Proof of common sense when maths is lacking concept

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The discussion centers on the relationship between power consumption, resistance, and current in electrical appliances, specifically comparing electric fans and kettles. It clarifies that while a fan has lower wattage than a kettle, it can have a higher resistance, which leads to less current draw and thus lower power consumption. The conversation highlights the importance of understanding the distinction between resistance and impedance, especially in AC circuits, where inductive effects can complicate power calculations. Participants emphasize that power dissipation is primarily related to the resistive component of impedance, and that the phase relationship between current and voltage in AC circuits is crucial for accurate power assessment. Overall, the thread illustrates the complexities of electrical principles that can lead to misconceptions about power usage in different devices.
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Ok, (an embarassing question) well I know an electric fan is relatively low wattage compared to say an electric kettle (while both on for the same amount of time). But also that smaller resistance draws more current than larger resistance, and by this logic (v2/R or I*R) the smaller resistance uses more power.
To reitterate the electric fan uses less power than the kettle (or water heater, air con etc.) so what is this model failing to take into consideration? Power factor or something?

Thanks!
 
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toneboy1,

Ok, (an embarassing question) well I know an electric fan is relatively low wattage compared to say an electric kettle (while both on for the same amount of time).

Irrelevant point, the length of time an appliance is on has nothing to do the rate electrical energy is consummed. In other words, a 45 W bulb will consume energy at half the rate of a 90 W bulb no matter how long it is on.

But also that smaller resistance draws more current than larger resistance, and by this logic (v2/R or I*R) the smaller resistance uses more power.

The correct term for power at a constant voltage is (I^2)*R, not I*R. Yes, according to (V^2)/R, a smaller restance will consume more power.

To reitterate the electric fan uses less power than the kettle (or water heater, air con etc.) so what is this model failing to take into consideration? Power factor or something?

You failed to specify what the problem is.

Ratch
 
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Not quite sure what you mean, so I'm just taking a shot here - you'll have to forgive me if I've misunderstood the question.

Less resistance gives you more current for the same voltage. The instantaneous power delivered to the circuit is current x voltage. The resistance of the electric fan at its terminals will be higher than that of the heater (if it draws less current for the same voltage you apply to the heater).
 
First of all, thanks for the reply;
Ratch said:
toneboy1,



Irrelevant point, the length of time an appliance is not has nothing to do the rate electrical energy is consummed. In other words, a 45 W bulb will consume energy at half the rate of a 90 W bulb no matter how long it is on.

I understand that, what I was trying to make clear that one appliance uses more than the other, I imagined someone saying 'but you leave a fan on and a kettle turns off after boiled'.

Ratch said:
The correct term for power at a constant voltage is (I^2)*R, not I*R. Yes, according to (V^2)/R, a smaller restance will consume more power.
Indeed.

Ratch said:
You failed to specify what the problem is.

Ok, well to the fan uses less power yet, has less 'resistance' (being for the most part an inductive motor) I assume than say an electric water heater, so how is this seeming contradiction wrong?
 
There's your problem - less power does not mean less ohmic resistance.
 
milesyoung said:
There's your problem - less power does not mean less ohmic resistance. .

On the contrary, it means more ohmic resistance, but what I'm saying is that say a fan would have LESS resistance than a heater but still use LESS power, or am I wrong, is a fan actually manifold more resistive?
 
Why would it have less resistance?
 
milesyoung said:
Why would it have less resistance?

I just thought it would because its just coils of copper and copper isn't that resistive. (not sure how many meters but it would seem like if I had a huge motor with more resistance than it would be less power to run than a small one, which is counter intuitive)

I would have thought, for an idea of proportionality a fan would be like 100 ohm fan and a heater 3k ohm (again, just for a relation, no idea what they would actually be)
Thanks
 
toneboy1,

A small fan has more resistance than a heavy duty heaater, plain and simple.

Ratch
 
  • #10
Ratch said:
toneboy1,

A small fan has more resistance than a heavy duty heaater, plain and simple.

Ratch

oh, ok, fairenough. What about a large motor to a small one?
 
  • #11
For a large motor you'll typically also use more material for the windings, so you can't really assume some kind of proportionality between size and winding resistance.

Regardless of what circuits you're working with, if one draws more current on average than another for the same voltage, it will have less equivalent resistance.
 
