Voltage and current phase shifting/Current without voltage?

In summary: It is enough that we should have a preconceived opinion."In summary, the current in an RLC circuit is maintained by the energy stored in the inductor or capacitor. The phase difference is a result of the energy storing ability of the reactive elements and their V-I relationship.
  • #36
anorlunda said:
I promised to work an example to explore whether using a square wave rather than a sin wave might make AC circuits easier to explain to beginners. As an old time analog guy, I always learn best from study of time plots. :wink:
I think the sinewave model will not be superseded. For a start, it deals with just one frequency and requires only a very few axioms to get started. I know it can't be used for explaining 'what really happens' to people who want to feel they know the topic really well.
But I say that they have to go along with the standard AC theory with all its limits or they have to get over the Maths of the Full Monty approach. They can't have it both ways because a difficult subject is . . . . Just DIFFICULT.
Annoying when they have been telling you in school that anything is possible but there it is.

[/B]
 
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  • #37
@sophiecentaur , did you read #34 and #35?

I am trying to find a way to introduce AC without phase angles, and without even mentioning frequency. Step 2 would be to move from square waves to sinusoidal waves. So the goal is not to replace the sinusoidal model, but to introduce it in 2 steps.

Remember the confusion of the OP of this thread. He thought that when V is zero, I must be zero simultaneously. That is the kind of misconception that students of traditional teaching come away with. I'm not after better science, but better teaching.
 
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  • #38
Purple_Dan said:
Shouldn't the zeros of voltage and current always align? How can there be current without voltage?
There's somebody not yet thinking in terms of differentials. Or even the precursor to derivatives, deltas.

Purple_Dan said:
But how can the current possibly maintain the same waveform? Shouldn't the zeros of voltage and current always align?
There's somebody not realizing sine and cosine have the same shape just are offset by 90 degrees, and have the strange property that one of them is always proportional to the other one's slope.

He needs to see some graphs. Then do some graphical exercise homework problems that demonstrate above points. The straight lines of triangle and square waves lead the mind directly to thinking about slope and rate of change. It's a small step from there to sinewaves..

Then be reminded "AC Circuit Analysis , having grown out of power field(Steinmetz and Tesla) naturally is based on steady state sine waves.
One must remember that sinewaves are a mathematical special case.
While they're the coin of the realm in power, in other fields of electronics they're not so ubiquitous .
All EE students first learn steady state sinewave circuit analysis . It's a century old tradition. It allows solution by simple algebra.
Non steady state behavior and non sinewave functions require solution by differential equations . Other mathematical tools like Laplace Transform are useful for solving them. .
So buckle up and learn your basic steady state sinewave AC circuit analysis. "

That's how i was taught AC before i took Calculus.
 
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  • #39
@jim hardy, @anorlunda, I have a question regarding the capacitor waveforms in #34.
I understood the square-triangular graphs for capacitor and I understand I=CdV/dt for a capacitor.
Now, suppose you take a capacitor and connect it to a triangular-wave voltage source through a switch and keep the switch open. This switch is closed at the instant when the triangular voltage wave reaches its peak. So the voltage is applied across the capacitor when it is at the peak. Call this time as t=0. So from t=0, the capacitor will see a negative rate of change of voltage. What should the current waveform look like in this case?
 
  • #40
cnh1995 said:
@jim hardy, @anorlunda, I have a question regarding the capacitor waveforms in #34.
I understood the square-triangular graphs for capacitor and I understand I=CdV/dt for a capacitor.
Now, suppose you take a capacitor and connect it to a triangular-wave voltage source through a switch and keep the switch open. This switch is closed at the instant when the triangular voltage wave reaches its peak. So the voltage is applied across the capacitor when it is at the peak. Call this time as t=0. So from t=0, the capacitor will see a negative rate of change of voltage. What should the current waveform look like in this case?

The voltage across a capacitor can't jump instantaneously, that would take infinite current. So if you connect an uncharged capacitor to an ideal voltage source, you created a contradiction. The voltage at t=0+ must be V but it also must be zero. Something has to give. In practice, it would likely be that the voltage source is not ideal. It has an internal resistance that limits the current. So the circuit and the initial transient would resemble those in #31 of this thread.

