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QJEEM24Phba04: JEE Main 2024 Physics - Class 12 JEEM24Phba04 Solution: is the uniform surface charge density of a thin spherical shell …

σ\sigma is the uniform surface charge density of a thin spherical shell of radius R. The electric field at any point on the surface of the spherical shell is :

Multiple Choice Options

  • A σ/ϵoR\sigma / \epsilon_o R
  • B σ/∈o\sigma / \in_o
  • C σ/2ϵo\sigma / 2 \epsilon_o
  • D σ/4ϵo\sigma / 4 \epsilon_o

Step-by-Step Verified Solution

The question is about calculating the electric field at the surface of a thin spherical shell with a uniform surface charge density denoted by σ\sigma . To determine the electric field at any point on the surface of the shell, we can use Gauss's law, which is particularly useful for systems with high symmetry like a spherical shell.

Gauss's law in its integral form states that the electric flux through a closed surface is equal to the charge enclosed by the surface divided by the permittivity of free space ( ϵ0\epsilon_0 ), mathematically represented as:

ΦE=Qencϵ0\Phi_E = \frac{Q_{\text{enc}}}{\epsilon_0}

In the case of a spherical shell of radius RR , the total charge QencQ_{\text{enc}} on the shell can be written in terms of the surface charge density σ\sigma as:

Qenc=σ×4πR2Q_{\text{enc}} = \sigma \times 4\pi R^2

Now, we apply Gauss's law using a Gaussian surface that coincides with the surface of the spherical shell. The electric field EE at the surface of the shell is uniform over the Gaussian surface, and the area of the Gaussian surface (which is also the area of the spherical shell) is 4πR24\pi R^2 . Thus, the electric flux ΦE\Phi_E through the Gaussian surface is:

ΦE=E⋅4πR2\Phi_E = E \cdot 4\pi R^2

Using Gauss's law:

E⋅4πR2=σ⋅4πR2ϵ0E \cdot 4\pi R^2 = \frac{\sigma \cdot 4\pi R^2}{\epsilon_0}

Simplifying this equation gives us the electric field at the surface of the spherical shell:

E=σϵ0E = \frac{\sigma}{\epsilon_0}

Therefore, the correct answer is Option B:

σϵ0\frac{\sigma}{\epsilon_0}

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