  • #12
milesyoung said:
For a large motor you'll typically also use more material for the windings, so you can't really assume some kind of proportionality between size and winding resistance.

Regardless of what circuits you're working with, if one draws more current on average than another for the same voltage, it will have less equivalent resistance.

I see what your saying, if you endulge me, so if I had two motors, both with the same gauge wire, one with more windings and larger, one with less and smaller, the smaller one would have more current and thus use more power?

Thanks again
 
  • #13
I think some of the confusion here is the distinction between resistance and impedance. Resistance is a coverall term for DC circuits but is meaningless for AC circuits, which use the term impedance which takes into account non-DC effects.

That is, a coil of wire can have REALLY low "resistance" as measured by a DC ohmmeter, but when you run an AC current through it, the inductance causes a high impedance.
 
  • #14
phinds said:
I think some of the confusion here is the distinction between resistance and impedance. Resistance is a coverall term for DC circuits but is meaningless for AC circuits, which use the term impedance which takes into account non-DC effects.

That is, a coil of wire can have REALLY low "resistance" as measured by a DC ohmmeter, but when you run an AC current through it, the inductance causes a high impedance.

Quite right, but power only uses the ohmic resistance 'real' part of impedance doesn't it? So for my last question the larger motor would still have more real impedance. (just trying to illustrate how I can clarify my counter-intuitive confustion)
Cheers
 
  • #15
If we're just talking about motors in the sense that we model them as a series connection of a resistor and an inductor, then yes - the small motor will draw more current for the same voltage and thus use more power.

Edit: And of course as phinds pointed out, I assume we're strictly talking DC here.

Edit: You're not actually going to use this argument for anything important, right? There's a lot more to motors..
 
  • #16
milesyoung said:
If we're just talking about motors in the sense that we model them as a series connection of a resistor and an inductor, then yes - the small motor will draw more current for the same voltage and thus use more power.

Edit: And of course as phinds pointed out, I assume we're strictly talking DC here.

that seems like it's violating concervation of energy (I know it mustn't be) but you know what I mean, the more you get (like more torque or whatever) the less power, for that matter it seems like I could just put a resistor on the end of the terminal and make it use even less power (though that would probably slow the fan down). Sorry this question must be so irritating but I hope you can see why I'm confused
 
  • #17
You are oversimplifying motors. Less windings also mean less torque - typically (there are a lot more factors to consider here but for the sake of argument).
 
  • #18
milesyoung said:
You are oversimplifying motors. Less windings also mean less torque - typically (there are a lot more factors to consider here but for the sake of argument).

I know, that's what I said, so you make a huge motor, with heaps of windings (and torque) and yet is uses less power than a small one...
 
  • #19
Hehe, yes - less power but also less current, which means less field strength and less torque. It's really not that simple.
 
  • #20
milesyoung said:
Hehe, yes - less power but also less current, which means less field strength and less torque. It's really not that simple.

M'mm, I'll accept that. I'm going to get my multimeter tomorrow and check what my fan and 500W distiller are, I really can't believe a fan would be so resistive.

Thanks for your help.
 
  • #21
toneboy1,

I see what your saying,

I am not so sure about that.

...if you endulge me, so if I had two motors, both with the same gauge wire, one with more windings and larger, one with less and smaller, the smaller one would have more current and thus use more power?

Are the current and voltage in phase? If you applied AC line voltage to a single coil of high inductance, you could have a tremendous amount of current, and yet dissipate a very small amount of power. That is because the voltage and current are out of phase with each other. It will take a large amount of current to build up energy in the magnetic field of the coil during a quarter cycle, but that energy will be given back to the circuit in the next quarter cycle, and repeat the process in the reverse direction. Therefore, it will be large current and small power dissipation.

You are trying to confuse AC power distribution with DC power. It doesn't work that way. You need to know the phase ramifications of AC before you can calculate AC power.

Only the resistance part of the impedance dissipates power. The more the voltage and current are in phase, the more the resistance dominates the impedance.

Ratch
 
  • #22
Ratch said:
toneboy1,

Are the current and voltage in phase? If you applied AC line voltage to a single coil of high inductance, you could have a tremendous amount of current, and yet dissipate a very small amount of power. That is because the voltage and current are out of phase with each other. It will take a large amount of current to build up energy in the magnetic field of the coil during a quarter cycle, but that energy will be given back to the circuit in the next quarter cycle, and repeat the process in the reverse direction. Therefore, it will be large current and small power dissipation.

