Hi again,
A lot of times when you have two parameters that seem to be able to vary one
of them ends up being dependent on something else too. For example, one
resistor value may be the coil ohms instead of an actual resistor and so
you have to go with that. In times when they can both vary then you have
to ask yourself if something else enters the picture too which helps to fix
or limit the range of one of the two parameters.
Of course sometimes we want to study the effects of BOTH parameters varying
and for that we would simply resort to moving to a dimension one more than we
are currently working in. That is, we would look at several values of say R and C
letting R vary from say 100 to 500 ohms in steps of 100 ohms and for each R
we let C be maybe 500uf to 2000uf (500uf steps) and consider the results from all of these
combinations. For that example of R and C, we would end up with 5 values for R
and 4 values for C, where each value of C is used with each value of R. This would
result in a total of 4 times 5 or 20 different results which we could look at and
this might give us some more insight for picking the right two values, or it may
simply suggest that any combination of values would work as long as the time
constant or other objective met some criterion, or maybe even a range for R and C.
If the time constant ended up being a constraint in the application, then our values
would end up being constrained to T=R*C which means that although we might be
allowed to vary R from 100 to 500 ohms, we would have only one value of C that
worked with each value of R. Thus now instead of having 20 results to consider
we would only have 5 different results to think about.
If you have some particular application in mind we can look at that in more detail and
perhaps come up with some more exacting data.
The max power of the 180 ohm resistor depends on the max voltage and the
max time it has to run at that voltage and the duty cycle, however if the
resistor is to be run at some voltage V for several minutes then it's a good idea
to rate the resistor according to the max voltage that will ever be encountered.
That would of course be P=V^2/R and that's the easiest way to do that.
If it does indeed vary quite a bit then you would have to resort to calculating
the average power using the integral to calculate power over time. Of course
if you dont want to do that you can also try experimenting a little as long as you
allow ambient to go up to the max that will be encountered in the final application.
Before i forget, there is one more little point about driving a RELAY with a resistor
and cap. That is that if the cap delays the turn on or turn off of the relay then it
is entirely possible that it causes the relay contacts to open or close too slowly.
This happens because the voltage to the coil does not suddenly increase or
decrease but builds up slowly over time and the armature does not move as fast
as if it was driven directly with a fast changing drive signal.
This can be a problem if the contacts arc over as it takes longer to extinguish the
arc if the cap charges or discharges too slowly. Sometimes you cant actually do
it that way, but have to resort to a little switching circuit with at least one
transistor to drive the coil while the cap and resistor end up on the base of the
transistor. The upside to doing it this way is not only faster contact switching but
also the ability to use a much smaller capacitor value and thus save cost that way.
The cost of a small transistor and small cap can often be cheaper than a larger
cap, and might save from buying a power resistor too. Something to think about.
Of course a slightly more complex circuit with a little hysteresis is even better.
A lot of times when you have two parameters that seem to be able to vary one
of them ends up being dependent on something else too. For example, one
resistor value may be the coil ohms instead of an actual resistor and so
you have to go with that. In times when they can both vary then you have
to ask yourself if something else enters the picture too which helps to fix
or limit the range of one of the two parameters.
Of course sometimes we want to study the effects of BOTH parameters varying
and for that we would simply resort to moving to a dimension one more than we
are currently working in. That is, we would look at several values of say R and C
letting R vary from say 100 to 500 ohms in steps of 100 ohms and for each R
we let C be maybe 500uf to 2000uf (500uf steps) and consider the results from all of these
combinations. For that example of R and C, we would end up with 5 values for R
and 4 values for C, where each value of C is used with each value of R. This would
result in a total of 4 times 5 or 20 different results which we could look at and
this might give us some more insight for picking the right two values, or it may
simply suggest that any combination of values would work as long as the time
constant or other objective met some criterion, or maybe even a range for R and C.
If the time constant ended up being a constraint in the application, then our values
would end up being constrained to T=R*C which means that although we might be
allowed to vary R from 100 to 500 ohms, we would have only one value of C that
worked with each value of R. Thus now instead of having 20 results to consider
we would only have 5 different results to think about.
If you have some particular application in mind we can look at that in more detail and
perhaps come up with some more exacting data.
The max power of the 180 ohm resistor depends on the max voltage and the
max time it has to run at that voltage and the duty cycle, however if the
resistor is to be run at some voltage V for several minutes then it's a good idea
to rate the resistor according to the max voltage that will ever be encountered.
That would of course be P=V^2/R and that's the easiest way to do that.
If it does indeed vary quite a bit then you would have to resort to calculating
the average power using the integral to calculate power over time. Of course
if you dont want to do that you can also try experimenting a little as long as you
allow ambient to go up to the max that will be encountered in the final application.
Before i forget, there is one more little point about driving a RELAY with a resistor
and cap. That is that if the cap delays the turn on or turn off of the relay then it
is entirely possible that it causes the relay contacts to open or close too slowly.
This happens because the voltage to the coil does not suddenly increase or
decrease but builds up slowly over time and the armature does not move as fast
as if it was driven directly with a fast changing drive signal.
This can be a problem if the contacts arc over as it takes longer to extinguish the
arc if the cap charges or discharges too slowly. Sometimes you cant actually do
it that way, but have to resort to a little switching circuit with at least one
transistor to drive the coil while the cap and resistor end up on the base of the
transistor. The upside to doing it this way is not only faster contact switching but
also the ability to use a much smaller capacitor value and thus save cost that way.
The cost of a small transistor and small cap can often be cheaper than a larger
cap, and might save from buying a power resistor too. Something to think about.
Of course a slightly more complex circuit with a little hysteresis is even better.
Last edited: