To find the point on the equatorial line where the force on a test charge \( q_0 \) is maximum, consider the setup with two equal positive point charges \( +Q \) separated by a distance \( 2a \). The equatorial line is perpendicular to the line joining the charges and passes through their midpoint.
The force \( F \) on a test charge \( q_0 \) at a distance \( y \) from the midpoint along the equatorial line due to one charge \( +Q \) is given by \( F = \frac{kQq_0}{r^2} \), where \( k \) is Coulomb's constant and \( r \) is the distance from the charge to the point \( y \). By geometry, \( r = \sqrt{a^2 + y^2} \).
The net force \( F_{\text{net}} \) due to both charges is along the y-axis, as the x-components cancel out. Thus, it's given by \( F_{\text{net}} = 2F \cos\theta \), where \( \cos\theta = \frac{a}{\sqrt{a^2+y^2}} \). Thus:
\( F_{\text{net}} = 2 \left(\frac{kQq_0}{a^2+y^2}\right) \left(\frac{a}{\sqrt{a^2+y^2}}\right) = \frac{2kQq_0a}{(a^2+y^2)^{3/2}} \)
To maximize \( F_{\text{net}} \), differentiate w.r.t. \( y \) and set the derivative to zero:
\(\frac{d}{dy}\left(\frac{2kQq_0a}{(a^2+y^2)^{3/2}}\right) = 0\)
After simplification, we find \( y = \frac{a}{\sqrt{2}} \).
So, the value of \( x \) such that \( \frac{a}{\sqrt{x}} = \frac{a}{\sqrt{2}} \) is \( x = 2 \). This value fits within the given range (2,2).

A person moved from A to B on a circular path as shown in figure If the distance travelled by him is 60 m, then the magnitude of displacement would be Given ( Cos 135° = -0.7)