Calculate the B field inside and outside a wire

AI Thread Summary
To calculate the magnetic field B inside and outside a long, straight wire with a given current density J = J0e−β(α−ρ)uz, the current I must first be determined by integrating the current density over the wire's cross-sectional area. The integration should be performed with respect to the area element dA, leading to the expression for current I. The magnetic field B can then be derived using the formula B = (μIρ)/(2πa^2). Clarification on the limits of integration is necessary, particularly since the problem assumes a steady state with J0 as the initial value. The discussion emphasizes the importance of correctly applying the integration limits and understanding the context of the variables involved.
DODGEVIPER13
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Homework Statement


A long, straight wire of radius a has current density J = J0e−β(α−ρ)uz where β is a
constant and ρ < α. Determine B inside and outside the wire.

Homework Equations


J=I/((pi)a^2)
B=(μIρ)/(2(pi)(a)^2)

The Attempt at a Solution


Here is what I did B=(μρ/2)J0e^(-β(alpha-ρ))
 
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Is the problem confusing?
 
DODGEVIPER13 said:
Is the problem confusing?

Not at all. First find i by integrating J then find B. di = JdA
 
So ∫J0e^-β(α-ρ) from 0 to a but what should I integrate with respect too?
 
J=di/dA maybe?
 
well since beta is constant and alpha is greater than rho then e^(-beta(alpha-rho)) whould go to 0 if I took the limit from 0 to infinty
 
hmmm well I guess the problem does not consider time as it uses J0 which I assume stands for the intial value
 
So my limit I idea is flawed then
 
Anything else?
 
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