Magnetized Toroid Problem 6.10 - Griffiths EM

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The discussion revolves around solving problem 6.10 from Griffiths' Electromagnetism, which involves finding the magnetic field at the center of a gap in a bent iron rod with uniform magnetization. The initial approach suggests using the formula for the magnetic field inside a toroid and relating the total current to the magnetization. Participants clarify that the bound surface current is equal to the magnetization, allowing for the calculation of total current. The final expression for the magnetic field is refined to account for the geometry of the setup, leading to a conclusion that the field should not depend on the length of the rod. The conversation emphasizes the importance of correctly interpreting the relationships between magnetization, current, and geometry in magnetic field calculations.
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Hello,

I needed some help with a problem from the Griffiths Book on EM. It's problem number 6.10 if anyone has the book. Here is the problem and I have attached a crude drawing using MSPaint.

An iron rod of length L and square cross section (side a), is given a uniform longitudinal magnetization M, and then bent around into a circle with a narrow gap (width w). Find the magnetic field at the center of the gap, assuming w << a << L. [Hint: treat it as the superposition of a complete torus plus a square loop with reversed current.]

The field inside a toroid is: B= \frac{\mu_0 NI}{2\pi s}. The hint would lead me to believe that I can take NI -> M. The field at the center of the gap due to a loop of current in the opposite direction would be:B=-\frac{2\sqrt{2}\mu_0 I}{\pi a}.

This means the answer would be:
B=\frac{\mu_0 NI}{L} - \frac{2\sqrt{2}\mu_0 I}{\pi a}.

However I don't see how to resolve the current(I) in this problem. Is there a way to relate M and I or am I going about this problem in the completely wrong direction.
 

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buhthestuh said:
The field inside a toroid is: B= \frac{\mu_0 NI}{2\pi s}. The hint would lead me to believe that I can take NI -> M.
Not quite. NI would be the TOTAL current in the toroid. You've probably figured out the bound surface current is K_b=M. So knowing you have this bound surface currentm you can solve for the total current and equate that NI.
 
Ok it seems then that the field should be

B = \frac{\mu_0 M}{L} - \frac{2\sqrt{2}\mu_0 Mw}{\pi a}<br />

or

<br /> B = \mu_0 M \left[ \frac{1}{L} - \frac{2\sqrt{2}w}{\pi a} \right]<br />

However since L >> a and 2\sqrt{2}w &gt;&gt; 1 the field would be negative. But that seems proposterous considering that w is just a minute width compared to the whole of the toroid.
 
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That ain't right. How'd you get the L? The field shouldn't depend on L. (It also doesn't add up unit wise).

For the whole loop the total current is K_b(2\pi s) so B=\mu_0M.
The rest is all ok.
 

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