Re: how is power usage of CF\'s calculated?
Hi there Brock,
I see you have your web site arranged so everything can be found
quickly in one place. That's very nice.
Your idea of the current not always being the same is
sort of correct because the two waves (voltage and current)
are sine waves, so they never stay at the same level, so the
instantaneous power delivered is never constant.
I hope this doesnt come off too 'authoritative', i just want
to give a reasonable answer to one of life's mysteries
The interesting thing is that the RMS voltage and current
measurements are considered to be constant. The catch is
that their values only have meaning when dealing with a
purely resistive load. This means that if we dont have
a resistive load, the meaning of the two cant be applied
to calculate power, unless of course we know two more things:
the angle between current and voltage, and they are both
sine waves.
This means that
if we know the RMS voltage and current through a measurement
with the meter we can calculate power simply by multiplying V * I
but only if the load is a pure resistance. That's the unfortunate
catch; if the load is anything other then a resistance we
still cant calculate the power knowing only the RMS current
and voltage.
The reason for this is that the RMS voltage value
(or peak, or average) is a property of the voltage alone,
and the RMS current value is a property of the current alone,
whereas
the average power (usually just called 'power') is a property
of both the voltage and the current taken simultaneously.
This is because power is not only dependent on the voltage
and current amplitudes, it's also dependent on the relationship
between the two. This in turn means in order to measure power
we would need a single instrument to make the simultaneous
measurements of voltage and current.
When we take the two instantaneous values simultaneously, we
multiply each point on the current waveform times each
corresponding point on the voltage waveform and generate
a third waveform. This third waveform represents the instantaneous
power. This really is simply current times voltage, but it's
done on a point by point basis, for every point in time.
Once we get this waveform, we then take it's average value.
The average value of this wave is the average power, commonly
called 'power'.
There is no way to reduce the calculation without knowing
each individual point in both waves for the most general case.
This might sound hard to do, and yes it's harder to do then
simply multiplying volts time amps, but it's not really as
hard as it sounds. If we pick 20 or so time points
equally spaced across a half cycle, we can multiply
the current points times the voltage points and add them
all up and divide the result by 20 and come up with a
decent accuracy for most purposes. It's also interesting
to do this on graph paper, drawing two sine waves
out of phase. If we draw the third resulting wave, it
looks more peaked then the other two waves because it's
not a sine wave.
If the two waves are sine waves, then we can apply the
simple formula:
P=I*E*cos(angle)
but we do have to know the angle.
To see how much error can occur without considering the angle,
lets see what would happen if we had an angle of 90 degrees...
If we had 120 volts rms and 1 amp rms, 60Hz lets say,
E*I equals 120. Is this 120 watts?
Since cos(90) equals zero,
E*I*0 equals 0.
Note that what looked at first like 120 watts turned out to
be in fact no power at all! This is close to what a real
inductor or capacitor would show.
Note also that the RMS voltage is still 120 volts, and the
RMS current is still 1 amp too, but the power in this case is 0.
To show how true this is, we could compare the temperature of
say a capacitor that draws 0.83 amps at 120vac to a 100 watt light
bulb. The 100 watt light bulb gets way too hot to touch while
the capactor doesnt even get warm yet they both draw the same
current
CONCLUSIONS
[1]
If we are dealing with pure dc or pure resistance, we can
multiply volts times amps to get the power.
[2]
If we are dealing with pure sine waves, we can use the
cosine of the angle between current and voltage to help
determine the true power, but we do have to have a way
of measuring the angle.
[3]
If we are dealing with an arbitrary waveform (triangle, etc)
we have to multiply the amplitudes of the
voltage wave by the amplitudes of the current wave for
each equally spaced point in time and
sum the results and divide by the number of points to
get an approximation of the true power.
One last thing to mention is that power meters have two inputs,
one for voltage and one for current, so that they can measure
both values at the same time and do the math.
Take care,
Al