Answer
346.8k+ views
Hint: First of all read the question carefully and understand the values or quantities given in the question. Also observe the diagram carefully. After that apply Coulomb’s law. Since the two forces are acting at right angles we must calculate the resultant force. Then equate it with the force due to Q. Thus by rearranging and substituting the values we get the value of q.
Complete step-by-step solution:
Let the side of the square be ‘a’. Then by Pythagoras theorem the diagonal of the square is $\sqrt{2}a$.
Thus the force due to the charge Q at A and C is,
$F=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{Q}^{2}}}{2{{a}^{2}}}$
And the direction of this force is outward.
Hence in order to become the net force to zero, the force ${{F}_{1}}$ on Q due to q must be equal to the force ${{F}_{2}}$ on Q due to q.
Thus,
${{F}_{1}}={{F}_{2}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Qq}{{{a}^{2}}}$
As ${{F}_{1}}$and ${{F}_{2}}$are at right angles.
${{F}_{12}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{\sqrt{2}Qq}{{{a}^{2}}}$
For the equilibrium condition of Q,
$F={{F}_{12}}$
$\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{Q}^{2}}}{2{{a}^{2}}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{\sqrt{2}Qq}{{{a}^{2}}}$
$\Rightarrow \dfrac{Q}{2}=\sqrt{2}q$
We have to find q. Hence rearranging and substituting the values we get,
$q=\dfrac{Q}{2\sqrt{2}}$
$\therefore q=\dfrac{\sqrt{2}\mu C}{2\sqrt{2}}=0.5\mu C$
Note:Remember that the resultant force is the difference in the magnitude of larger force to the smaller force. If the two forces have the same magnitude and if they are acting just in the opposite direction to one another then the resultant force is zero.
Complete step-by-step solution:
Let the side of the square be ‘a’. Then by Pythagoras theorem the diagonal of the square is $\sqrt{2}a$.
Thus the force due to the charge Q at A and C is,
$F=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{Q}^{2}}}{2{{a}^{2}}}$
And the direction of this force is outward.
Hence in order to become the net force to zero, the force ${{F}_{1}}$ on Q due to q must be equal to the force ${{F}_{2}}$ on Q due to q.
Thus,
${{F}_{1}}={{F}_{2}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{Qq}{{{a}^{2}}}$
As ${{F}_{1}}$and ${{F}_{2}}$are at right angles.
${{F}_{12}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{\sqrt{2}Qq}{{{a}^{2}}}$
For the equilibrium condition of Q,
$F={{F}_{12}}$
$\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{{{Q}^{2}}}{2{{a}^{2}}}=\dfrac{1}{4\pi {{\varepsilon }_{0}}}\dfrac{\sqrt{2}Qq}{{{a}^{2}}}$
$\Rightarrow \dfrac{Q}{2}=\sqrt{2}q$
We have to find q. Hence rearranging and substituting the values we get,
$q=\dfrac{Q}{2\sqrt{2}}$
$\therefore q=\dfrac{\sqrt{2}\mu C}{2\sqrt{2}}=0.5\mu C$
Note:Remember that the resultant force is the difference in the magnitude of larger force to the smaller force. If the two forces have the same magnitude and if they are acting just in the opposite direction to one another then the resultant force is zero.
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