We get similar questions all the time. "What happens to I=V/R when R=0?" The answer is that Ohm's Law and circuit analysis apply only over reasonable ranges of V and I. Infinity is never reasonable.
 
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  • #41
anorlunda said:
So if you connect an uncharged capacitor to an ideal voltage source, you created a contradiction.
Exactly!
This is why the result of the simulation I just ran is showing a very large spike of current, which is an indication of something invalid.

I knew that 'an ideal inductor fed from an ideal current source' is an invalid situation. But it never occurs in ac circuits.

But if a capacitor is energized when the input voltage is at its peak (or any non-zero value), it should create an invalid situation (in ideal case of course).
(It's strange that it didn't occur to me even after knowing about inductorso0)).

Thanks a lot!
 
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  • #42
Indeed you'd get a current spike . How big ?
This is where 'ideal' components in thought experiments can get you in trouble
Let's take your capacitor thought experiment
As anorlunda said much earlier, at any instant AC is DC because current flows only one direction at a time
i = c X dv/dt or if you prefer i = c X Δv / Δt
at the instant of switch closure,
Δv is a real number, the triangle wave peak
and Δt is zero.
Sophiecentaur tells us to 'use the maths'
and division by zero does not give infinity, it is undefined. Its limit approaches infinity as denominator approaches zero,
but division by zero is not allowed
and any rigorous math model should blow up (or if a computer program, complain..)

Were there any resistance in the circuit to drop the source voltage you could solve for real and finite current
but the ideal capacitor has none.
Any real capacitor has some resistance in its wires ,
so in your thought experiment as that resistance approaches zero, ,,,,, think about it - resistance will be in the denominator too
as resistance approaches zero current can only approach the mathematical limit which is infinity . But you'll never get all the way there .

The math works out ! (again)

The end result of all this is just what anorlunda said - you can't have finite Δv in zero Δt , you have to take the average over some finite Δt. This is where graphic solutions excel in teaching basics . I talk myself through any approach to math problems before setting pencil to paper to test my logic. Given my Latex Illiteracy Syndrome i especially have to talk through them here.
https://en.wikipedia.org/wiki/Division_by_zero
Historical accidents
  • On September 21, 1997, a division by zero error in the "Remote Data Base Manager" aboard USS Yorktown (CG-48) brought down all the machines on the network, causing the ship's propulsion system to fail.[12][13]
 
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  • #43
These are some simulation results for inductive ac circuits.

1)Purely inductive circuit:
Switching instant:
Voltage(green) zero crossing.

Remarks: Maximum dc offset in current (blue), no damping because of absence of resistance.
Hence, no negative half in the current waveform.
Screenshot_20170705-192637.png


2)Purely inductive circuit:
Switching instant: Voltage peak (almost).

Remarks: Zero dc offset in current, symmetrical current waveform.
Screenshot_20170705-192930.png


3)Purely inductive circuit:
Switching instant: Between voltage zero and peak.
Remarks:Non-zero dc offset (intermediate), no damping.
Screenshot_20170705-193057.png


You can see how VL=Ldi/dt is satisfied in every waveform.
 
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  • #44
Post #43 Continued...

4)R-L circuit:
Switching instant:
Voltage(green) zero crossing.
Remarks: Initial dc offset current dies out exponentially (transient) and the phase difference between voltage and current(red) becomes equal to the power factor angle at the end of this transient.

Screenshot_20170705-202812.png


Here's what the entire transient looks like:
Screenshot_20170705-202929.png


If the switching angle is equal to the power factor angle, there is zero dc offset i.e. no transient.
 
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  • #45
Thank you @cnh1995

those DC offsets in inductors are real and the math will show them.

They cause saturation in power transformers which gives huge inrush current for first few half cycles should one happen to switch it on near the zero crossing.
That's why they make peak switching solid state relays for inductive loads and zero switching ones for capacitive loads.

Nice demonstration , practical application of theory - thanks again !

old jim
 
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  • #46
anorlunda said:
@sophiecentaur , did you read #34 and #35?

