D
daestrom
---daestrom said:[email protected] wrote:
The way a kWh meter works is the reverse of this. It develops a
torque proportional to VA*pf. Vary the power factor and the
torque developed in the disk varies. A drag magnet develops
counter-torque proportional to disk speed. The result is disk
*speed* is proportional to VA*pf.
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I have to disagree here, the instantaneous torque is proportional
to instantaneous va or power. Inertia averages this to get the
average power over each cycle (or longer). VA*pf implies that it
measures the product rms voltage and current and applies a bugger
(oops power) factor. The meter "sees" none of these because they
are not physically there. the equivalence is there in that the time
varying instantaneous values can be represented by their rms
frequency domain equivalents in steady state. Analysis of the meter
uses the rms approach as you have done (it avoids a nasty mess of
non-linear differential equations) but the meter doesn't.
But wouldn't you say that the torque developed is a function of the
phase angle between current and voltage? If the current lags 90
degrees from the applied voltage, then the magnetic fields of the
current coil and voltage coil are almost exactly in-phase (owing to
the high inductance in the potential coil). With the two magnetic
fields pulsing 'in-phase', there is no torque either forward or
reverse developed.
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I have no problem with this. The meter doesn't measure phase angle.
Note that the induction disc motor is essentially a form of single
phase motor. The disc wont start but if already rotating there will
be a torque bias in that direction. A single phase motor depends on
this bias which is greatest near synchronous speed. However, in the
case of the induction disc there will be very little unbalance torque
-if any as the torque speed curve is essentially (and desirably)
constant torque in the operating region (just about standstill)
There will be a pulsating torque.
The simple fact that power flow in the opposite direction develops
torque in the opposite direction shows that phase-angle between
current and applied voltage is 'built-in' to the device.
Yes it is, in the same way it is built into a conventional
electromechanical (dynamometer) wattmeter. The torque at any instant
depends on the product of instantaneous voltage and instantaneous
current. On this basis, it simply averages the instantaneous torque.
If the voltage and current are 90 out of phase, the instantaneous
voltages and currents result in a double frequency power with 0 average
Mathematically we can say -for sinusoids:
p(t)=Vmcos(wt)*Imsin(wt+phi) =(VmIm/2){cos(phi) +a second harmonic
power term with 0 average]
The average over a period is (VmIm/2)*cos phi +0 =Vrms*Irms* cos(phi)
Physically the meter simply produces a torque which is proportional
to the instantaneous power and inertially averages it.
Specifically, it doesn't measure phase angles, rms voltages or find
pf -that is my point.
If the voltage and current coils have high R/X values then the meter
will be able to handle distorted waves with reasonable accuracy (and
without doing a fourier analysis). A digital KWH meter will simply
do the same v(t)*I (t) and averaging as a mechanical meter but with
a few bells and whistles can be made to measure KVAH (pf*H is
possible but meaningless) as well but such measurements aren't
required or necessary for determination of energy.
Yes, of course you're right that the inertia *averages* out the
torque, but it's not 'instantaneous va', it's 'instantaneous
power'. But 'average power' *is* rms-volt * rms-current *
power-factor in a sine-wave only system (i.e. no harmonic content)
instantaneous power = v(t)i(t) This happens to be the same as
instantaneous va but I should not have used that term. The concepts
of VA and VAR's are related to phasor analysis which is a
mathematical model which gives us the pertinent information without
the labor of solving a mess of differential equations. At your 120V
outlet- there is no actual 120V source as can be seen if you
examine the voltage with an oscilloscope.
Certainly, use of rms volts(magnitude)*rms current magnitude *power
factor will give the same average power. That's part of the reason we
use this model- it works.
Also, this "model" allows us a reasonable chance of solving
not-so-simple circuits. Think of what the situation would be in
solving load flows for large systems using differential equations!
Phasor analysis essentially replaces these differential equations by
algebraic equations.
Another convenient model is the use of symmetrical components for
fault studies.
Another is the use of forward/backward fields to model a single
phase machine as two opposing machines.
In these cases there are direct relationships between the model
quantities and the actual quantities present.
You know all this. The point of this long winded diatribe is that,
too often, people think that the model is the actual thing.
(you're too kind
I understand that the 'true' measure of power is instantaneous V *
instantaneous I and that that can simplify to simpler terms in certain
specific situations (such as DC or sine waveforms).
I guess I just can't 'wrap my head around' the meter responding to
instantaneous V*I when the magnetic field from the potential coil is
delayed nearly 90 degrees from V.
The voltage coil and current coils are not co-axial. If the voltage
coil is displaced from the current coil, then when the current is
maximum, the flux of this coil is maximum but that of the voltage coil
is 0. When the voltage coil produces maximum flux , the current coil
flux is 0. So , as seen from outside, there is a shift of flux .