You are trying to confuse AC power distribution with DC power. It doesn't work that way. You need to know the phase ramifications of AC before you can calculate AC power.

Only the resistance part of the impedance dissipates power. The more the voltage and current are in phase, the more the resistance dominates the impedance.

Ratch

YES that's more the answer I've been looking for! THANK YOU, I knew a bloody fan wasn't that resistive.
Out of curiosity, what about a DC motor, given that there is no phase change (or voltage lag) would one use more power than its ac counterpart?
 
  • #23
milesyoung said:
Edit: And of course as phinds pointed out, I assume we're strictly talking DC here.

Edit: You're not actually going to use this argument for anything important, right? There's a lot more to motors..

I wasn't just talking DC, yeah I know there is a lot more to motors but every analogy I use seems to make the question harder to explain, I knew there was just a simple answer, I just ended up using motors to make the point.

EDIT: DC probably would have simplified things though :P
 
  • #24
I was just about to write that you were probably going to come back tomorrow angry that you've measured the resistance using an ohmmeter and you were right about the resistance etc :)

Just to make my point clear - I've only been talking about DC current and ohmic resistance. If you measure the average current into your circuit for some voltage, that relationship will give you its effective DC resistance - it won't have much to do with the winding resistance you'll measure (which will be very low).
 
  • #25
TB1,

Out of curiosity, what about a DC motor, given that there is no phase change (or voltage lag) would one use more power than its ac counterpart?

A DC motor has a commutator that switches the current direction in the rotor. That causes magnetic fields to form and collapse, thereby storing and releasing energy. This in turn causes a phase change in the voltage and current. Its behavior is complicated. See the neat animation at this link http://en.wikipedia.org/wiki/DC_motor .

Ratch
 
  • #26
When a DC motor is rotating it acts like a generator, and creates a "back EMF", in other words a DC voltage that is opposite to the applied voltage. If you prevent the motor from turnng, the current through it is be given the Ohm's law. That is called the "stall current" for the motor and it can be much higher than the normal working current.

When the motor is turning, the back EMF (which is proportional to the RPM) reduces the current. So as the motor speed increases, the current decreases and the electrical power decreases.

The amount of mechanical work being done by the motor usually increases with the RPM, and the result is that the motor runs at the speed where the electrical power equals the mechanical power. Below that speed, the electrical power "wins" and speeds the motor up. Above that speed, the mechanical work "wins" and slows it down.

The same idea applies to AC motors, but it gets complicated trying to explain it in words rather than doing the math, and from your original question, I'm guessing you are not familiar with how to analyse AC electrical circuits yet.
 
  • #27
The fan and the heater are both connected to an AC outlet. So we have to consider the AC system.

The heater would be made up of some sort of simple ohmic resistance that can handle a lot of power.

The power dissipated by the heater would then be (V_rms^2)/R.

The fan is a coil/resistance circuit. Possibly the resistances are not very big. But the coils may have a large inductance. Because of the large inductance, the circuit will not draw very much current because it is running in AC mode. Thus, the resistances are not dissipating very much power.

Heater - Small resistance - High power.
Fan - Large indutance leads to less AC current - Low power.
 
  • #28
milesyoung,

If you measure the average current into your circuit for some voltage, that relationship will give you its effective DC resistance - it won't have much to do with the winding resistance you'll measure (which will be very low).

Perhaps you know more about this than I do, but let me give you my take on what happens.

The average current is zero, just like it is when you apply an AC voltage across a plain resistor. DC resistance is the same as AC resistance, specifically the resistance of the motor coils and brush resistance. I don't know what effective DC resistance is. When a motor is running with no load, its voltage and current are way out of phase, and it is taking relatively little power from its voltage source. When a motor has a load, its impedance lessens because its reactance lessens, and its impedance becomes more resistive. This causes the motor to draw more power from the voltage source due to the phase change. During this time the resistance has not changed. It is only the reactance that has changed, which in turn changes the phase and increases power consumption.

Ratch
 
  • #29
Ratch,

I can't argue with any of that. It seemed like at the start that there were some trouble with the basics, so I was trying to stick to the definition of resistance and avoid the details of AC/motors: A DC motor would appear as having a higher resistance at its terminals when running due to back-emf.
 
  • #30
How can you say who use more power if there is no specification of the heater and fan? You can have a really big fan and a tiny heater!
 
