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Question: A cube is arranged such that its length, breadth, height are along X, Y and Z directions. One of its...

A cube is arranged such that its length, breadth, height are along X, Y and Z directions. One of its corners is situated at the origin. Length of each side of the cube is 25cm. The components of electric field are Ex=4002NC1{{E}_{x}}=400\sqrt{2}N{{C}^{-1}}, Ey=0{{E}_{y}}=0 and Ez=0{{E}_{z}}=0 respectively. Then what will be the flux coming out of the cube at one end, whose plane is perpendicular to X axis?
A. 252 Nm2C-1\text{A}\text{. 25}\sqrt{2}\text{ N}{{\text{m}}^{\text{2}}}{{\text{C}}^{\text{-1}}}
B. 52 Nm2C-1\text{B}\text{. 5}\sqrt{2}\text{ N}{{\text{m}}^{\text{2}}}{{\text{C}}^{\text{-1}}}
C. 2502 Nm2C-1\text{C}\text{. 250}\sqrt{2}\text{ N}{{\text{m}}^{\text{2}}}{{\text{C}}^{\text{-1}}}
D. 25 Nm2C-1\text{D}\text{. 25 N}{{\text{m}}^{\text{2}}}{{\text{C}}^{\text{-1}}}

Explanation

Solution

Electric flux is a property of the electric field. Electric flux can be defined as the number of electric field lines passing perpendicular through the surface. In this question, we can calculate electric flux through the required plane by directly using the expression of electric flux.

Formula used: Electric flux ϕE=!!!!!SE.dS{{\phi }_{E}}=\mathop{{\int\\!\\!\\!\\!\\!\int}\mkern-21mu \bigcirc}\limits_S \vec{E}.d\vec{S}

Complete step by step answer:
The cube is placed as shown in the diagram below.

“Electric flux is the rate of flow of the electric field through a given area.” Electric flux through a surface SS is defined as the surface integral of dot product of electric field and surface area vector.
ϕE=!!!!!SE.dS{{\phi }_{E}}=\mathop{{\int\\!\\!\\!\\!\\!\int}\mkern-21mu \bigcirc}\limits_S \vec{E}.d\vec{S}
Where
ϕE=\phi_E= Electric flux
E=\vec{E}= Electric field vector
dS=d\vec{S}= Differential area on the closed surface S with a surface normal in outward direction
Electric Flux has SI unit Nm2C1N{{m}^{2}}{{C}^{-1}}
According to question,
E=4002 i^\vec{E}=400\sqrt{2}\text{ }\hat{i} and dS=A i^d\vec{S}=A\text{ }\hat{i} (where A=surface area of the surface)
Substituting the values in Gauss’ law, we get
ϕE=!!!!!ABCD(4002i).(0.252i){{\phi }_{E}}=\mathop{{\int\\!\\!\\!\\!\\!\int}\mkern-21mu \bigcirc}\limits_ABCD (400\sqrt{2}i).({{0.25}^{2}}i)
ϕE=252 Nm2C1{{\phi }_{E}}=25\sqrt{2}\text{ N}{{\text{m}}^{2}}{{C}^{-1}}

So, the correct answer is “Option A”.

Additional Information: If we had calculated the electric flux through EFGH surface, we would have gotten the same result but with a negative sign indicating opposite direction.

Note: It can be noted that electric flux through the surface which has its plane parallel to direction of electric field is zero because the surface area vector for the case is perpendicular to the electric field vector.
In this problem, net electric flux through the cube is zero. This is because there is no net charge inside the cube.