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Question: If the electric field to the right of two sheets is \(\dfrac{{K\sigma }}{{{\varepsilon _0}}}\). Find...

If the electric field to the right of two sheets is Kσε0\dfrac{{K\sigma }}{{{\varepsilon _0}}}. Find KK ?

Explanation

Solution

In order to solve this question we need to understand gauss law for electro statistics. According to gauss law, net flux enclosed by a closed surface is equal to net charge enclosed by surface divided by permittivity of free space ε0{\varepsilon _0} also the flux is equivalent to E.dS\oint {\vec E.d\vec S} . Here, E\vec E is an electric field and dSd\vec S is an elemental area vector having direction normal to the plane of the surface. Using this we can calculate electric fields across any surface.

Complete step by step answer:
Consider a plane sheet of charge having surface charge distribution σ\sigma .Then using gauss law, we get electric field around sheet as,
E=σ2ε0n^\vec E = \dfrac{\sigma }{{2{\varepsilon _0}}}\hat n
Consider a point P in right side of both sheets, then electric field at P due to plane sheet of charge distribution is, E1=σ2ε0{E_1} = \dfrac{\sigma }{{2{\varepsilon _0}}} having direction away from each other. And, electric field at P due to plane sheet of charge distribution is, E2=σ2ε0{E_2} = \dfrac{{ - \sigma }}{{2{\varepsilon _0}}} having direction towards it.So from superposition principle, net electric field is due to,
E=E1+E2E = {E_1} + {E_2}
E=σ2ε0+σ2ε0\Rightarrow E = \dfrac{\sigma }{{2{\varepsilon _0}}} + \dfrac{{ - \sigma }}{{2{\varepsilon _0}}}
E=0\therefore E = 0
So there is no electric field on the right side of both sheets.Comparing with the given value of EE in question we get, K=0K = 0.

Note: It should be remembered that gauss law is only applicable for closed surfaces enclosing some net charge. Also the qnet{q_{net}} on right hand side of gauss law implies the total charge enclosed by surface whereas the term EE in left hand side of gauss law implies electric field and it is due to all charges on interior, exterior or on the closed surface.