  • #31
... To reitterate the electric fan uses less power than the kettle (or water heater, air con etc.) ...

He/she did mention it in the OP..
 
  • #32
yungman,


See post #9 of this thread.

Ratch
 
  • #33
toneboy1 said:
that seems like it's violating concervation of energy (I know it mustn't be) but you know what I mean, the more you get (like more torque or whatever) the less power, for that matter it seems like I could just put a resistor on the end of the terminal and make it use even less power (though that would probably slow the fan down). Sorry this question must be so irritating but I hope you can see why I'm confused

I cannot understand why you are confused. But I have extensive electrical training/education/background.

Electric Kettle:
rated power: 1500 watts
line voltage: 120
derived current: p/v=i --> 1500/120=12.5 amps
derived resistance: v/i=r --> 120/12.5=9.6 ohms

Electric Fan:
rated power: 100 watts
line voltage: 120
derived current: p/v=i --> 100/120=.833 amps
derived resistance: v/i=r --> 120/.833=144 ohms

I guess I don't understand where common sense comes into play with this problem. There are only equations.

hmmm... (scratches head, runs aerodynamic analogy through skull...)

Ah ha! I think I understand what you are asking. Interesting.

If mythical car A has an aerodynamic drag resistance of 144 units, it would make sense that it would consume more power than mythical car B with an aerodynamic drag resistance of 9.6 units.

(I'm ignoring back EMF and inductive resistance here, as I'm obviously interpreting your question differently than others.)

hmmm.. Where do we go from here? The mythical cars will both have to have engines. I'll give them both the same engine, rated at 120 mythical units, which I will call volts.

And what does this tell us so far? It tells us how fast the cars will go! Volts/Ohms = Amps.

Amps are the mythical unit for velocity that the cars will travel at.
(This is somewhat of a bad analogy, as real Amps are a measure of a certain number of electrons passing a certain point per second. Kind of like the number of cars driving through an intersection per second. But it kind of implies motion, and I'll stick with it. Let's just pretend that each car is negatively charged with an excess of 6.241 × 1018 electrons(or 1 Coulomb), and each cars length is equal to 1 coulomb per 0.003 miles, and see what happens)

Car A: (aka, the fan)
volts: 120
ohms: 144
amps: .833
(e-gads. now I understand the PF-EE heavyweights aversion to analogy)
length: 13 feet
velocity: 9 mph
power: (Force, aka volts)*Velocity = 1076 oomphs(new mythical name of electro-aerodynamic power unit)

Car B: (aka, the kettle)
volts: 120
ohms: 9.6
amps: 12.5
(why is length based on charge?)
length: 198 feet
velocity: 135 mph
power: 16,200 oomphs

So what does this all mean? They've both got the same motive force. But the car with the least resistance is using the most power.

scratches head again. hmmm... It still doesn't make sense, but at least the maths worked out:

16,200 oomphs / 1076 oomphs = 15.06
1500 watts / 100 watts = 15

-----------------------------
ok to delete. I enjoy nothing more than Sunday morning mental aerobics. :smile:
 
  • #34
Some good points were made and I did understand everything said and why, except for maybe you cheeto, but it was a hilarious departure nevertheless.

AlephZero said:
When the motor is turning, the back EMF (which is proportional to the RPM) reduces the current. So as the motor speed increases, the current decreases and the electrical power decreases.

The amount of mechanical work being done by the motor usually increases with the RPM, and the result is that the motor runs at the speed where the electrical power equals the mechanical power. Below that speed, the electrical power "wins" and speeds the motor up. Above that speed, the mechanical work "wins" and slows it down.

The same idea applies to AC motors, but it gets complicated trying to explain it in words rather then doing the math, and from your original question, I'm guessing you are not familiar with how to analyse AC electrical circuits yet.

Actually I have some experience with AC circuits a few years ago but have learned a lot since than and you know what they say, learn something new pushes something old out of your brain. I need a refresher.
So to summerise, the more resistance of a load on a motor, the more it increases the current, which makes it use more power. So if it's an ac motor it will change the phase of the voltage or current, (which I don't know) so the peaks will be closer and I*V will be bigger, or if its DC then the back emf will decrease and it will use more power. COOL. Exactly the sort of explanation I was looking for.

thanks

EDIT: If any of you (possibly clever engineers) could, I have an algebraic nightmare (a few of them) in this thread: https://www.physicsforums.com/showthread.php?p=4165324&posted=1#post4165324

I'd REALLY appreciate some help!

