How does the radial current density affect the area element dA in Ampere's Law?

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The discussion centers on the application of Ampere's Law to a solid cylindrical wire with a radially varying current density described by the equation J=J0*r^2. The key formula used is B*2*pi*r = μ0 * ∫J dA, where dA is defined as 2*pi*r*dr for cylindrical coordinates. This definition arises from the geometry of the cylindrical shell, where dA represents the area of an infinitesimally thin ring at radius r. The current density is confirmed to vary radially, not along the length of the cylinder.

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Ampere's Law question (need quick answer test tomorrow)

Using Ampere's Law on a solid cylindrical wire with radius R and a current density in the direction of the symmetry axis of the wire. The current density varies radially. J=J0*r^2. What is the magnitude of the the magnetic field when r>R, outside the wire?

Using the formula B*2*pi*r= U0* [tex]\int[/tex]J dA. Which equals B*2*pi*r = U0 * [tex]\int[/tex] J0* r^2 dA.

Now why does dA = 2*pi*r dr?
Can you guys give me an explanation? How does the information that the current density varies radially show that dA= 2*pi*r*dr? I am having trouble visualizing dA.

If the current density varied along the length of the cylinder wouldn't dA= pi*r^2dx? Would the current density vary along the length of the cylinder or will the current density always vary radially?

Thanks for the help.
Stephen
 
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