Gauss' Law for magnetism, ∇⋅B=0 suggests we can generate a potential for B. What form should the definition of this potential take (Φ and A are placeholder scalar and vector functions, respectively)?
B=∇Φ
B=∇×Φ
B=∇⋅A
B=∇×A
Something else?!
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Consider a toroid, which is like a finite solenoid connected end to end. In which direction do you expect the B field to point?
Azimuthally (ˆϕ direction)
Radially (ˆs direction)
In the ˆz direction (perp. to page)
Loops around the rim
Mix of the above...
Which Amperian loop would you draw to find B “inside” the Torus (region II)?
Large "azimuthal" loop
Smallish loop from region II to outside (where B=0)
Small loop in region II
Like A, but perp to page
Something entirely different
With ∇2A=−μ0J, we can write (in Cartesian coordinates):
∇2Ax=−μ0Jx
Does that also mean in spherical coordinates that ∇2Ar=−μ0Jr?
Yes
No
We can compute A using the following integral:
A(r)=μ04π∫J(r′)Rdτ′
Can you calculate that integral using spherical coordinates?
Yes, no problem
Yes, r′ can be in spherical, but J still needs to be in Cartesian components
No.
For a infinite solenoid of radius R, with current I, and n turns per unit length, which is the current density J?
J=nIˆϕ
J=nIδ(r−R)ˆϕ
J=Inδ(r−R)ˆϕ
J=μ0nIδ(r−R)ˆϕ
Something else?!
Gauss' Law for magnetism, ∇⋅B=0 suggests we can generate a potential for B. What form should the definition of this potential take (Φ and A are placeholder scalar and vector functions, respectively)?
B=∇ΦB=∇×ΦB=∇⋅AB=∇×A
Something else?!
CORRECT ANSWER: D