EDIT: What the hell, I have a Fourier question too for what it's worth:
https://www.physicsforums.com/showthread.php?p=4165336#post4165336
 
  • #35
Hello Toneboy - it may be possible that if you just measure the Resistance of the motor it has less resistance then the heater - but STILL uses less power - why? Because a motor when running - is not a resistor. The structure of the motor generates a magnetic field, and as the motor rotates, it generates "back EMF" - and still a little more dynamic than just impedance - for example a DC motor generated Back EMF - but steady state DC in an inductor does not have back EMF.
Since now the motor is generating EMF ( simply put Voltage) that opposes the voltage being applied - this reduces the current.
 
  • #36
toneboy1,

So to summerise, the more resistance of a load on a motor, the more it increases the current, which makes it use more power.

You still don't have it quite right. Yes, you can stall the motor and draw a fuse popping, wire burning, switch melting amount of current, but if the current is not in phase with the voltage across the motor, the power will not appear. I tried to explain that with my inductor example previously.

So if it's an ac motor it will change the phase of the voltage or current,

All motors will change the phase of their voltage/current if they have inductance.

so the peaks will be closer

The peaks are determined by the line frequency. That usually does not change.

and I*V will be bigger,

The power will be greater because the voltage and current are in phase longer.

or if its DC then the back emf will decrease and it will use more power.

The "back EMF" is due to the collapsing magnetic field. Any motor type that uses inductance will have a back voltage. A motor will use more power if its voltage and current are in phase during more of the rotation cycle.

COOL. Exactly the sort of explanation I was looking for.

Are you sure about that?

If any of you (possibly clever engineers) could, I have an algebraic nightmare (a few of them) in this thread: https://www.physicsforums.com/showthr...=1#post4165324

I'd REALLY appreciate some help!

You should start a new thread in the math section for that problem.

Ratch
 
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  • #37
It would be a great idea if this problem could be sorted out for Resistive Loads first. When we've got that all straightened out then we could move on to inductive and rotating loads. These are much more complicated and certainly not to be leaped into without getting the basics first.
For resistive loads, all you need to thing of is
1) P = IV : the Power relationship
and 2) R = V/I : the way we define Resistance

Combine these two together and you get two more useful formulae:
3) P = V2/R
and
4) P = I2R

Those four formulae will give you the answer to all possible questions about resistance, power and the way it can be supplied.
3) shows you that the power delivered (and used) goes down as the resistance is increased.
4) shows how the power lost in a supply wire, for instance, will increase as the resistance of the wire increases (that's if you keep the current the same)
 
  • #38
toneboy1 said:
On the contrary, it means more ohmic resistance, but what I'm saying is that say a fan would have LESS resistance than a heater but still use LESS power, or am I wrong, is a fan actually manifold more resistive?
Correct, your fan's motor could have less resistance and yet still use less power. Indeed, as an experiment you could make your motor windings have almost no resistance by using pure gold wire, an almost perfect conductor, and the fan would still draw less current* and use less power than the heater.

This is because the current in a fast spinning fan is largely not determined by the windings' resistance. As others have pointed out, the electrical model for a fan is not simply a fixed resistance and nothing else. It's that "something else" that is the key to explaining why it is that motors use more power the harder they work. http://physicsforums.bernhardtmediall.netdna-cdn.com/images/icons/icon6.gif
 
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  • #39
Thanks Windadct. Rach: "The power will be greater because the voltage and current are in phase longer." good way to put it, but I didn't necessarily mean stall the motor, just slow it down.

"The "back EMF" is due to the collapsing magnetic field" Ah, right, ofcourse, thanks.

As for the thread in the math section, I did, but I from what I've seen the people here stand a better chance of allowing me to figure it out.Thanks sophiecentaur, I think I've got the purely resistive relationships down and as far as I'm aware the phase relationship of an ac motor too.
The only possible area of lacking I feel might be possible is the way the EMF reduces the current in a DC motor. That said I'm still satisfied.
 
  • #40
TB1,

If any of you (possibly clever engineers) could, I have an algebraic nightmare (a few of them) in this thread: https://www.physicsforums.com/showthr...=1#post4165324

I'd REALLY appreciate some help!


