The 555 can operate in either monostable or astable mode, depending on
the connections to and the arrangement of the external components. Thus,
it can either produce a single pulse when triggered, or it can produce a
continuous pulse train as long as it remains powered.
In monostable mode, the timing interval, t, is set by a single resistor
and capacitor, as shown to the right. Both the threshhold input and the
discharge transistor (pins 6 & 7) are connected directly to the capacitor,
while the trigger input is held at +VCC through a resistor. In
the absence of any input, the output at pin 3 remains low and the
discharge transistor prevents capacitor C from charging.
When an input pulse arrives, it is capacitively coupled to pin 2, the
trigger input. The pulse can be either polarity; its falling edge will
trigger the 555. At this point, the output rises to +VCC and
the discharge transistor turns off. Capacitor C charges through R towards
+VCC. During this interval, additional pulses received at pin 2
will have no effect on circuit operation.
The standard equation for a charging capacitor applies here:
e = E(1 - (-t/RC)). Here, "e" is the capacitor voltage at
some instant in time, "E" is the supply voltage, VCC,
and "" is the base
for natural logarithms, approximately 2.718. The value "t"
denotes the time that has passed, in seconds, since the capacitor started
charging.
We already know that the capacitor will charge until its voltage
reaches (2/3)+VCC, whatever that voltage may be. This doesn't
give us absolute values for "e" or "E," but it does
give us the ratio e/E = 2/3. We can use this to compute the
time, t, required to charge capacitor C to the voltage that will activate
the threshhold comparator:
- 2/3 = 1 - (-t/RC)
- -1/3 = -(-t/RC)
- 1/3 = (-t/RC)
- ln(1/3) = -t/RC
- -1.0986123 = -t/RC
- t = 1.0986123RC
- t = 1.1RC
The value of 1.1RC isn't exactly precise, of course, but the roundoff
error amounts to about 0.126%, which is much closer than component
tolerances in practical circuits, and is very easy to use. The values of R
and C must be given in Ohms and Farads, respectively, and the time will be
in seconds. You can scale the values as needed and appropriate for your
application, provided you keep proper track of your powers of 10. For
example, if you specify R in megohms and C in microfarads, t will still be
in seconds. But if you specify R in kilohms and C in microfarads, t will
be in milliseconds. It's not difficult to keep track of this, but you must
be sure to do it accurately in order to correctly calculate the component
values you need for any given time interval.
The timing interval is completed when the capacitor voltage reaches the
(2/3)+VCC upper threshhold as monitored at pin 6. When this
threshhold voltage is reached, the output at pin 3 goes low again, the
discharge transistor (pin 7) is turned on, and the capacitor rapidly
discharges back to ground once more. The circuit is now ready to be
triggered once again.
If we rearrange the circuit slightly so that both the trigger and
threshhold inputs are controlled by the capacitor voltage, we can cause
the 555 to trigger itself repeatedly. In this case, we need two resistors
in the capacitor charging path so that one of them can also be in the
capacitor discharge path. This gives us the circuit shown to the left.
In this mode, the initial pulse when power is first applied is a bit
longer than the others, having a duration of 1.1(Ra + Rb)C. However, from
then on, the capacitor alternately charges and discharges between the two
comparator threshhold voltages. When charging, C starts at
(1/3)VCC and charges towards VCC. However, it is
interrupted exactly halfway there, at (2/3)VCC. Therefore, the
charging time, t1, is
-ln(1/2)(Ra + Rb)C = 0.693(Ra + Rb)C.
When the capacitor voltage reaches (2/3)VCC, the discharge
transistor is enabled (pin 7), and this point in the circuit becomes
grounded. Capacitor C now discharges through Rb alone. Starting at
(2/3)VCC, it discharges towards ground, but again is
interrupted halfway there, at (1/3)VCC. The discharge time, t2,
then, is -ln(1/2)(Rb)C = 0.693(Rb)C.
The total period of the pulse train is t1 + t2, or
0.693(Ra + 2Rb)C. The output frequency of this circuit is the
inverse of the period, or 1.44/(Ra + 2Rb)C.
Note that the duty cycle of the 555 timer circuit in astable mode
cannot reach 50%. On time must always be longer than off time, because Ra
must have a resistance value greater than zero to prevent the discharge
transistor from directly shorting VCC to ground. Such an action
would immediately destroy the 555 IC.
One interesting and very useful feature of the 555 timer in either mode
is that the timing interval for either charge or discharge is independent
of the supply voltage, VCC. This is because the same
VCC is used both as the charging voltage and as the basis of
the reference voltages for the two comparators inside the 555. Thus, the
timing equations above depend only on the values for R and C in either
operating mode.
In addition, since all three of the internal resistors used to make up
the reference voltage divider are manufactured next to each other on the
same chip at the same time, they are as nearly identical as can be.
Therefore, changes in temperature will also have very little effect on the
timing intervals, provided the external components are temperature stable.
A typical commercial 555 timer will show a drift of 50 parts per million
per Centigrade degree of temperature change (50 ppm/°C) and
0.01%/Volt change in VCC. This is negligible in most practical
applications.
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