Step-by-step explanation:
For this problem we have to take into account the expression
J = I/area = I/(π*r^(2))
By taking I we have
I = π*r^(2)*J
(a)
For Ja = J0r/R the current is not constant in the wire. Hence

and on the surface the current is

(b)
For Jb = J0(1 - r/R)

and on the surface

(c)
Ja maximizes the current density near the wire's surface
Additional point
The total current in the wire is obtained by integrating

and in a simmilar way for Jb
![I_(T)=\pi J_(0) \int\limits^R_0 {r^(2)(1-r/R)} \, dr = \pi J_(0)[(R^(3))/(3)-(R^(2))/(2R)]=\pi J_(0)[(R^(3))/(3)-(R^(2))/(2)]](https://img.qammunity.org/2021/formulas/physics/college/9tam9fkzgbr9w00otvn9ujmooyl1pyp3eq.png)
And it is only necessary to replace J0 and R.
I hope this is useful for you
regards