As for the thread in the math section, I did, but I from what I've seen the people here stand a better chance of allowing me to figure it out.

You really need to get a computer program that can do equations like that. Otherwise you can spend hours and hours spinning your wheels and probably making lots of mistakes. I think there are some trial programs and freebies on the web from outfits like Wolfram, but I am not sure. Anyway, the first thing to do is rationalize both sides of the equation and see if they match. Rationalize means no complex terms in the denominator. That is a lot of work, but if they do match, then you proved they are equal and are finished. You rationalize the left side by first calculating a common denominator, and then multiply the numerator and denominator by the conjugate of each complex term in the denominator. Collect similar terms whenever you can. That is a lot of scut work, but it shows if the equations match. As you can see from the attachment, the right side should be twice what the rationalization shows to equal what the left side is, so the problem equation is wrong. You might be tempted to look for shortcuts by finding equal terms in the numerator and denominator, but for an equation that complex, you will probably just get tangled up trying to take advantage that situation. I think, to just do it systematically. (Ugh)

Ratch
 

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  • #41
Ratch said:
TB1,



You really need to get a computer program that can do equations like that. Otherwise you can spend hours and hours spinning your wheels and probably making lots of mistakes. I think there are some trial programs and freebies on the web from outfits like Wolfram, but I am not sure. Anyway, the first thing to do is rationalize both sides of the equation and see if they match. That is a lot of work, but if they do match, then you proved they are equal and are finished. You rationalize the left side by first calculating a common denominator, and then multiply the numerator and denominator by the conjugate of each complex term in the denominator. Collect similar terms whenever you can. That is a lot of scut work, but it shows if the equations match. As you can see from the attachment, the right side should be twice what the rationalization shows to equal what the left side is, so the problem equation is wrong. You might be tempted to look for shortcuts by finding equal terms in the numerator and denominator, but for an equation that complex, you will probably just get tangled up trying to take advantage that situation. I think, to just do it systematically. (Ugh)

Ratch


Thanks, well I had no reason to think they wouldn't be the same, but you're saying they're not equal? That shouldn't be, are you sure?

For argument's sake if I just had the LHS and wanted to reduce it to the form of the RHS would I still have to do the conjugate times numerator and denominator? (surely not)

I was just looking for the simplest way to solve the LHS without expanding into 25 term polynomials and having to factorise cubics.

I've used wolfram on the net and I have MATLAB and I think maple (which I've never used) but I don't know what I'd use to show me how to solve anything like that.
 
  • #42
TB1,

Thanks, well I had no reason to think they wouldn't be the same, but you're saying they're not equal? That shouldn't be, are you sure?

Yes, I am. I used Maple, and it has never given me a wrong answer. I rationalized both the RHS and the LHS, and they don't come out equal. You can spend a lot of time trying to wrestle one expression into another, especially if they are not equal. There are a zillion alternative ways to represent an expression, but if you know the end result, it is best just to determine if they are equal and walk away.

For argument's sake if I just had the LHS and wanted to reduce it to the form of the RHS would I still have to do the conjugate times numerator and denominator? (surely not)

To do it the hard way, first rationalize it. Then multiply the numerator by a hairy factor to get what you want in the numerator. Multiply the denominator by the same factor to keep everything equal. Simplify the denominator. Then use the terms in the denominator, and factor if necessary to create your own expression. You have to use all the denominator terms, and cannot use extra terms. Of course, you can use the computer to subtract the terms you use, and factor if necessary. The choices are many.

I was just looking for the simplest way to solve the LHS without expanding into 25 term polynomials and having to factorise cubics.

You are not solving an equation. You are proving an equality.

I've used wolfram on the net and I have MATLAB and I think maple (which I've never used) but I don't know what I'd use to show me how to solve anything like that.

Sounds like you are well stocked with software.

Ratch
 
  • #43
Thanks for pointing out that they're not equal, I could have wasted even more time.
I'll have to give maple a go when I get a chance. To varify.
To clarify, these two steps were in someone's working out, and I didn't know how they got from LHS to RHS, it wasn't a question of proove they're equal or not (if there's been a misunderstanding). I still don't see how I'd factorise the denominator to get it like ()^2 + ()^2 from the denominator of your (1). To do this it doesn't matter if there are j's in the denominator.
 
