Calculating Heat Generated in a Coil due to Changing Current and Resistance

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SUMMARY

The discussion focuses on calculating the heat generated in a coil with resistance R due to a charge q passing through it while the current decreases uniformly to zero over a time interval Δt. The relevant equations include dH = i²Rdt and i = dq/dt. Participants explore the relationship between current, charge, and time, ultimately deriving the equation i = i₀ - at, where i₀ is the initial current and a is a constant related to the rate of decrease. The final expression for heat generated is H = (i₀²RΔt - aRΔt²/2).

PREREQUISITES
  • Understanding of electrical concepts such as current, resistance, and charge.
  • Familiarity with calculus, particularly differential equations and integration.
  • Knowledge of the relationship between current and charge over time.
  • Ability to manipulate and solve equations involving multiple variables.
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  • Study the derivation of the heat equation in electrical circuits, focusing on dH = i²Rdt.
  • Learn about the integration of piecewise linear functions to understand current decay.
  • Research the relationship between charge, current, and time in electrical systems.
  • Explore advanced topics in thermodynamics related to heat generation in resistive materials.
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AdityaDev
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Homework Statement



What amount of heat will be generated in a coil of resistance R due to a charge q passing through it if the current in the coil decreases down to zero uniformly during a time interval ##\Delta t##

Homework Equations



##dH=i^2Rdt##
##i=\frac{dq}{dt}##

The Attempt at a Solution


##dH=i^2Rdt##
##dH={\frac{dq}{dt}}^2Rdt##
##dH=\frac{{dq}^2R}{dt}##
How do I solve this multi variable differential equation?
 
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AdityaDev said:

Homework Statement



What amount of heat will be generated in a coil of resistance R due to a charge q passing through it if the current in the coil decreases down to zero uniformly during a time interval ##\Delta t##

Homework Equations



##dH=i^2Rdt##
##i=\frac{dq}{dt}##

The Attempt at a Solution


##dH=i^2Rdt##
##dH={\frac{dq}{dt}}^2Rdt##
##dH=\frac{{dq}^2R}{dt}##
How do I solve this multi variable differential equation?
Your are told the current decreases uniformly with time. Write that as an equation.
 
haruspex said:
Your are told the current decreases uniformly with time. Write that as an equation.
##i=-at##
##di=-adt##
##dH=iR^2dt##
##dH=-aR^2tdt##
##H=-aR^2\frac{t^2}{2}##
 
I see an unknown a appearing, whereas the known (given) q has disappeared.
And the math leaves to be desired:
  • ##i = -at## can't be right (try ## t=0## and ## t = \Delta t##)
  • Any reason for ##i^2R## changing into ##iR^2## ?
With ##t## in the answer I suppose you mean ##\Delta t## ?
Any chance to present the answer in terms of the givens ?
 
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BvU said:
  • Any reason for ##i^2R## changing into ##iR^2## ?
Big typing mistake sorry
##di/dt = -a##
This shows that i decreases with time, just like dN/dt=-N for nuclear decay.
Hence you will again get I=-at.
 
AdityaDev said:
Big typing mistake sorry
##di/dt = -a##
This shows that i decreases with time, just like dN/dt=-N for nuclear decay.
Hence you will again get I=-at.
You're forgetting the constant of integration. The current starts positive and finishes at zero. And you need to relate a to q.
And it is not like nuclear decay which follows a negative exponential with time, not linear.
 
haruspex said:
You're forgetting the constant of integration. The current starts positive and finishes at zero. And you need to relate a to q.
And it is not like nuclear decay which follows a negative exponential with time, not linear.
##i = i_0 - at##
##dH= (i_0 - at)^2Rdt##
##H=i_0^2Rt - aRt^2/2##
 
Still this annoying a ...

And a strange result for the integral...
 
BvU said:
Still this annoying a ...
##i=i_0-bt##
Please help me solve this
 
  • #10
You can't exclude a because the equation will become dimensionally incorrect
 
  • #11
BvU said:
  • ##i = -at## can't be right (try ## t=0## and ## t = \Delta t##)
Now it fits for t=0. Next: make it fit for ## t = \Delta t##.
And (to keep in the back of your mind): ##q = \int_0^{\Delta t}\; i \;dt ## to eliminate ##I_0##

[edit] from zero to Delta t
 
  • #12
BvU said:
Now it fits for t=0. Next: make it fit for ## t = \Delta t##.
##i=\frac{q}{\Delta t} - at##
 
  • #13
No that doesn't seem right.
 
  • #14
##i=i_0 - \frac{i_0t}{\Delta t}##
 
  • #15
##i=i_0-at## not good ? try ##i=i_0-bt## or ##i=i_0-ct## :)

Reminded me of this joke where you see Einstein in front of a blackboard with ## E=ma^2 ## and ## E=mb^2 ## stricken through, and then ## E=mc^2 ## ! (with an exclamation mark). Sorry.

What I am pushing towards: ##i=i_0-at## is correct, but not good enough. t = 0 works fine, now fill in ##\Delta t## when you know ##i(\Delta t) = 0 ## you get a.
Bit now you have ##i_0## as unknown. However, ... (see post #11)

[edit] crossed post #14. Bingo !
 
  • #16
BvU said:
What I am pushing towards: ##i=i_0-at## is correct, but not good enough. t = 0 works fine, now fill in ##\Delta t## when you know ##i(\Delta t) = 0 ## you get a.
Bit now you have ##i_0## as unknown. However, ... (see post #11)
Ok...here comes my updated equation
##i=\frac{q}{\Delta t} - \frac{q}{(\Delta t)^2}t##
 
  • #17
Almost :)
 
  • #18
Is it correct?
Now can I use i2Rt?
 
  • #19
Almost means: not there yet: $$q \; {?\atop =}\ \int_0^{\Delta t}\; i \;dt = {q\over \Delta t} \int_0^{\Delta t} \;(1-{t\over \Delta t}) \; dt = {q} \int_0^{\Delta t} \;(1-{t\over \Delta t}) \; d({t\over \Delta t}) = q\int_0^1 (1-u) du = {q\over 2}$$so there is a 2 missing. Obvious if you sketch i(t), a triangle.
 
  • #20
At t=0,you get ##q=i\Delta t##.
Here you get Q=q/2
What is the difference between the two 'q's?
(I got the answer after using post 19. Thank you very much)
 
  • #21
No, at t=0 you get ##i = i_0 = {2q\Delta t}##

Q = q/2 ? There should come q = q !

And the picture refuses to be uploaded, sorry. Can't copy and paste a picture either. Must be some issue thanks to the security mafia.
1000 words:

a triangle from (0, ##I_0##) to (##\Delta t##, 0).

Area ##{1\over 2} I_0\Delta t \equiv q \Rightarrow I_0 = ...##
 
  • #22
BvU said:
Still this annoying a ...

And a strange result for the integral...
I don't know why you had this objection to introducing a. It should then have been a simple matter to find a in terms of q and ##\Delta t## by integrating.
 
  • #23
haruspex said:
I don't know why you had this objection to introducing a. It should then have been a simple matter to find a in terms of q and ##\Delta t## by integrating.
Yes, we're working on that. Nearly done (see post #16). Or completely -- I don't know what I can deduce from post #20.

It was more the duo ##i_0## and a , of which I picked a to eliminate. But you are referring to post #8; we are at over 20 now ...
 
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