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Question: A charged particle q is shot towards another charged particle \( Q \) which is fixed, with a speed \...

A charged particle q is shot towards another charged particle QQ which is fixed, with a speed vv . It approaches QQ upto a closest distance of rr and then returns. If qq was given a speed 2v2v , find the closest distance of approach.

(A) rr
(B) 2r2r
(C) r/2r/2
(D) r/4r/4

Explanation

Solution

Hint : We need to use the law of conservation of energy to solve this problem. We need to equate the total initial and final energy of the system and then by substituting the values of the initial and final potential energy, we will be able to calculate the distance of closest approach.

Formula Used: The following formulae are used to solve this question, (P.E.+K.E.)initial=(P.E.+K.E.)final{\left( {P.E. + K.E.} \right)_{initial}} = {\left( {P.E. + K.E.} \right)_{final}} where K.E.K.E. and P.E.P.E. are the kinetic energy and potential energy of a body respectively.
K.E.=12mv2\Rightarrow K.E. = \dfrac{1}{2}m{v^2} where mm is the mass and vv is the velocity of a body.
P.E.=14πε0Qqr\Rightarrow P.E. = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{r} where QQ and qq are two charges and rr is the closest distance of approach.

Complete step by step answer
Kinetic energy is the energy an object possesses because of its motion. This energy is dependent on the velocity of the object squared.
K.E.=12mv2\Rightarrow K.E. = \dfrac{1}{2}m{v^2} where mm is the mass and vv is the velocity of a body.
Potential energy is energy stored as the result of its position. The electric potential energy of any given system of charges is the work done by an external agent in bringing the charge from infinity to the present configuration in an electric field.
According to the law of conservation of energy, energy is neither created nor destroyed. It is only transformed from state to another.
Thus for the given system, it can be written that,
(P.E.+K.E.)initial=(P.E.+K.E.)final\Rightarrow {\left( {P.E. + K.E.} \right)_{initial}} = {\left( {P.E. + K.E.} \right)_{final}} where K.E.K.E. and P.E.P.E. are the kinetic energy and potential energy of a body respectively.
The particle carrying charge qq comes to rest momentarily at rr distance from the particle carrying QQ charge. At this point all the kinetic energy of qq is transformed into potential energy.
Thus, K.E.=12mv2=P.E.K.E. = \dfrac{1}{2}m{v^2} = P.E. and
P.E.=14πε0Qqr\Rightarrow P.E. = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{r} where QQ and qq are two charges and rr is the closest distance of approach.
12mv2=14πε0Qqr\therefore \dfrac{1}{2}m{v^2} = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{r}
Therefore the distance of closest approach is given by the equation above:
12mv2=14πε0Qqr\therefore \dfrac{1}{2}m{v^2} = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{r}
r=qQ4πε02mv2\Rightarrow r = \dfrac{{qQ}}{{4\pi {\varepsilon _0}}} \cdot \dfrac{2}{{m{v^2}}}
Thus the relation between rr and vv can be derived from here.
rα1v2r\alpha \dfrac{1}{{{v^2}}} , that is, rr varies inversely with the square of velocity vv .
Hence, if v=2vv = 2v , then, the distance of closest approach r becomes
r4\dfrac{r}{4} .
\therefore The correct answer is Option D.

Note
Another method to solve this question is given as,
So far, we know that, 12mv2=14πε0Qqr\dfrac{1}{2}m{v^2} = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{r} ………………………….(1)
This is equation (1).
Let us assume RR is the closest distance of approach when charge qq possesses a velocity of 2v2v .
Thus, substituting the values of velocity and distance in the equation,
12m(2v)2=14πε0QqR\dfrac{1}{2}m{\left( {2v} \right)^2} = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{R}
4×12mv2=14πε0QqR\Rightarrow 4 \times \dfrac{1}{2}m{v^2} = \dfrac{1}{{4\pi {\varepsilon _0}}}\dfrac{{Qq}}{R} ………………………………..(2)
This is equation (2).
Thus the value of RR is found by solving equation (1) and (2) as,
14=rR\dfrac{1}{4} = \dfrac{r}{R}
R=r4\Rightarrow R = \dfrac{r}{4}
\therefore The correct answer is Option D.