Calculating Energy Dissipation in a Rectangular Coil with Time-Varying Current

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Homework Help Overview

The discussion revolves around calculating the total energy dissipated in a rectangular coil with a time-varying current. The coil has specific parameters including resistance, number of turns, and dimensions, while the current is defined by an exponential decay function. Participants are exploring the integration of power over time to find the energy dissipated.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integration of power, questioning the correct application of exponential functions and the differentiation of the current. There are attempts to clarify the relationship between voltage, power, and energy, as well as the correct handling of constants during integration.

Discussion Status

The discussion is active, with participants providing guidance on the integration process and the correct formulation of equations. There is recognition of potential computational errors and the importance of including all relevant parameters, such as the number of turns in the coil.

Contextual Notes

Participants note the importance of correctly applying mathematical operations, particularly when squaring terms and integrating. There are mentions of specific constants and parameters that need to be included in calculations, highlighting the complexity of the problem.

arl146
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Homework Statement


A rectangular coil with N = 2,000 turns that has a resistance of 7.90 Ohms is coplanar with a long wire which carries a current which depends on time according to I0 *exp(-t/tau), where I0 = 6.50 A and tau = 4.30 s. The rectangular loop has a width of W = 2.00 cm and length L = 7.60 cm. The near side of the loop is a distance D = 2.90 cm from the wire.

What is the total energy dissipated in the entire coil from t = 0 to t = 2.60 s?

Homework Equations


I=I0*exp(-t/tau)
Flux= [L*mu*I*ln(1+w/d)] / 2*pi
V (or EMF) = d(flux)/dt = [ (L*mu*ln(1+w/d)) / 2*pi ]*(-I0*exp(-t/tau))
where this, (-I0*exp(-t/tau)) , is the time derivative of I
P=(V^2)/R
Energy= integral(P)

The Attempt at a Solution


I already got the previous questions for this problem. The answers resulted in: Flux for one turn of the coil at 2.6 seconds= 2.83×10-8 T*m^2, EMF for entire coil at 2.6 seconds= 1.32×10-5 V, and the power dissipated from the coil at 2.6 seconds=2.19×10-11 W.

I just don't know how to integrate the power equation.
Thanks!
 
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You left out 1/tau while differentiating with respect to time.
The dissipated energy is the integral of the power from t= to t=2.6 s. And the power is (V^2)/R as you have shown. The emf is of the form C exp(-t/tau) where C is a constant. What is its square?
You certainly know what is the integral of an exponential function.

ehild
 
ehild said:
You left out 1/tau while differentiating with respect to time.
The dissipated energy is the integral of the power from t= to t=2.6 s. And the power is (V^2)/R as you have shown. The emf is of the form C exp(-t/tau) where C is a constant. What is its square?
You certainly know what is the integral of an exponential function.

ehild

Well, I actually had the 1/tau in my work I just accidentally didn't type it. Well, the intergral of exp(-t/tau) would just be -tau*exp(-t/tau) ?? So the emf would just be -(tau^2)*exp(-(t^2)/(tau^2)) ? and divide by same R i was using ? It's that simple ? What would the constant be?
 
Last edited:
Take care when you square an exponential function. (exp(x))^2=exp(2x)
And the square of a negative quantity is positive. ehild
 
ehild said:
Take care when you square an exponential function. (exp(x))^2=exp(2x)
And the square of a negative quantity is positive.


ehild

Wait, I'm confused so you square it first then take the integral or what
 
First square the emf as P=(V^2)/R , then integrate with respect to the time.

You wrote in a previous post that

"V (or EMF) = d(flux)/dt = [ (L*mu*ln(1+w/d)) / 2*pi ]*(-I0*exp(-t/tau))
where this, (-I0*exp(-t/tau)) , is the time derivative of I"

Here is a 1/tau missing. The time derivative of I is -I0*1/(tau)*exp(-t/tau), so the emf is

V=[ (L*mu*ln(1+w/d)) / 2*pi ]*(-I0(1/tau)*exp(-t/tau)).

You have to square this whole thing, divide by R and integrate.

ehild
 
ehild said:
First square the emf as P=(V^2)/R , then integrate with respect to the time.

