Solving Faraday's Disk: Induced Voltage & Max Current

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Discussion Overview

The discussion revolves around calculating the induced voltage and maximum current in Faraday's disk, which rotates in a homogeneous magnetic field. Participants explore the relationship between angular velocity and the rotational speed of the disk, as well as the implications for induced electromotive force (emf) and current through a resistor. The context includes both theoretical and mathematical reasoning related to electromagnetic induction.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation
  • Exploratory

Main Points Raised

  • Some participants express uncertainty about how to relate the rotational speed of the disk (1000 rpm) to angular velocity (ω), seeking clarification on the conversion between these units.
  • There is a discussion on the formula for induced voltage, with some participants proposing the integration of the expression for induced emf from radius r1 to r2.
  • One participant suggests that the direction of rotation affects the polarity of the induced voltage, while others note that the angle between the velocity vector and the magnetic field remains 90 degrees regardless of rotation direction.
  • Participants explore the relationship v = ωr, with some providing intuitive explanations for why this relationship holds in the context of the rotating disk.
  • Some participants emphasize the need to understand the physical meaning behind the equations and the implications of the geometry of the disk on the induced voltage.

Areas of Agreement / Disagreement

Participants generally agree on the need to clarify the relationship between rotational speed and angular velocity, but there is no consensus on the best way to approach the integration for induced voltage or the implications of the direction of rotation on voltage polarity.

Contextual Notes

Participants note that the integration limits for the induced voltage calculation should be from r1 to r2, but there is some confusion regarding the exact form of the velocity as a function of radius. Additionally, the discussion highlights the importance of understanding the physical context of the equations used.

cdummie
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Homework Statement


Faraday's disk with radius of axle r1 and radius of disc r2 is shown in the picture below. Disc rotates in the homogenous magnetic field whose vector B is vertical to the disc. If disc is spinning 1000 rpm find induced voltage between r1 and r2 and what is maximal value of current through the resistor. Known values are: B=1T, r1=1cm, r2=20cm and R=10 Ω.

Screenshot_1.png


Homework Equations


eind=∫(v×B)dl

The Attempt at a Solution



Eind=v×B=vBsin(v,B)

if there's 1000 rpm that is 16.7 rps and that is what i don't know, what to do next?
 
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cdummie said:

Homework Statement


Faraday's disk with radius of axle r1 and radius of disc r2 is shown in the picture below. Disc rotates in the homogenous magnetic field whose vector B is vertical to the disc. If disc is spinning 1000 rpm find induced voltage between r1 and r2 and what is maximal value of current through the resistor. Known values are: B=1T, r1=1cm, r2=20cm and R=10 Ω.

View attachment 87128

Homework Equations


eind=∫(v×B)dl

Just perform the integration from l = r1 to l = r2. What is v(l)?

 
rude man said:
Just perform the integration from l = r1 to l = r2. What is v(l)?
Ok, this is what i have:

eind=∫(v×B)dl (i can't put limits of integration here but they are r1 lower and r2 upper limit)

Eind=v×B=vBsin(v,B) , since there's no data about direction of the rotation i will assume it's counterclockwise (even though i think it doesn't matter because even if direction of ω is clockwise, angle between v and B would remain 90 degrees)
anyway,

Eind=vB=ωrB since v=ωr, direction of Eind[/SUB is radial.

Now, back to eind

eind=∫ωrBdl*cos(Eind,dl) since both Eind and dl are radial (it also means i can write dl as dr) then cosine between them is 1, so i have:

eind=∫ωrBdr (again, limits of integration are: r1 lower and r2 upper)

eind=ωB(r22 r21)/2

Now, i have B and i have both r1 and r2 but i don't know how is the fact that disc is spinning 1000rpm is related to angular velocity (ω), that is the only thing missing, i mean, it's what i don't understand.

Now for the current through the resistor, it is just:

I=eind/R correct me if i made a mistake somewhere, but main problem is that i don't know the relation between speed of spinning and angular velocity.
 
cdummie said:
Eind=v×B=vBsin(v,B) , since there's no data about direction of the rotation i will assume it's counterclockwise (even though i think it doesn't matter because even if direction of ω is clockwise, angle between v and B would remain 90 degrees)
Right, but the polarity of the voltage will be determined by the direction of rotation.
Now, i have B and i have both r1 and r2 but i don't know how is the fact that disc is spinning 1000rpm is related to angular velocity (ω), that is the only thing missing, i mean, it's what i don't understand.
Angular velocity is radians per second. rpm is rotations per minute.
How many radians in 1 rotation?
How many seconds in 1 minute? You've done well so far, this should be a gimme. Like figuring out mph vs. ft per second!
You wrote v = ωr, you need to fully understand this relationship. Why is v = ωr?
Otherwise - good!
For one way to better understanding the physics, think of the disc as comprising a lot of thin radial wires each separated by thin insulation. The wires are thus all connected in parallel so the voltage is the same for all wires as they cut the flux lines of B. You learned emf = (B x l)⋅v I'm sure for a length of wire l. Least that's how I think of the Faraday disc.
 
rude man said:
Right, but the polarity of the voltage will be determined by the direction of rotation.

Angular velocity is radians per second. rpm is rotations per minute.
How many radians in 1 rotation?
How many seconds in 1 minute? You've done well so far, this should be a gimme. Like figuring out mph vs. ft per second!
You wrote v = ωr, you need to fully understand this relationship. Why is v = ωr?
Otherwise - good!
For one way to better understanding the physics, think of the disc as comprising a lot of thin radial wires each separated by thin insulation. The wires are thus all connected in parallel so the voltage is the same for all wires as they cut the flux lines of B. You learned emf = (B x l)⋅v I'm sure for a length of wire l. Least that's how I think of the Faraday disc.

Well, in one rotation there's 2π radians, since one rotation means one full circle, and there's 60s in one minute, so i have to multiply value i have for rpm with radians and then divide it by 60. The way i think of relation v=ωr is that v is velocity as if the object that spins with angular velocity ω stops going around making circles because the whole system stops spinning and the object being there spinning along with the system (Faraday's disc in this case) just slips off, and the direction where it goes after that is the direction that vector v has at that point (this is the way i think of it). Since, in cases like this vectors r and ω are orthogonal it means that their cross product will give the direction of vector v at any point along the circle. Anyway, thanks a lot for the help!
 
cdummie said:
Well, in one rotation there's 2π radians, since one rotation means one full circle, and there's 60s in one minute, so i have to multiply value i have for rpm with radians and then divide it by 60. The way i think of relation v=ωr is that v is velocity as if the object that spins with angular velocity ω stops going around making circles because the whole system stops spinning and the object being there spinning along with the system (Faraday's disc in this case) just slips off, and the direction where it goes after that is the direction that vector v has at that point (this is the way i think of it). Since, in cases like this vectors r and ω are orthogonal it means that their cross product will give the direction of vector v at any point along the circle. Anyway, thanks a lot for the help!
That sounds OK, at least your computation of ω is. But perhaps you're complicating the formula v = ωr. Think of a round race track, radius r. You're running around it with ω. Should be clear that your ground speed is v = ωr, ω in rad/s, r in meters, v in m/s.
 
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