91Ó°ÊÓ

Magnetic field is$0.40\mathrm{T}$

Radius of top face is

$\begin{array}{c}\mathrm{r}=4.2\mathrm{cm}\\ =4.2×{10}^{-2}\mathrm{m}\end{array}$

Here, we have to use the formula for the magnetic flux in terms of the magnetic field and area. As the total flux passing inward for any closed surface is equal to the total flux going out. we can find the flux through the curved surface.

Formula:

$\mathrm{A}={\mathrm{Ï€°ù}}^2$

$\mathrm{Ï•}=\mathrm{BA}$

The magnitude of the magnetic flux.

The area of the top face is as follow:

$\begin{array}{c}\mathrm{A}={\mathrm{Ï€°ù}}^2\\ =\mathrm{Ï€}{(4.2×{10}^{−2})}^2\end{array}$

So, the flux passing through the top surface is

$\begin{array}{c}{\mathrm{ϕ}}_{\mathrm{top}}=\mathrm{BA}\\ =0.4×\mathrm{π}×{(4.2×{10}^{−2})}^2\\ =2.125×{10}^{-3}\mathrm{Wb}\end{array}$

So, the net flux inside the surface is

$\begin{array}{c}\mathrm{ϕ}={\mathrm{ϕ}}_{\mathrm{bottom}}+{\mathrm{ϕ}}_{\mathrm{top}}\\ =7.0×{10}^{−3}+2.125×{10}^{−3}\\ =9.21×{10}^{-3}\mathrm{Wb}\end{array}$

Now, the total inward flux is equal to the total outward flux

${\mathrm{Ï•}}_{\mathrm{in}}={\mathrm{Ï•}}_{\mathrm{out}}$

Hence, the magnitude of the magnetic flux through the curved surface is

$\mathrm{ϕ}=9.21×{10}^{-3}\mathrm{Wb}$

The direction of the flux.

As the flux is going out through both the top and the bottom flat surfaces, the direction of the flux through the curved surface must be inward.