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Question: Two infinite (non-conducting) planes each with uniform surface charge density +$\sigma$ are kept in ...

Two infinite (non-conducting) planes each with uniform surface charge density +σ\sigma are kept in such a way that the angle between them is 60°. The electric field in the region shown between them is given by:

A

σ2ϵ0[(32)x^+y^2]\frac{\sigma}{2\epsilon_0} \left[ (-\frac{\sqrt{3}}{2}) \hat{x} + \frac{\hat{y}}{2} \right]

B

σ2ϵ0[(1+3)y^x^2]\frac{\sigma}{2\epsilon_0} \left[ (1+\sqrt{3}) \hat{y} - \frac{\hat{x}}{2} \right]

C

σ2ϵ0[(1+3)y^+x^2]\frac{\sigma}{2\epsilon_0} \left[ (1+\sqrt{3}) \hat{y} + \frac{\hat{x}}{2} \right]

D

σϵ0[(1+32)y^+x^2]\frac{\sigma}{\epsilon_0} \left[ (1+\frac{\sqrt{3}}{2}) \hat{y} + \frac{\hat{x}}{2} \right]

Answer

σ2ϵ0[(1+3)y^+x^2]\frac{\sigma}{2\epsilon_0} \left[ (1+\sqrt{3}) \hat{y} + \frac{\hat{x}}{2} \right]

Explanation

Solution

The electric field due to an infinite non-conducting plane with a uniform surface charge density σ\sigma is given by E=σ2ϵ0E = \frac{\sigma}{2\epsilon_0}. The direction of the electric field is perpendicular to the plane and points away from the plane if the charge density is positive.

Let's denote the electric field due to the horizontal plane as E1\vec{E}_1 and the electric field due to the inclined plane as E2\vec{E}_2. Both planes have a positive surface charge density +σ+\sigma.

  1. Electric field due to the horizontal plane (E1\vec{E}_1):

    The horizontal plane lies along the x-axis. The electric field due to this plane will point perpendicularly away from it, i.e., in the positive y-direction.

    E1=σ2ϵ0y^\vec{E}_1 = \frac{\sigma}{2\epsilon_0} \hat{y}
  2. Electric field due to the inclined plane (E2\vec{E}_2):

    The inclined plane makes an angle of 6060^\circ with the positive x-axis. Since the plane has a positive charge density, the electric field E2\vec{E}_2 will point perpendicularly away from the plane.

    To find the direction of E2\vec{E}_2, we need a unit vector perpendicular to the plane. If the plane's angle with the x-axis is θp=60\theta_p = 60^\circ, then the normal vector pointing "downwards" from the plane will have an angle of θp90=6090=30\theta_p - 90^\circ = 60^\circ - 90^\circ = -30^\circ with the positive x-axis.

    The unit vector in this direction is:

    n^2=cos(30)x^+sin(30)y^\hat{n}_2 = \cos(-30^\circ) \hat{x} + \sin(-30^\circ) \hat{y}

    Since cos(30)=cos(30)=32\cos(-30^\circ) = \cos(30^\circ) = \frac{\sqrt{3}}{2} and sin(30)=sin(30)=12\sin(-30^\circ) = -\sin(30^\circ) = -\frac{1}{2}:

    n^2=32x^12y^\hat{n}_2 = \frac{\sqrt{3}}{2} \hat{x} - \frac{1}{2} \hat{y}

    Therefore, the electric field due to the inclined plane is:

    E2=σ2ϵ0(32x^12y^)\vec{E}_2 = \frac{\sigma}{2\epsilon_0} \left( \frac{\sqrt{3}}{2} \hat{x} - \frac{1}{2} \hat{y} \right)
  3. Total Electric Field (E\vec{E}):

    The total electric field in the region is the vector sum of E1\vec{E}_1 and E2\vec{E}_2:

    E=E1+E2\vec{E} = \vec{E}_1 + \vec{E}_2 E=σ2ϵ0y^+σ2ϵ0(32x^12y^)\vec{E} = \frac{\sigma}{2\epsilon_0} \hat{y} + \frac{\sigma}{2\epsilon_0} \left( \frac{\sqrt{3}}{2} \hat{x} - \frac{1}{2} \hat{y} \right)

    Factor out σ2ϵ0\frac{\sigma}{2\epsilon_0}:

    E=σ2ϵ0[y^+32x^12y^]\vec{E} = \frac{\sigma}{2\epsilon_0} \left[ \hat{y} + \frac{\sqrt{3}}{2} \hat{x} - \frac{1}{2} \hat{y} \right]

    Combine the x^\hat{x} and y^\hat{y} components:

    E=σ2ϵ0[32x^+(112)y^]\vec{E} = \frac{\sigma}{2\epsilon_0} \left[ \frac{\sqrt{3}}{2} \hat{x} + \left(1 - \frac{1}{2}\right) \hat{y} \right] E=σ2ϵ0[32x^+12y^]\vec{E} = \frac{\sigma}{2\epsilon_0} \left[ \frac{\sqrt{3}}{2} \hat{x} + \frac{1}{2} \hat{y} \right]

    None of the options exactly match this result. However, let's re-examine the options carefully.

    Let's consider a possibility: what if the angle 6060^\circ was interpreted differently, for instance, if the inclined plane was making 3030^\circ with the y-axis.

    Let's assume there is a typo in the question and the inclined plane makes an angle of 3030^\circ with the y-axis, or 6060^\circ with the y-axis.

    Let's re-verify the problem statement and image. The image is clear. The angle is 6060^\circ between the positive x-axis and the inclined plane.

    The calculated result is E=σ2ϵ0[32x^+12y^]\vec{E} = \frac{\sigma}{2\epsilon_0} \left[ \frac{\sqrt{3}}{2} \hat{x} + \frac{1}{2} \hat{y} \right].

    Given the choices, it's possible that the diagram implies the angle 6060^\circ is made by the inclined plane with the y-axis.

    If the inclined plane makes 6060^\circ with the y-axis, then it makes 3030^\circ with the x-axis.

    Let's assume the given answer is option (3) and try to work backward to see if any interpretation makes sense. Option (3): σ2ϵ0[(1+3)y^+x^2]\frac{\sigma}{2\epsilon_0} \left[ (1+\sqrt{3}) \hat{y} + \frac{\hat{x}}{2} \right].

    Given that this is a multiple choice question and one option is expected to be correct, there might be a non-standard interpretation.