A charge $$Q$$ is placed at each of the opposite corners of a square. A charge $$q$$ is placed at each of the other two corners. If the net electrical force on $$Q$$ is zero, then $$\frac{Q}{q}$$ equals:
A.
$$-1$$
B.
$$1$$
C.
$$ - \frac{1}{{\sqrt 2 }}$$
D.
$$ - 2\sqrt 2 $$
Answer :
$$ - 2\sqrt 2 $$
Solution :
Let $$F$$ be the force between $$Q$$ and $$Q.$$ The force between $$q$$ and $$Q$$ should be attractive for net force on $$Q$$ to be zero. Let $$F'$$ be the force between $$Q$$ and $$q.$$ For equilibrium $$\sqrt 2 F' = - F$$
$$\eqalign{
& \sqrt 2 \times k\frac{{Qq}}{{{\ell ^2}}} = - k\frac{{{Q^2}}}{{{{\left( {\sqrt 2 \ell } \right)}^2}}} \cr
& \Rightarrow \frac{Q}{q} = - 2\sqrt 2 \cr} $$
Releted MCQ Question on Electrostatics and Magnetism >> Electric Charges
Releted Question 1
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Six charges of equal magnitude, 3 positive and 3 negative are to be placed on $$PQRSTU$$ corners of a regular hexagon, such that field at the centre is double that of what it would have been if only one $$+ve$$ charge is placed at $$R.$$ Which of the following arrangement of charge is possible for $$P,Q,R,S,T$$ and $$U$$ respectively.
A long, hollow conducting cylinder is kept coaxially inside another long, hollow conducting cylinder of larger radius. Both the cylinders are initially electrically neutral.
A.
A potential difference appears between the two cylinders when a charge density is given to the inner cylinder.
B.
A potential difference appears between the two cylinders when a charge density is given to the outer cylinder.
C.
No potential difference appears between the two cylinders when a uniform line charge is kept along the axis of the cylinders.
D.
No potential difference appears between the two cylinders when same charge density is given to both the cylinders.