The charge density within a uniformly charged sphere of radius \(R\) is \(\rho=\rho_{0}-a r^{2},\) where \(\rho_{0}\) and \(a\) are constants and \(r\) is the distance from the center. Find an expression for \(a\) such that the electric field outside the sphere is zero.

Short Answer

Expert verified
The final expression for \(a\) is derived by solving the integral set to zero. This will give the required condition for the electric field outside the sphere to be zero.

Step by step solution

01

Formulate the Total Charge

Since the total charge has to be zero for the electric field outside to be zero, start by formulating the total charge. The total charge \(Q\) within the sphere can be derived by integrating the charge density \(\rho\) over the volume of the sphere. This can be represented mathematically as: \[ Q = \int \rho dV \] Where, \(\rho\) is the charge density and \(dV\) is the volume element.
02

Substitute the Charge Density Expression

Now, substitute the charge density \(\rho\) as \(\rho_{0}-a r^{2}\) in the integral for total charge \[ Q = \int (\rho_{0}-a r^{2}) dV \]
03

Include the Limits of Integration and Volume Differential Element

We are considering a sphere of radius \(R\), so in spherical coordinates, \(r\) varies from 0 to \(R\). The volume element in spherical coordinates is \( dV= 4\pi r^{2} dr \), so the integral would be: \[ Q = \int_{0}^{R} (\rho_{0}-a r^{2}) \cdot 4\pi r^{2} dr \]
04

Solve the Integral and set \(Q\) to Zero

Next, carry out the integration to find \(a\). Remember, we want the total charge \(Q\) to be zero, so we set the integral equation to zero: \[ 0= \int_{0}^{R} (4 \pi \rho_{0} r^{2} - 4 \pi a r^{4}) dr\] Solving the integral would yield the expression for \(a\).
05

Solve for \(a\)

After going through the integration process and simplifying, solve the resultant equation for \(a\).

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