- #1
spaghetti3451
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I am looking to use Gauss's law to find the electric field in ##1+1## dimensional spacetime:
##\int \vec{E}\cdot d\vec{A}=\frac{Q}{\epsilon_{0}}##
Now, for a point charge in ##1+1## dimensional spacetime, the Gaussian surface is the two endpoints (a distance ##r## away from the point charge) along which the electric field points outwards. How do I account for ##d\vec{A}## of the two endpoints?
##\int \vec{E}\cdot d\vec{A}=\frac{Q}{\epsilon_{0}}##
Now, for a point charge in ##1+1## dimensional spacetime, the Gaussian surface is the two endpoints (a distance ##r## away from the point charge) along which the electric field points outwards. How do I account for ##d\vec{A}## of the two endpoints?