1 × 10−6C
2 × 10−5C
To determine the charge on the copper ball required for it to remain suspended in the oil, we require the net force on the ball to be zero. The forces acting on the copper ball are:
where:
The volume \(V\) of the sphere is calculated as:
\(V = \frac{4}{3}\pi r^3\) with \(r = 0.5 \, \text{cm} = 0.005 \, \text{m}\).
Therefore,
\(V = \frac{4}{3}\pi (0.005)^3 = \frac{4}{3}\pi \times 1.25 \times 10^{-7} = \frac{5\pi}{3} \times 10^{-7} \, \text{m}^3\).
For the ball to be suspended, the total upward force must equal the downward force:
\((F_b + F_e) = F_g\).
Substituting the force expressions yields:
\(V \cdot \rho_o \cdot g + qE = V \cdot \rho_c \cdot g\).
Rearranging the equation to solve for \(q\):
\(q = \frac{V(\rho_c - \rho_o)g}{E}\).
Using the provided values:
The charge \(q\) is calculated as:
\(q = \frac{\left(\frac{5\pi}{3} \times 10^{-7}\right)(8000 - 800) \cdot 10}{600\pi} = \frac{\frac{5\pi}{3} \times 10^{-7} \cdot 7200 \cdot 10}{600\pi}\).
This simplifies to:
\(q = \frac{5 \times 7200 \times 10^{-7} \cdot 10}{3 \times 600} = \frac{5 \times 7200 \times 10^{-6}}{1800}\).
\(= \frac{5 \times 4}{10} \times 10^{-6} = 2 \times 10^{-5} \, \text{C}\).
The required charge on the copper ball is \(2 \times 10^{-5} \text{C}\).
A point charge \(q = 1\,\mu\text{C}\) is located at a distance \(2\,\text{cm}\) from one end of a thin insulating wire of length \(10\,\text{cm}\) having a charge \(Q = 24\,\mu\text{C}\), distributed uniformly along its length, as shown in the figure. Force between \(q\) and wire is ________ N. 