If the linear charge density of an infinitely long straight uniformly charged wire is λ, then the force on the charge q present at a distance r from the wire is:

1
\(\frac{\lambda q}{2\pi \epsilon_o r}\)
2
\(\frac{\lambda^2 q}{2\pi \epsilon_o r}\)
3
\(\frac{\lambda q}{2\pi \epsilon_o r^2}\)
4
\(\frac{\lambda^2 q}{2\pi \epsilon_o r^2}\)

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