Sphere of inner radius a and outer radius b is made of `p` uniform resistivity find resistance between inner and outer surface
Sphere of inner radius a and outer radius b is made of `p` uniform resistivity find resistance between inner and outer surface
A
`(rho)/(4pi)((1)/(a)-(1)/(b))`
B
`(rho)/(2pi)((1)/(a)-(1)/(b))`
C
`(rho)/(2pi)((1)/(a)+(1)/(a)+(1)/(b))`
D
`(rho)/(4pi)((1)/(a)+(1)/(b))`
Text Solution
AI Generated Solution
The correct Answer is:
To find the resistance between the inner and outer surfaces of a spherical shell with inner radius \( a \) and outer radius \( b \), made of a material with uniform resistivity \( \rho \), we can follow these steps:
### Step-by-Step Solution:
1. **Understand the Concept of Resistance**:
The resistance \( R \) of a conductor is given by the formula:
\[
R = \frac{\rho l}{A}
\]
where \( \rho \) is the resistivity, \( l \) is the length (or thickness) through which current flows, and \( A \) is the cross-sectional area.
2. **Consider a Thin Spherical Shell**:
To find the total resistance between the inner and outer surfaces, we consider a thin spherical shell of radius \( r \) and thickness \( dr \). The resistance of this thin shell can be expressed as:
\[
dR = \frac{\rho \, dr}{A}
\]
where \( A \) is the surface area of the thin shell.
3. **Calculate the Surface Area**:
The surface area \( A \) of a sphere of radius \( r \) is given by:
\[
A = 4\pi r^2
\]
Therefore, we can substitute this into our expression for \( dR \):
\[
dR = \frac{\rho \, dr}{4\pi r^2}
\]
4. **Integrate to Find Total Resistance**:
To find the total resistance \( R \) from the inner radius \( a \) to the outer radius \( b \), we need to integrate \( dR \) from \( r = a \) to \( r = b \):
\[
R = \int_{a}^{b} dR = \int_{a}^{b} \frac{\rho \, dr}{4\pi r^2}
\]
5. **Perform the Integration**:
The integral can be solved as follows:
\[
R = \frac{\rho}{4\pi} \int_{a}^{b} \frac{dr}{r^2}
\]
The integral of \( \frac{1}{r^2} \) is:
\[
-\frac{1}{r}
\]
Thus, we have:
\[
R = \frac{\rho}{4\pi} \left[-\frac{1}{r}\right]_{a}^{b} = \frac{\rho}{4\pi} \left(-\frac{1}{b} + \frac{1}{a}\right)
\]
6. **Simplify the Result**:
This simplifies to:
\[
R = \frac{\rho}{4\pi} \left(\frac{1}{a} - \frac{1}{b}\right)
\]
### Final Result:
The resistance between the inner and outer surfaces of the spherical shell is:
\[
R = \frac{\rho}{4\pi} \left(\frac{1}{a} - \frac{1}{b}\right)
\]
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