The charge per unit length on a long, straight filament is -91.9 µC/m.
(a) Find the electric field 10.0 cm from the filament, where distances are measured perpendicular to the length of the filament. (Take radially inward toward the filament as the positive direction.) MN/C
(b) Find the electric field 50.0 cm from the filament, where distances are measured perpendicular to the length of the filament. MN/C
(c) Find the electric field 150 cm from the filament, where distances are measured perpendicular to the length of the filament.
$λ_q=\frac{dq}{dl}→dq=λ_qdl$
$\vec{E} =k_e\frac{q}{r^2}\hat{r}$
$||\vec{E}||=\frac{λ_qdl}{r^2}$ How can I solve this without knowing the length of the filament? Supposedly this is the suggested way of solving this problem--and I'd like to understand this method very much. Could someone help me?
Also, in addition to solving it by this expedient, is it possible to solve this problem by employing a Gaussian surface?