I am trying to find a way to introduce AC without phase angles, and without even mentioning frequency. Step 2 would be to move from square waves to sinusoidal waves. So the goal is not to replace the sinusoidal model, but to introduce it in 2 steps.

Remember the confusion of the OP of this thread. He thought that when V is zero, I must be zero simultaneously. That is the kind of misconception that students of traditional teaching come away with. I'm not after better science, but better teaching.
My point is that sometimes there are limits to how easy you can present a subject without losing the meaning or further confusion. What I call AC theory is a way to present a limited set of EE which is more or less self consistent. It is no surprise that it emerged as a field in itself because it does so well as a tool which copes with such a lot of EE problems. If someone wants to 'argue' with the validity of just dealing with 50/60Hz signals then they don't have a leg to stand on. It's proved it's utility.
it is very risky to try half way house approaches without a very thorough treatment.
A really useful radical to teaching method would have to be in the form of a proper textbook, I think. Else it would generate as many new questions as answers. A private exercise is, of course fine but you'd need a very complete picture to justify not doing the whole thing.
Frequency and phase are essentials so what are you proposing to get across whilst avoiding them? And why?
Bending the subject to fit the student is very risky. The way to deal with difficult bits is to study harder or to admit it's too hard and do something else. Mainstream always gets criticized when individuals have problems. What about the vast majority who actually get along with it?
 
  • #47
sophiecentaur said:
Frequency and phase are essentials so what are you proposing to get across whilst avoiding them? And why?

I'm not proposing to avoid them
just to postpone leaping into them until we've got students familiarized with slope and graphical methods applied to simple square and triangle waves , so as to lead their minds into the differential relation that's so necessary to understand reactance.

I guess I'm biased because it's how i was taught long before i'd taken any math class that even mentioned Euler and his identity..
 
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  • #48
jim hardy said:
I'm not proposing to avoid them
just to postpone leaping into them until we've got students familiarized with slope and graphical methods applied to simple square and triangle waves , so as to lead their minds into the differential relation that's so necessary to understand reactance.

I guess I'm biased because it's how i was taught long before i'd taken any math class that even mentioned Euler and his identity..
This confuses me a bit. Why were you being taught about "waveforms" etc. before circuit theory? What was the context? Perhaps in the services as a trainee operator? That, I could understand and it could be the reason for my 'dissonance' because my education always involved Deferred Gratification - until we had the Maths to deal with things.
 
  • #49
sophiecentaur said:
What was the context? Perhaps in the services as a trainee operator?

Probably close. High school electronics class, taught by a retired Merchant Marine radioman turned engineer turned teacher.

After DC circuits analysis we of course moved into AC. Learned first about exponential charging , decay, time constants , effect of differentiator and low pass on step and triangle functions. Became skilled with slide rule and 1/e to work them.
Then he introduced us to rotating phasors to represent sines, real and imaginary components and operator j , and rectangular-polar conversion by slide rule.
He drilled us nearly to death doing sinewave AC circuit analysis with slide rules. He didn't take us into three phase power, instead into tubes and radio, transmission lines and antennas, finally transistors.
Setting was lab environment . We were two boys to a bench each bench with an oscilloscope, meters, power supplies, a "trainer" rack with tube sockets and patch panels to build circuits. By end of 11th grade we boys knew every resistor in an AM or FM radio reciever & transmitter and were handy with Smith charts.
Teacher was a very hands-on type guy , Monday was lecture day, Tuesday and Wednesday a lab covering the previous days' lectures, Thursday we wrote and presented our reports..
Friday was project day, everybody had to build something for his personal use from surplus electronic parts. He had access to leftovers from Cape Canaveral so there was no shortage of those . I built several tube hi-fi amplifiers and a Wheatstone bridge for measuring precision resistors (this was early 60's when digital meters were exotic rarities).

So we learned basic electronics and test equipment;
how to do an experiment and write up an organized report with purpose, method, presentation of data, observations and conclusions, ;
and how to build something starting with a blank aluminum chassis and Greenlee tube socket punch. .

