Electric field at a point inside a non-uniformly charged sphere

In summary, the electric field at a point inside a non-uniformly charged sphere can be determined using Gauss's law and the principles of electrostatics. Unlike a uniformly charged sphere, where the electric field inside is zero, a non-uniform charge distribution results in a varying electric field dependent on the specific charge distribution. To calculate the electric field at a given point, one must consider the contributions from all charged elements within the sphere, often requiring integration over the volume of the sphere. The resulting electric field will vary with position and reflect the complexity of the charge distribution.
  • #1
Necrolunatic
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Homework Statement
What is electric field at distance $r$ from the center of a sphere of radius $R$ with the charge density $$\rho = \rho_0(R^2 - r^2)$$ where $$\rho_0$$ is a constant and $$r < R$$
Relevant Equations
$$\rho = \rho_0(R^2 - r^2)$$
$$q = \varepsilon_0 \int E.dA$$
My solution is this:
$$q = \varepsilon_0 \int E.dA$$
Based on gauss's law.

Taking the derivative of both sides with respect to $$A$$ we get:
$$\frac{dq}{dA} = \varepsilon_0 E$$
From chain rule:
$$\frac{dq}{dA} = \frac{\frac{dq}{dr}}{\frac{dA}{dr}}$$

On the other hand:
$$q = \int \rho dv = \int \rho \frac{dv}{dr} dr = \int \rho 4 \pi r^2 dr$$
Then the derivative of $$q$$ with respect to $$r$$ is $$\frac{dq}{dr} = \rho 4 \pi r^2$$

And $$A$$ equals $$4 \pi r^2$$, therefor $$\frac{dA}{dr} = 8 \pi r$$
Then we get:
$$\varepsilon_0 E = \frac{dq}{dA} = \frac{\rho 4 \pi r^2}{8 \pi r} = \frac{\rho}{2} r$$

So the electric field at a point within the sphere with distance $$r$$ from the center is
$$E = \frac{\rho}{2 \varepsilon_0} r$$

I don't have the answer to the question but this doesn't seem correct, because in a uniformly charged sphere where $$\rho$$ is $$\frac{Q}{\frac{4}{3} \pi R^3}$$, replacing that into the formula I geta
$$\frac{3 Q}{8 \pi \varepsilon_0 R^3} r$$ which is $$\frac{3}{2}$$ times the actual value $$\frac{Q}{4 \pi \varepsilon_0 R^3} r$$. What am I doing wrong?
 
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  • #2
Understand Gauss’s law first. Then integrate instead of taking derivatives.
 
  • #3
Necrolunatic said:
Taking the derivative of both sides with respect to $$A$$ we get:
$$\frac{dq}{dA} = \varepsilon_0 E$$
This is incorrect. You are effectively differentiating wrt the radius here based on what you do later, but the electric field also depends on the radius so you are missing derivatives.

Much easier is to just note that the rhs is ##\varepsilon_0 EA## and divide both sides by ##\varepsilon_0 A##.
 
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  • #4
Orodruin said:
Much easier is to just note that the rhs is ##\varepsilon_0 EA## and divide both sides by ##\varepsilon_0 A##.
Wouldn't one have to integrate the lhs to get ##q## before dividing by ##\varepsilon_0 A##?
 
  • #5
kuruman said:
Wouldn't one have to integrate the lhs to get ##q## before dividing by ##\varepsilon_0 A##?
Obviously you still have to do the integral to get ##q##.
 
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  • #6
Orodruin said:
Obviously you still have to do the integral to get ##q##.
Judging from OP's initial approach to differentiate both sides, I wanted to make sure that it's also obvious to OP.
 
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  • #7
Of course, this is integral (🤭) to understanding Gauss’ law.
 
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FAQ: Electric field at a point inside a non-uniformly charged sphere

What is an electric field?

An electric field is a region around a charged particle where other charged particles experience a force. It is represented by the electric field vector, which indicates the direction and strength of the force that a positive test charge would experience in that field.

How is the electric field calculated inside a non-uniformly charged sphere?

The electric field inside a non-uniformly charged sphere can be calculated using Gauss's Law, which relates the electric field to the charge enclosed by a Gaussian surface. The specific distribution of charge must be known to integrate the electric field contributions from each infinitesimal charge element within the sphere.

Does the electric field inside a non-uniformly charged sphere vary with distance from the center?

Yes, the electric field inside a non-uniformly charged sphere generally varies with distance from the center, depending on the charge distribution. Unlike a uniformly charged sphere, where the electric field inside is constant and zero at the center, a non-uniform distribution leads to a gradient in the electric field strength.

What role does charge density play in determining the electric field inside the sphere?

Charge density is critical in determining the electric field inside a non-uniformly charged sphere. The electric field at any point is influenced by the local charge density and the geometry of the charge distribution. Higher charge density in a region will result in a stronger electric field in that area.

Can the electric field inside a non-uniformly charged sphere be zero?

Yes, it is possible for the electric field inside a non-uniformly charged sphere to be zero at certain points, depending on the specific charge distribution. For example, if the charge density is arranged symmetrically in such a way that the contributions from different regions cancel out, the net electric field at that point could be zero.

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