Ideally, if the voltage coil is 90 degrees apart in space from the
current coil, you would get a "2 phase" motor with only a rotating field
. Since the displacement is not 90 degrees, you get a weaker rotating
field as well as a pulsating field. Another example is a shaded pole
motor as used in small fans.
Yes, yes, I'm familiar with two phase motors and the 'shift' of the
flux. But since the disk is not ferromagnetic, that alone doesn't
create a torque (i.e. it's not a reluctance motor). So we have to have
an eddy current induced in the disk (a 'rotor current') and to my mind
it's the interaction of that eddy current with the magnetic field that
produces a torque. Much like the current in the squirrel cage of a
conventional single-phase motor.
A disk that was composed of numerous 'pie slices' insulated from one
another would not work. Right?
I think you have part of it but a conventional single phase motor
without a starting winding will, at start, have 0 average torque but a
healthy pulsating torque. If you have a second winding which is
ideally 90 degrees electrically (physically 90 degrees for a two pole
machine) AND the flux due to the second winding is delayed 90 degrees in
time, then you have a situation where you have a true rotating field
with no pulsating torque- as in a 2 phase motor, 3 phase motor or a
single phase motor with a dominant capacitor on the second winding.
A single phase meter lies somewhere in between -think of the voltage
coil as a starting winding which is always in the circuit. It may not
be in physical quadrature (e.g the shaded pole doesn't shift flux by 90
degrees) The torque will have pulsations as well as a steady component
but the pulsations have a 0 average.
Should the disk R/X be low? Since the "start winding" is always in
service the physical position of this winding with respect to the other
winding provides the needed bias. It seems, on a first consideration,
that a R/X ratio near 1 in the disk may be desirable in that the torque
will be nearly constant and maximized near standstill- just as in the
case of a class D induction motor. --
R/X near 1 would certainly work, but an R/X near infinity might not
(i.e. there has to be some inductance). With the eddy currents exactly
in phase with one winding's flux, the currents would decay before the
other winding's flux increased very much. I see your point about R/X
near unity, after all as you said class D motors have some of the best
starting torques and that is how they achieve this.
The disk doesn't see the voltage and current directly but does respond
to the total of currents in the v and I windings interacting with the
currents in the disk. You can then consider a model with two stator
coils and two rotor coils and wade through a bloody "gawdoffal" mess of
math (task given to grad students) to come up with an expression for
torque dependent upon both the position of the coils and the currents in
them to find an instantaneous torque expression. Then you can consider
steady state (sinusoid) at some given speed ( in any motor the torque
has nothing to do with Ldi/dt but is affected by I*dL/dx* dx/dt or the
speed voltage) and come up with a model using rms voltages and currents
and the phase between them. The fact that this model typically agrees
with simpler approaches used in typical steady state handwaving analysis
of induction machines is comforting.
Krause "Analysis of Electric Machinery" deals with some of this (at near
graduate level) and an old book by White and Wilson "electromagnetic
energy conversion" is another- this is definitely a graduate level
text. Many other texts simply jump into the steady state models- a bit
more practical but losing some concepts.
Well without getting into 'gawdoffal' calculations, it just seems that
if the eddy currents in the disk lag behind the flux that produces them
(i.e. the disk has some inductance) then the torque pulses would seem to
lag behind the instantaneous power 'pulses' that occur at twice line
frequency.
So I wonder how close the disk is operating near 'synchronous speed'.
Where I think the synchronous speed in this case is function of
mechanical shift between current and voltage coils (i.e. the equivalent
'number of poles' arranged around the rotor). But also the phase shift
between current in the two coils (which of course depends on connected
load and R/X of potential coil). That is, the time shift between the
flux of one pole and the other.
If the maximum power to be registered is anywhere near a fraction of
this 'sync speed', then you effectively have a significant variation in
slip of the rotor. Of course some motors have a pretty flat torque
curve at the lower end of speed when starting and for a given applied
voltage/current, that's what we want here. So that torque produced is
*not* a function of %slip but only the measured power. Or variations in
%slip are tiny because the 'sync speed' is so much higher than expected
speed of the rotor.
(ouch, my head's starting to hurt ;-) )
--
The voltage coil may not have a low R/X ratio. However, you don't want
it producing flux in phase with the current -
High harmonic content is still a problem because you do want the torque
independent of winding impedance- variations which comes back to the
desirability of an R/X that is on the high side.
All of the references I've found on the matter seem to say that the
potential coil does have a low R/X so that magnetic flux is nearly 90
lagging from applied voltage. If it's something 'in between', wouldn't
that give you some calibration issues? For example, if R/X is 1 in the
voltage coil, then a connected load with a current lagging by 45 degrees
would be exactly in-phase with the voltage coil's current. No torque
produced but the customer is getting power (at 0.707 pf)
daestrom