Write Coulomb’s law and explain its scalar form.
The electric force between two point charges varied inversely as the square of the distance between the charges and was directly proportional to the product of the magnitude of the two charges and acted along the line joining the two charges.
Thus, if two point charges $q_{1}, q_{2}$ are separated by a distance $r$ in vacuum, the magnitude of the force (F) between them is given by,
$\mathrm{F} \propto \frac{q_{1} q_{2}}{r^{2}}$
$\therefore \mathrm{F}=k \frac{q_{1} q_{2}}{r^{2}} \quad \ldots$ $(1)$
where, $k$ is the proportionality constant also called Coulombian constant.
Experimentally it is found that $k=8.9875 \times 10^{9} \mathrm{Nm}^{2} \mathrm{C}^{-2}$. In general, it is taken as $k=9 \times$ $10^{9} \mathrm{Nm}^{2} \mathrm{C}^{-2}$.
$K=\frac{1}{4 \pi \epsilon_{0}}$
where, $\epsilon_{0}=$ permittivity in free space
$=8.854185 \times 10^{-12} \mathrm{C}^{2} \mathrm{~N}^{-1} \mathrm{~m}^{-2}$
$\approx 8.9 \times 10^{-12} \mathrm{C}^{2} \mathrm{~N}^{-1} \mathrm{~m}^{-2}$
Hence, electric force is free space,
$\mathrm{F}=\frac{1}{4 \pi \epsilon_{0}} \frac{q_{1} q_{2}}{r^{2}}$
$\ldots$ $(2)$
If the charges are at distance ' $r$ ' in any medium instead of free space, then electric force in medium,
$\mathrm{F}_{m}=\frac{1}{4 \pi \varepsilon} \frac{q_{1} q_{2}}{r^{2}}$
where, $\varepsilon=$ permittivity in medium.
Now, relative permittivity $=\epsilon_{r}=\frac{\epsilon}{\epsilon_{0}}=k=$ dielectric constant
By taking ratio of equation (3) to (2),
$\frac{\mathrm{F}_{\mathrm{m}}}{\mathrm{F}}=\frac{\epsilon_{0}}{\epsilon}=\frac{1}{k}$
$\therefore \quad \mathrm{F}_{\mathrm{m}}=\frac{\mathrm{F}}{k}$
Thus, electric force between two charges in medium is $\frac{1}{k}$ times the electric force in free space.
Electric charges of $1\,\mu C,\, - 1\,\mu C$ and $2\,\mu C$ are placed in air at the corners $A$, $B$ and $C$ respectively of an equilateral triangle $ABC$ having length of each side $10 \,cm$. The resultant force on the charge at $C$ is......$N$
A particle of mass $1 \,{mg}$ and charge $q$ is lying at the mid-point of two stationary particles kept at a distance $'2 \,{m}^{\prime}$ when each is carrying same charge $'q'.$ If the free charged particle is displaced from its equilibrium position through distance $'x'$ $(x\,< \,1\, {m})$. The particle executes $SHM.$ Its angular frequency of oscillation will be $....\,\times 10^{8}\, {rad} / {s}$ if ${q}^{2}=10\, {C}^{2}$
Four charge $Q _1, Q _2, Q _3$, and $Q _4$, of same magnitude are fixed along the $x$ axis at $x =-2 a - a ,+ a$ and $+2 a$, respectively. A positive charge $q$ is placed on the positive $y$ axis at a distance $b > 0$. Four options of the signs of these charges are given in List-$I$ . The direction of the forces on the charge q is given in List-$II$ Match List-$1$ with List-$II$ and select the correct answer using the code given below the lists.$Image$
List-$I$ | List-$II$ |
$P.$ $\quad Q _1, Q _2, Q _3, Q _4$, all positive | $1.\quad$ $+ x$ |
$Q.$ $\quad Q_1, Q_2$ positive $Q_3, Q_4$ negative | $2.\quad$ $-x$ |
$R.$ $\quad Q_1, Q_4$ positive $Q_2, Q_3$ negative | $3.\quad$ $+ y$ |
$S.$ $\quad Q_1, Q_3$ positive $Q_2, Q_4$ negative | $4.\quad$ $-y$ |
Total charge $-\,Q$ is uniformly spread along length of a ring of radius $R$. A small test charge $+q$ of mass m is kept at the centre of the ring and is given a gentle push along the axis of the ring.
$(a) $ Show that the particle executes a simple harmonic oscillation.
$(b)$ Obtain its time period.
Two particles $X $ and $Y$, of equal mass and with unequal positive charges, are free to move and are initially far away from each other. With $Y$ at rest, $X$ begins to move towards it with initial velocity $u$. After a long time, finally