The total current is defined as the current density integrated over the cross-sectional area:
I = ∫JdA
I = total current, J = current density, dA = area element
We already have I as a given quantity:
J = (J₀/R)r
We need to find dA in terms of another variable so we can actually calculate the integral:
A = πr²
Differentiate both sides with respect to r:
dA/dr = 2πr
dA = 2πrdr
The conductor has a radius R, so set the integration bounds to [0, R]. Set the integrand to (2πJ₀/R)[tex]r^{2}[/tex] with r being the variable of integration.
I = (2πJ₀/3R)[tex]r^{3}[/tex] evaluated between r = 0 and r = R
I = (2πJ₀/3R)[tex]R^{3}[/tex]
I = (2πJ₀/3)[tex]R^{2}[/tex]
I = 2π[tex]R^{2}[/tex]J₀/3
Substitute π[tex]R^{2}[/tex] with area A:
I = 2AJ₀/3