Electric Field and Gaussian Pillbox

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stunner5000pt
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check whether this result of this problem is consistent with this statement
[tex]\vec{E_{above}} - \vec{E_{below}} = \frac{\sigma}{\epsilon_{0}} \hat{n}[/tex]


an infinite plan carries a uniform surface charge sigma. Find its electric field
Solution:

Draw a Gaussian Pillbox extending above and below the plane. Then
since [tex]\oint \vec{E} \bullet d\vec{a} = \frac{Q_{enc}}{\epsilon_{0}}[/tex]

and since[tex]Q_{enc} = \sigma A[/tex]

By Symmetry E points up and down

so
[tex]\int \vec{E} \bullet d\vec{a} = 2A |\vec{E}|[/tex]

so [tex]\vec{E} = \frac{\sigma}{2\epsilon_{0}} \hat{n}[/tex]

Now to tackle the question

Well for an infinite sheet for each side the Electric field points normal to the sheet, right?
SO the electric field for the top is [itex]\vec{E} = \frac{\sigma}{\epsilon_{0}} \hat{n}[/itex]
and te bottom is the negative of that

So when you add those two together you get [tex]\vec{E} = \frac{\sigma}{\epsilon_{0}} \hat{n}[/tex]

and this is consistent with statement. Easy enough. i just want to know whether this kind of 'proof' for the statement is satisfactory.
 
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