You wrote in a previous post that

"V (or EMF) = d(flux)/dt = [ (L*mu*ln(1+w/d)) / 2*pi ]*(-I0*exp(-t/tau))
where this, (-I0*exp(-t/tau)) , is the time derivative of I"

Here is a 1/tau missing. The time derivative of I is -I0*1/(tau)*exp(-t/tau), so the emf is

V=[ (L*mu*ln(1+w/d)) / 2*pi ]*(-I0(1/tau)*exp(-t/tau)).

You have to square this whole thing, divide by R and integrate.

ehild

Yea, I know I left that out by accident. So V^2= [L^2*mu^2*I0^2*(ln(1+w/d))^2*exp(-2t/tau)] / 4*pi^2*tau^2 ?

So P= V^2/R= [(L^2*mu^2*I0^2*(ln(1+w/d))^2*exp(-2t/tau)) / 4*pi^2*tau^2] / R

Take the integral of that, would you pull everything out except for exp(-2t/tau) ? So really you are just integrating that, the rest a constants ? So the integral of exp(-2t/tau) would equal -((tau*exp(-2t/tau))/2) ?



Or no, it wouldn't be exp(-2t/tau) it would be exp(t^2/tau^2) ? but to integrate that I'm not sure of .. Ughh, I'm so confused for no reason =(
 
Last edited:
arl146 said:
So P= V^2/R= [(L^2*mu^2*I0^2*(ln(1+w/d))^2*exp(-2t/tau)) / 4*pi^2*tau^2] / R

Take the integral of that, would you pull everything out except for exp(-2t/tau) ? So really you are just integrating that, the rest a constants ? So the integral of exp(-2t/tau) would equal -((tau*exp(-2t/tau))/2) ?

Yes, integrate the exponential function between t=0 and t=2.6 s and multiply by everything else.

arl146 said:
Or no, it wouldn't be exp(-2t/tau) it would be exp(t^2/tau^2) ? but to integrate that I'm not sure of .. Ughh, I'm so confused for no reason =(

Forget exp(t^2/tau^2). exp(x) is e on the x-th power ex. (ex)^2=(ex)*(ex)=e(x+x)=e2x.

ehild
 
ehild said:
Forget exp(t^2/tau^2). exp(x) is e on the x-th power ex. (ex)^2=(ex)*(ex)=e(x+x)=e2x.

ehild

Oh, okay. Thanks ^.^ I'll try it out and if there's a problem, I'll be back after I try it out a few times! Hopefully I won't have to.
 
  • #10
Okay, I have a problem. This is all of my work:


V= -\frac{L \mu ln(1+w/d) (I0) exp(-t/\tau)}{2 \pi \tau}

V2 = \frac{L^2 \mu^2 (ln(1+w/d))^2 I0^2 exp(-2t/\tau)}{4 \pi^2 \tau^2}


P= \frac{V^2}{R}

\int P dt = Energy = \frac {L^2 \mu^2 (I0^2) (ln(1+w/d))^2}{4 \pi^2 \tau^2 R} * \int exp(-2t/\tau) dt

E= \frac {L^2 \mu^2 (I0^2) (ln(1+w/d))^2}{4 \pi^2 \tau^2 R^2} * [ exp(-2t/tau)*(-tau/2) ]

the boundaries on that is 0 to 2.6 ;
my answer i got after many times of trying was 2.773358998E-17 J
What is wrong ?
 
  • #11
I do not see N (the 2000 turns).

ehild
 
  • #12
Ohhhhh ... *facepalm* I even thought of that but figured that wasn't right so I didn't even try it. Thanks! again!
 
  • #13
Can I just multiply by answer above by N^2 ?
 
  • #14
arl146 said:
Can I just multiply by answer above by N^2 ?
It would be enough, but there is some other computational error somewhere. It was not a good idea to square everything separately. Evaluate the constant of V first before squaring. And you can cancel pi as mu=4pi˙10-7.

ehild
 
  • #15
I mean, how do you square it without squaring each thing separately ? ...and what do you mean evaluate the constant of V first?
 
  • #16
Here is a simple example: evaluate (2*3)2. You can do it by evaluating 2*3 first, then squaring the result: it is 62=36,
or squaring separately: 22*32=4*9=36.

And I found just now that you divided V^2 by R^2 instead of R.

ehild
 
  • #17
No, I divided by R I don't know why I put R^2. But I got the answer. All I needed to do was multiply by N^2. thanks for the help
 
  • #18
Splendid!
You are welcome.

ehild
 

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