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The intensity of an electric field depen...

The intensity of an electric field depends only on the co-ordinates x, y and z as follows:
`vecE=a((xhati+yhatj+zhatk))/((x^2+y^2+z^2)^(3//2))`unit.
The electrostatic energy stored between two imaginary concentric spherical shells of radii R and 2R with centre at origin is

A

`(4piepsilon_0a^2)/R`

B

`(2piepsilon_0a^2)/R`

C

`(piepsilon_0a^2)/R`

D

`(piepsilon_0a^2)/(2R)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the electrostatic energy stored between two concentric spherical shells of radii \( R \) and \( 2R \), we can follow these steps: ### Step 1: Understand the electric field The electric field is given by: \[ \vec{E} = \frac{a (x \hat{i} + y \hat{j} + z \hat{k})}{(x^2 + y^2 + z^2)^{3/2}} \] This can be expressed in terms of the position vector \( \vec{r} \): \[ \vec{E} = \frac{a \vec{r}}{|\vec{r}|^3} \] where \( |\vec{r}| = \sqrt{x^2 + y^2 + z^2} \). ### Step 2: Calculate the energy density The energy density \( u \) in an electric field is given by: \[ u = \frac{1}{2} \epsilon_0 E^2 \] Substituting the expression for \( E \): \[ E = \frac{a}{r^2} \quad \text{(since } |\vec{r}| = r\text{)} \] Thus, \[ E^2 = \left(\frac{a}{r^2}\right)^2 = \frac{a^2}{r^4} \] Now, substituting this into the energy density formula: \[ u = \frac{1}{2} \epsilon_0 \frac{a^2}{r^4} \] ### Step 3: Calculate the differential volume element The differential volume element \( dv \) for a spherical shell is given by: \[ dv = 4\pi r^2 dr \] ### Step 4: Write the expression for differential energy The differential energy \( du \) stored in the shell can be expressed as: \[ du = u \cdot dv = \frac{1}{2} \epsilon_0 \frac{a^2}{r^4} \cdot 4\pi r^2 dr \] This simplifies to: \[ du = 2\pi \epsilon_0 a^2 \frac{1}{r^2} dr \] ### Step 5: Integrate to find total energy To find the total energy \( U \) stored between the shells from \( r = R \) to \( r = 2R \), we integrate \( du \): \[ U = \int_{R}^{2R} du = \int_{R}^{2R} 2\pi \epsilon_0 a^2 \frac{1}{r^2} dr \] Calculating the integral: \[ U = 2\pi \epsilon_0 a^2 \left[-\frac{1}{r}\right]_{R}^{2R} = 2\pi \epsilon_0 a^2 \left(-\frac{1}{2R} + \frac{1}{R}\right) \] This simplifies to: \[ U = 2\pi \epsilon_0 a^2 \left(\frac{1}{R} - \frac{1}{2R}\right) = 2\pi \epsilon_0 a^2 \left(\frac{1}{2R}\right) = \frac{\pi \epsilon_0 a^2}{R} \] ### Final Result Thus, the total electrostatic energy stored between the two spherical shells is: \[ U = \frac{\pi \epsilon_0 a^2}{R} \] ---
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