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Physics 16 Online
OpenStudy (mani_jha):

Is there any way to calculate the total charge of the earth?(Theoretically or experimentally) I know the capacitance of the earth, but have no idea what to do with it.

OpenStudy (experimentx):

perhaps my measuring the force on charged object at space.

OpenStudy (mani_jha):

That's a nice idea. I see values of charge of the earth on the net, but I wonder how they have got that!

OpenStudy (experimentx):

Gauss law .. perhaps.

OpenStudy (shane_b):

http://www.rheintech.com/blog/archives/1025

OpenStudy (unklerhaukus):

i know the sun has quite a charge ,

OpenStudy (anonymous):

If we assume that the electric field at the surface of Earth is E, according to Gauss law we have:\[\epsilon _{0} \int\limits E.dA=q \rightarrow \epsilon _{0}(E.dA)=dq=\sigma dA\]after simplification we have:\[\sigma=\epsilon_{0}E\]the whole charge is:\[Q=\sigma(4\pi R_{E}^2)=4\pi \epsilon_{0}ER_{E}^2\] we know that at a fine day E is about 150 N/C. now we can calculate the total charge: \[Q=(4)(3.141)(8.854 \times 10^{-12})(150)(6.37 \times 10^6)^2=6.77 \times 10^5 C \approx 6.8 \times 10^5 C\]

OpenStudy (anonymous):

Oh my God! how stupid I am! there is a very simple way too: "the magnitude of the electric field outside a uniformly charged sphere is the same as if all the charge were concentrated at the center." so we have:\[E=Q/4\pi \epsilon_{0} R_{E}^2 \rightarrow Q=4\pi \epsilon_{0}E R_{E}^2\]

OpenStudy (anonymous):

because they are different values declared for electric field at the surface of earth we may find different numbers for Q. but they are similar enough to make a good approximation. the values are between 100 and 150 N/C. so the amount of charge might be between 680KC and 450KC. hence, the best answer we could define is about:\[5.6 \pm 1.1 \times 10^5C\]

OpenStudy (mani_jha):

@ParsaN, I think you have considered the earth to be a hollow sphere. But it is a solid sphere in fact. So surface charge density should be replaced by volume density.

OpenStudy (anonymous):

the Earth is firmly conductor, hence the charge spreads on its surface.

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