Consider the magnitude of electric field E at a point at distance r due to an infinitely long straight wire charged with a uniform charge density λ. Then for a given λ.

1
E ∝ r
2
\(\rm E \propto \frac{1}{r}\)
3
\(\rm E \propto \frac{1}{r^2}\)
4
\(\rm E \propto \frac{1}{r^3}\)

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