Calculating total charge when the electric field is given

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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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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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