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Re: [Phys-l] induced electric field



I'm in over my head...but I want to re-ask my question, and then I can work on the answer on my own:

"In a region in space where the magnetic field is steadily increasing at 1 T/s in the z-direction. A proton is released from rest at the point with (x,y,z) coordinates (1,0,0) . What is the magnitude and direction of the force that the proton experiences as a result of this changing field?"

Is this an answerable question as is or do I have to specify the boundary conditions that give rise to the increasing magnetic field? If it is answerable as is, what is the answer?! And why did the coordinates of the location matter?

Sorry if I am being obtuse. It isn't willful.

-----Original Message-----
From: phys-l-bounces@carnot.physics.buffalo.edu [mailto:phys-l-
bounces@carnot.physics.buffalo.edu] On Behalf Of John Mallinckrodt
Sent: Monday, November 23, 2009 4:38 AM
To: Forum for Physics Educators
Subject: Re: [Phys-l] induced electric field

On Nov 22, 2009, at 8:36 PM, John Denker wrote:

I think the shoe is on the other foot. Some folks are
assuming without proof -- indeed without evidence -- that
the squarish solution exists.

... proponents of squarish solutions are encouraged
to exhibit some such thing, in specific and formal terms,
and show that it solves the relevant Maxwell equation in
the given situation. I don't think it exists: too much
curl near the corners of the "square" and not enough
elsewhere.

Well, in fact, I actually did do some numerical calculations based on
a Biot-Savart-like transformation of Faraday's law and they clearly
do support the "squarish solution."

It shouldn't surprise anyone that the solution we seek is identical
in form to that for the B-field produced by a uniform current density
within a region having a square cross section. For a quick and dirty
solution I set up a spreadsheet with a 20x20 array of 400 "wires"
carrying "current" in the +z direction and used it to calculate the
resulting field at arbitrary positions in the x-y plane. Inside the
square, the solution is a little too too susceptible to the varying
distance to the nearest wire to be reliable, but outside the solution
is quite stable and smooth. For a radius of 15 units, I calculated
the B-field every 3 degrees from 0 to 45 degrees and found that the
field is purely tangential at 0 and 45 degrees as expected, but has a
positive radial component for angles in between (and a negative
radial component for angles between 45 and 90 degrees.) In addition,
I found that the field increases monotonically in magnitude as one
moves from 0 to 45 degrees. These are exactly the signatures one
would expect for the squarish solution and I would further expect the
boundary conditions to require the "squarish solution" to propagate
into the inner region.

John Mallinckrodt
Cal Poly Pomona
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