  • #44
TB1,

Thanks for pointing out that they're not equal, I could have wasted even more time.
I'll have to give maple a go when I get a chance. To varify.
To clarify, these two steps were in someone's working out, and I didn't know how they got from LHS to RHS, it wasn't a question of proove they're equal or not (if there's been a misunderstanding). I still don't see how I'd factorise the denominator to get it like ()^2 + ()^2 from the denominator of your (1). To do this it doesn't matter if there are j's in the denominator.

You can see from the attachment that I used the rationalize function of Maple. I would have thought that Matlab and the Wolf could do what Maple did. Maple can factor expressions, but that is not necessary to rationalize an expression, even if you do it manually. You need to multiply by conjugates to get rid of complex terms in the denominator. Then use the procedure I outlined previously to make any expression that is possible from the terms in the denominator.

Ratch
 
  • #45
Ratch said:
TB1,
You can see from the attachment that I used the rationalize function of Maple. I would have thought that Matlab and the Wolf could do what Maple did. Maple can factor expressions, but that is not necessary to rationalize an expression, even if you do it manually. You need to multiply by conjugates to get rid of complex terms in the denominator. Then use the procedure I outlined previously to make any expression that is possible from the terms in the denominator.

Ratch

I'm sure there is a way with them but I'm not that proficient yet (matlab wolf).
I don't see why it's necessary to eliminate all the complex numbers on the denominator or how it could be factorised to that, given the highest exponent of the solution saught will be 4, not 8. I could factorise the two term part by completing the square, but as for the 3 term polynomial squared, I wouldn't know where to start...Thanks for your help anyway.
 
  • #46
toneboy1 said:
Thanks sophiecentaur, I think I've got the purely resistive relationships down and as far as I'm aware the phase relationship of an ac motor too.
The only possible area of lacking I feel might be possible is the way the EMF reduces the current in a DC motor. That said I'm still satisfied.

Sorry for trying to teach my Grandmother to suck eggs! :smile:

Reading this thread reminds me how similar electric motors and radio antennae behave (and even loudspeakers). The up-front resistance is usually just not relevant to their performance - a dipole is an 'open circuit' but it can look like a useful 70Ω at the right frequency. Electrical resistance turns up where you'd least expect it but Energy Conservation requires it.
The Back EMF is only a 'way of looking at it', I think. There must be an alternative way of looking at it involving self inductance of a rotating machine.
 
  • #47
TB1,

I think I've got the purely resistive relationships down and as far as I'm aware the phase relationship of an ac motor too.
The only possible area of lacking I feel might be possible is the way the EMF reduces the current in a DC motor.

Like I said before, the back voltage is caused by the collapsing magnetic field when the current changes direction. It shouldn't be hard to imagine a "bucking" voltage going against the source voltage to reduce its value and lowering the current. It is a physical happening, and needs no alternative way at looking at it. The constant shift of electrical energy from the circuit to the inductor and back again also causes a current/voltage phase shift associated with inductive reactance.

Ratch
 
  • #48
TB1,

Just to follow up on your previous question about that math expression. If you look at equation (6) of the attachment, you can find an alternative form of that expression. If fact, there are many different forms. Once you have the denominator rationalized, you can use partial fraction expansions. Then the number of different expressions is only limited by your imagination.

Ratch
 

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  • #49
I'm going to throw in my 2 cents here because I think there's a small misconception with regards to self-inductance and its significance.

Let's consider a single winding of an AC motor which we'll model as a resistor in series with an inductor. It's true that a changing current through the winding will produce an opposing voltage in proportion to the self-inductance of the winding, but this isn't what limits the current in the circuit as the angular velocity of the rotor increases.

Be it a DC or an AC motor, as the motor speeds up, the current is limited by the voltage produced by the increasing rate of change of magnetic flux through the winding, due to the increasing angular velocity of the rotor field. It's this component of induced voltage that's usually termed 'back-EMF' in motors.
 
  • #50
milesyoung,

It's true that a changing current through the winding will produce an opposing voltage in proportion to the self-inductance of the winding, but this isn't what limits the current in the circuit as the angular velocity of the rotor increases.

Be it a DC or an AC motor, as the motor speeds up, the current is limited by the voltage produced by the increasing rate of change of magnetic flux through the winding, ...

I don't understand. First you say that the opposing voltage does not limit the current. Then you say that the voltage does limit the current. What's an inquiring mind to think?

Ratch
 
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