Inducing an EMF in an Aluminum Ring

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An aluminum ring with a radius of 5.00 cm and a resistance of 2.65 x 10^-4 Ω is placed around an air-core solenoid with 970 turns per meter, where the current is increasing at 270 A/s. The induced electromotive force (emf) can be calculated using the changing magnetic flux through the ring, which is assumed to be half the magnetic field strength at the center of the solenoid. The magnetic field (B) in the solenoid is given by B = μ0(turns/length)(current), and the flux through the ring can be derived from the area of the solenoid's end. The final expression for emf incorporates the magnetic field, the rate of change of current, and the area of the solenoid. This discussion emphasizes the relationship between changing current in the solenoid and the induced emf in the aluminum ring.
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Homework Statement



31-p-009.gif


An aluminum ring of radius r1 = 5.00 cm and a resistance of 2.65 x 10^-4 Ω is placed around one end of a long air-core solenoid with 970 turns per meter and radius r2 = 3.00 cm as shown in the figure. Assume the axial component of the field produced by the solenoid is one-half as strong over the area of the end of the solenoid as at the center of the solenoid. Also assume the solenoid produces negligible field outside its cross-sectional area. The current in the solenoid is increasing at a rate of 270 A/s.

Homework Equations

ε = d(magnetic flux) / dtmagnetic flux = ∫(B)(dA)I = ε / Rmagnetic field in a solenoid:

B = μ0(turns / length)(current)Ampere's law? :

∫B ds = μ0I(+ some other formula / combination I'm probably missing)

The Attempt at a Solution


I think I mostly need help just finding the induced emf (ε). I know you're to somehow find the magnetic flux of what I believe is the ring. Afterwards you find the magnetic flux and you can divide it by time (rather the time interval in which the magnetic flux changes) giving you the induced emf?

But it's complicated because there's changing current instead, which is in the solenoid, and I am not sure what to do about it, or how it relates to the change in flux over time. At the end you divide the induced emf by the resistance of the ring giving you the induced current.
 
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Hi Color_of_Cyan! :smile:
Color_of_Cyan said:
magnetic field in a solenoid:

B = μ0(turns / length)(current)

I think I mostly need help just finding the induced emf (ε).

I don't see the difficulty :confused:

B = μ0(turns / length)(current),

so dB/dt = μ0(turns / length)d(current)/dt​
 


tiny-tim said:
Hi Color_of_Cyan! :smile:I don't see the difficulty :confused:

B = μ0(turns / length)(current),

so dB/dt = μ0(turns / length)d(current)/dt​
Sorry if I sound dumb:If I solve for flux how do I account for the magnetic field that you now show is changing? (I'm really not too good with calculus either just so you know)I'm thinking since flux = ∫B dA

Then flux = ∫[ (dB/dt)(dA) ] ? (Not sure what to do about this)

On the subject of flux of the RING, the area is still πr2 right, even though it's a ring?

I guess the flux is changing as well since the magnetic field is changing. I'm thinking something along the lines that

flux = μ0(970 turns / meter)[ π(0.05m)2]

then emf is just = μ0(970 turns / meter)[ π(0.05m)2](270A / time change in s)

?
 
flux = ∫B dA

so d(flux)/dt = ∫[ (dB/dt)(dA) ]
On the subject of flux of the RING, the area is still πr2 right, even though it's a ring?

what matters is the flux through the ring

but the question tells you not to bother to calculate it properly …

it tells you to assume that the flux through the ring (radius r1) is simply the flux through radius r2, and also that the B field there is half the B field at the centre of the solenoid
 


Yes I meant flux through the ring, my bad.
tiny-tim said:
it tells you to assume that the flux through the ring (radius r1) is simply the flux through radius r2, and also that the B field there is half the B field at the centre of the solenoid

I can't see where you got that the flux through the ring is the same as the flux through r2 though


So, the flux would be the same using the area of the solenoid end though? Also multiply by 1/2 ?

So would it be

flux = ∫B dA

emf = d(flux)/dt

emf = (1/2)(μ0)(970 turns / meter)(270 A / s)[∏(0.03m)2]

?
 
Color_of_Cyan said:
I can't see where you got that the flux through the ring is the same as the flux through r2 though

from …
Color_of_Cyan said:
… Assume the axial component of the field produced by the solenoid is one-half as strong over the area of the end of the solenoid as at the center of the solenoid. Also assume the solenoid produces negligible field outside its cross-sectional area.

since the ring is perpendicular to the axis, and since the field is obviously cylindrically symmetrical, that means only the axial component is relevant to the flux through the ring

and it specifically tells you to ignore any field outside r2

so the flux through the ring (r1) is the same as the flux through r2 :wink:
So, the flux would be the same using the area of the solenoid end though? Also multiply by 1/2 ?

So would it be

flux = ∫B dA

emf = d(flux)/dt

emf = (1/2)(μ0)(970 turns / meter)(270 A / s)[∏(0.03m)2]

?

looks good! :smile:
 


Thanks.
 

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