A wire is aligned with the z -axis and carrying a current, with a steady current density of J = ( 0 , 0 , x 2 + y 2 ) for x 2 + y 2 ≤ 3 6 . The current produces a magnetic field B ( x , y , z ) ; Amp e ˋ re's circuital law tells us that ∇ × B = μ 0 J , where μ o is the magnetic constant.
Find μ 0 ∣ ∣ B ( 8 , 6 , 4 ) ∣ ∣ .
(from a recent test on vector calculus)
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Yes, exactly!! Very clearly and lucidly explained! Thank you!
My vector calculus class is about Maths, not Physics, at least according to the course catalogue. Maxwell's equations are not discussed in class, and the students are not expected to know them. In this problem, they are supposed to use Stokes' Theorem to get from the given differential form of Ampere's law to the integral form:
∫ ∂ S B ⋅ d s = ∫ S c u r l B ⋅ d S = μ 0 ∫ S J ⋅ d S where S is the disk x 2 + y 2 ≤ 1 0 0 , z = 4 . The ensuing computations are exactly those you performed, of course.
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I prefer the integral form of Ampere's law:
∫ C B ⋅ d ℓ = μ 0 I e n c l o s e d
Since the magnetic field is circular and constant in magnitude at a given radius, this reduces to:
2 π R B = μ 0 I e n c l o s e d R = 8 2 + 6 2 = 1 0 B = 2 0 π μ 0 I e n c l o s e d
Now to find the enclosed current:
∣ J ∣ = r d A = 2 π r d r d I = ∣ J ∣ d A = 2 π r 2 d r 0 ≤ r ≤ 6 I e n c l o s e d = 2 π ∫ 0 6 r 2 d r = 1 4 4 π
The B-field at the measurement point is therefore:
B = 2 0 π μ 0 1 4 4 π μ 0 B = 5 3 6 = 7 . 2