Two isolated metallic solid spheres of radii $R$ and $2 R$ are charged such that both have same charge density $\sigma$. The spheres are then connected by a thin conducting wire. If the new charge density of the bigger sphere is $\sigma^{\prime}$ The ratio $\frac{\sigma^{\prime}}{\sigma}$ is :
The relationship between the charges and radii is given by:
\[ \frac{1}{4 \pi \epsilon_0} \cdot \frac{Q_1'}{R} = \frac{1}{4 \pi \epsilon_0} \cdot \frac{Q_2'}{2R} \]
Simplifying, we find:
\[ Q_2' = 2Q_1' \]
Using the charge conservation equation:
\[ Q_1' + Q_2' = Q_1 + Q_2 \]
Substitute \(Q_2' = 2Q_1'\):
\[ Q_1' + 2Q_1' = 20 \pi R^2 \sigma \]
\[ 3Q_1' = 20 \pi R^2 \sigma \]
\[ Q_1' = \frac{20 \pi R^2 \sigma}{3} \]
Substitute \(Q_2' = 2Q_1'\):
\[ Q_2' = \frac{40 \pi R^2 \sigma}{3} \]
The surface charge densities are related by:
\[ \sigma' = \frac{Q_2'}{4 \pi (2R)^2} \]
\[ \sigma' = \frac{\frac{40 \pi R^2 \sigma}{3}}{16 \pi R^2} \]
\[ \sigma' = \frac{40}{3} \cdot \frac{1}{16} \cdot \sigma \]
\[ \sigma' = \frac{5}{6} \cdot \sigma \]
\(\frac{\sigma'}{\sigma} = \frac{5}{6}\)
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is:
Electric Field is the electric force experienced by a unit charge.
The electric force is calculated using the coulomb's law, whose formula is:
\(F=k\dfrac{|q_{1}q_{2}|}{r^{2}}\)
While substituting q2 as 1, electric field becomes:
\(E=k\dfrac{|q_{1}|}{r^{2}}\)
SI unit of Electric Field is V/m (Volt per meter).