Was it a disservice to launch us boys without the advanced math ?
I think not, for when in college i saw how calculus described what i had been doing with just arithmetic and operator j it was quite a thrill. Made me appreciate the genius of my high school teacher . I found myself explaining things to other students.
I'd not have made it through college antennas class had not we high school boys built that parallel wire transmission line (from #10 copper house wire on a 2X4) and done "slotted line" SWR & reflection coefficient measurements .

Besides, what're you going to do with a bunch of tenth graders who are just learning 2nd year algebra and trigonometry ?
Teach them to work with the tools they have.

As a teacher you know how a good one can affect a kid's life. He got me into EE and over the years i met several other of his students who were similarly influenced.
He made things intuitive for us boys.
Sorry for the ramble - it's not about me it's about " how does one teach ?"
For me something real makes the math intuitive, not the other way round. That's why i say so often here: "When your intuition leads you to the correct math you're beginning to understand".
Math closes the feedback loop and tells me i have achieved a valid mental model for something.

Perhaps my upbringing was weird but it's the only one I've got. I reckon it's why I'm a bit weird.

old jim
 
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  • #50
jim hardy said:
After DC circuits analysis we of course moved into AC. Learned first about exponential charging , decay, time constants , effect of differentiator and low pass on step and triangle functions. Became skilled with slide rule and i/e to work them.
Then he introduced us to rotating phasors to represent sines, real and imaginary components and operator j , and rectangular-polar conversion by slide rule.
He drilled us nearly to death doing sinewave AC circuit analysis with slide rules. He didn't take us into three phase power, instead into tubes and radio, transmission lines and antennas, finally transistors.
Setting was lab environment . We were two boys to a bench each bench with an oscilloscope, meters, power supplies, a "trainer" rack with tube sockets and patch panels to build circuits. By end of 11th grade we boys knew every resistor in an AM or FM radio reciever & transmitter and were handy with Smith charts.
Teacher was a very hands-on type guy , Monday was lecture day, Tuesday and Wednesday a lab covering the previous days' lectures, Thursday we wrote and presented our reports..
Friday was project day, everybody had to build something for his personal use from surplus electronic parts. He had access to leftovers from Cape Canaveral so there was no shortage of those . I built several tube hi-fi amplifiers and a Wheatstone bridge for measuring precision resistors (this was early 60's when digital meters were exotic rarities).

So we learned basic electronics and test equipment;
how to do an experiment and write up an organized report with purpose, method, presentation of data, observations and conclusions, ;
and how to build something starting with a blank aluminum chassis and Greenlee tube socket punch. .
I envy you!:wideeyed:..
 
  • #51
cnh1995 said:
I envy you!:wideeyed:..
Yes. A nice way in for Jim. I wonder how many of his cohort did as well as him. I'll make him blush by saying he is a bit special where E Engineers are concerned.
 
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  • #52
:blushing:Gosh, Sophie - THANK YOU SIR !:blushing:

I do admire (and envy) those like you for whom math seems so natuaral and are at home with it.
I always struggled with it.


old jim
 
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  • #53
jim hardy said:
I do admire (and envy) those like you for whom math seems so natuaral and are at home with it.
I always struggled with it.
You overrate my ability. :wink: With me, it's not like that. I am pretty rubbish at Maths because I was never bothered enough to learn enough of 'the rules' that you need when actually trying to work things out. It's more a matter of 'faith' that I could if I was bothered to - or at least that "it can be shown that" by someone smarter than me. I did work with a lot of people who could cope with higher levels of Maths than I could and I really believe it's a valid way through. That's just like using an electronic device with an in and an out and some control knobs. Your employer paid £10k for it so we all believe it and it checks out against other stuff that also cost a lot. Then you look at the system as a whole and wave yer arms about a bit for a result.
 
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  • #54
sophiecentaur said:
I did work with a lot of people who could cope with higher levels of Maths than I could and I really believe it's a valid way through. That's just like using an electronic device with an in and an out and some control knobs.

Amen.
Laplace transform is beyond my comprehension.
It's quite a handy tool, though.
I suppose one doesn't have to understand equations for impulse and momentum to apply a hammer to a nail .

:smile:
 
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