Calculating total charge when the electric field is given

AI Thread Summary
The discussion revolves around calculating total charge using Gauss' law, where two different methods yield conflicting results. The first method, using the equation E.A = q/ε0, suggests that the enclosed charge approaches zero as r approaches infinity. The second method, using the divergence of the electric field, neglects the contribution from a point charge at the origin, leading to a different total charge calculation. It is emphasized that the divergence computation must be valid for r = 0 to account for the delta function at the origin, indicating a point charge exists there. Ultimately, checking the flux through a sphere as r approaches zero confirms the presence of this charge.
Saptarshi Sarkar
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Homework Statement
Calculate the total charge of an unknown charge distribution for which the electric field is E=q/r^2 e^(-4r) r ̂
Relevant Equations
E.A = q/ε0
∇·E = ρ/ε0
I first tried to use the Gauss' law equation E.A = q/ε0 to find the total charge enclosed. The answer came out to be q(enclosed) = 4πqε0e^(-4r). So for r approaching infinity, q(enclosed) approached 0.

Next, I tried the equation ∇·E = ρ/ε0, calculated rho to be -4qε0e^(-4r)/r^2 and total charge to be -4πqε0.

Why are the answers different although both are derived from Gauss' law? What did I do wrong?
 

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Your computation for the divergence of the electric field is only valid for ##r > 0##. This means that you will miss the contribution from the point charge at the origin.
 
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Another thing you might think about is how the given electric field behaves as ##r## gets really big. Compare this to what the field of any point charge, ##q_o##, behaves for large ##r##. What does ##q_o## have to equal so that these distant fields are the same.
 
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Paul Colby said:
Another thing you might think about is how the given electric field behaves as ##r## gets really big. Compare this to what the field of any point charge, ##q_o##, behaves for large ##r##. What does ##q_o## have to equal so that these distant fields are the same.

For both the cases, the electric field approaches 0 as r approaches large numbers. Only conclusion I can draw from this is that the given electric field falls to 0 faster due to the exponential term.
 
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Orodruin said:
Your computation for the divergence of the electric field is only valid for ##r > 0##. This means that you will miss the contribution from the point charge at the origin.

I am not sure I am able to understand. How do I know that there is a charge at the centre and how should I calculate it?
 
If you compute the divergence with a method valid at ##r = 0##, you will find that, apart from your result, there is a delta function at the origin.

Alternatively, you can check this by taking the flux through a sphere with ##r \to 0##, which will yield a non-zero result, indicating that there is a point charge at the origin.
 
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Yes.
 
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