rude man said:
"Curling around it' is in the theta direction! Just apply Ampere's law to a B loop within a < r < b.
sorry got confused by the diagram
rude man said:
That's a very general statement, and incorrect. It's true for example that a charge is not affected by its own E field alone but certainly a current can produce its own B field, including within the current that causes it! And so the Lorentz force can exert a force on the shell.
thanks for the wonderful hint really helped me to see what is going on
rude man said:
I don't understand why this statement is made. The thickness is b - a.
now i know why it is because in this competition the use of integrals is not needed but can be used
with that being said i proceed by using integrals
by considering the cross sectional area of the cylinder
a ring of internal radius r and external radius of r + Δr
magnetic field in the ring
L - length of cylinder
J - current density
##
B = \frac{J \pi(r^2 - a^2) \mu_o}{2 \pi r}\\
I = J 2 \pi r dr\\
df= I L B\\
df = L \frac{J \pi(r^2 - a^2) \mu_0}{2 \pi r}J 2 \pi r dr\\
df = L \mu_0 J^2 \pi(r^2 - a^2) dr
##
is this the answer for the question
is the force radially outward
assuming it is correct (correct me if am wrong)
moving on to the next part of the question about calculating the pressure on curved walls##
\int df = \int _{r = a} ^b L \mu_0 J^2 \pi(r^2 - a^2) dr\\
F = L \mu_0 J^2 \pi \int _{r = a} ^b (r^2 - a^2) dr\\
F = L \mu_0 J^2 \pi [\frac{r^3}{3} - a^2 r]_a ^b\\
P = \frac{L \mu_0 J^2 \pi [\frac{r^3}{3} - a^2 r]_a ^b}{2 \pi b L}\\
##
how am i supposed to get a muerical answer out of this help again?
edit:
or for pressure on curved surface am i only supposed to use the force on the outermost shell