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Question: Charge \(Q\), is divided into two parts which are then kept some distance apart. The force between t...

Charge QQ, is divided into two parts which are then kept some distance apart. The force between them will be maximum if the two parts are having the charge
A) Q2\dfrac{Q}{2} each
B) Q4\dfrac{Q}{4} and 3Q4\dfrac{3Q}{4}
C) Q3\dfrac{Q}{3} and 2Q3\dfrac{2Q}{3}
D) ee and (Qe)(Q-e), where e=e=electronic charge

Explanation

Solution

The force of attraction between two charged particles at a distance is given by Coulomb’s law. The force of attraction between two stationary, electrically charged particles is maximum when the first derivative of the maximum force with respect to one of the charges is equal to zero.

Complete answer:
Coulomb’s law states that the force of attraction between two stationary, electrically charged particles is equal to
F=kq1q2r2F=k\dfrac{{{q}_{1}}{{q}_{2}}}{{{r}^{2}}}
where
FF is the force of attraction
q1{{q}_{1}} and q2{{q}_{2}} are the stationary charges
rr is the distance between the charges
kk is the Coulomb’s constant
Let this be equation 1.
From the question, we are provided that a charge QQ is divided into two and the force of attraction between the divided charges is maximum. We are required to find these charges.
Let us assume one of these charges to be qq. The other charge turns out to be QqQ-q. Also, let the distance between these two charges be dd as shown in the following figure.

Applying equation 1 to these parameters, we have
F=kq1q2r2=kq(Qq)d2F=k\dfrac{{{q}_{1}}{{q}_{2}}}{{{r}^{2}}}=k\dfrac{q(Q-q)}{{{d}^{2}}}
Let this be equation 2.
Now, we are given that the force of attraction between the charges QQ and QqQ-q is maximum.
For maximum force of attraction,
dFmaxdq=0\dfrac{d{{F}_{\max }}}{dq}=0
Let this be equation 3.
Applying equation 2 in equation 3, we have
dFmaxdq=dkq(Qq)d2dq=0kd2d[q(Qq)]dq=0d[q(Qq)]dq=0\dfrac{d{{F}_{\max }}}{dq}=\dfrac{dk\dfrac{q(Q-q)}{{{d}^{2}}}}{dq}=0\Rightarrow \dfrac{k}{{{d}^{2}}}\dfrac{d\left[ q(Q-q) \right]}{dq}=0\Rightarrow \dfrac{d\left[ q(Q-q) \right]}{dq}=0
On further simplification, we have
d[q(Qq)]dq=0d(qQq2)dq=0Q2q=0q=Q2\dfrac{d\left[ q(Q-q) \right]}{dq}=0\Rightarrow \dfrac{d(qQ-{{q}^{2}})}{dq}=0\Rightarrow Q-2q=0\Rightarrow q=\dfrac{Q}{2}
Therefore, one of the charges is equal to Q2\dfrac{Q}{2}. The other charge also turns out to be
Qq=QQ2=Q2Q-q=Q-\dfrac{Q}{2}=\dfrac{Q}{2}.

So, the correct answer is “Option A”.

Note:
The force determined through Coulomb’s law follows sign convention. If the stationary charges have opposite signs, then the force turns out to be negative and the nature of the force is attractive. If the stationary charges have the same signs, then the force turns out to be positive and the nature of the force is repulsive. Here, in this question, we have only dealt with the magnitude of force.