A tiny spherical oil drop carrying a net charge q is balanced in still air with a vertical uniform electrical field of strength \(\frac{81}{7}\pi\) x 105 V/m.When the field is switched off, the drop is observed to fall with terminal velocity 2 x 10-3 m/s. Here g = 9.8 m/s2, viscosity of air is 1.8 x 10-5 N/m2 and the density of the oil is 900 kg/m3. The magnitude of 'q' is
1.6 x 10-19 C
0.8 x 10-19 C
3.2 x 10-19 C
8 x 10-19 C
Step 1: Equating Gravitational Force and Drag Force
The gravitational force acting on the drop is given by:
\( F_{\text{gravity}} = m \cdot g \)
The drag force due to viscosity is given by Stokes' law:
\( F_{\text{drag}} = 6 \pi \eta r v \)
At terminal velocity, these two forces are balanced:
\( m \cdot g = 6 \pi \eta r v \)
Step 2: Solving for Mass
Rearranging the equation for \( m \):
\( m = \frac{6 \pi \eta r v}{g} \)
The mass of the drop can also be expressed in terms of its volume and density:
\( m = \frac{4}{3} \pi r^3 \rho \)
Substitute this expression for \( m \) into the equation:
\( \frac{4}{3} \pi r^3 \rho \cdot g = 6 \pi \eta r v \)
Step 3: Solving for the Radius \( r \)
Rearrange the equation to solve for \( r^2 \):
\( r^2 = \frac{9 \eta v}{2 \rho g} \)
Step 4: Substituting the Given Values
Given values:
Substitute these values into the equation:
\( r^2 = \frac{9 \times 1.8 \times 10^{-5} \times 2 \times 10^{-3}}{2 \times 900 \times 9.8} \)
Simplifying:
\( r^2 = \frac{9 \times 10^{-8}}{17640} \approx 5.10 \times 10^{-13} \)
Taking the square root of both sides:
\( r \approx 7.14 \times 10^{-7} \, \text{m} \)
Step 5: Finding the Charge \( q \)
The electric force acting on the oil drop is given by:
\( F_{\text{electric}} = q \cdot E \)
The electric field strength is given as:
\( E = \frac{81 \pi}{7 \times 10^3} \, \text{V/m} \)
The gravitational force can also be expressed as:
\( F_{\text{electric}} = \frac{4}{3} \pi r^3 \rho \cdot g \)
Equating the two expressions for the electric force:
\( q \cdot E = \frac{4}{3} \pi r^3 \rho \cdot g \)
Solving for \( q \):
\( q = \frac{\frac{4}{3} \pi r^3 \rho g}{E} \)
Substitute the known values:
\( q = \frac{\frac{4}{3} \pi \cdot (7.14 \times 10^{-7})^3 \cdot 900 \cdot 9.8}{\frac{81 \pi}{7 \times 10^3}} \)
Simplifying:
\( q \approx 8 \times 10^{-19} \, \text{C} \)
Therefore, the magnitude of the charge \( q \) is: \( 8 \times 10^{-19} \, \text{C} \) (option D).
Given the following equations:
\( qE = mg \quad \text{...(i)} \)
\( 6 \pi \eta r v = mg \)
Also, we have:
\( \frac{3}{4} \pi r^3 \rho g = mg \quad \text{...(ii)} \)
Solving for \( r \), we get:
\( r = \left( \frac{4 \pi \rho g}{3 mg} \right)^{1/3} \quad \text{...(iii)} \)
Substituting the value of \( r \) in Equation (ii), we get:
\( 6 \pi \eta v \left( \frac{4 \pi \rho g}{3 mg} \right)^{1/3} = mg \)
Now, simplifying this expression:
\( (6 \pi \eta v)^3 \left( \frac{4 \pi \rho g}{3 mg} \right) = (mg)^3 \)
Again, substituting \( mg = qE \), we get:
\( (qE)^2 = \left( \frac{4 \pi \rho g}{3} \right) \cdot (6 \pi \eta v)^3 \)
Thus, solving for \( qE \), we get:
\( qE = \left( \frac{4 \pi \rho g}{3} \right)^{1/2} \cdot (6 \pi \eta v)^{3/2} \)
Finally, we find \( q \) as:
\( q = E \left( \frac{4 \pi \rho g}{3} \right)^{1/2} \cdot (6 \pi \eta v)^{3/2} \)
Substituting the values:
\( q = \frac{81 \pi \times 10^5}{\sqrt{4 \pi \times 900 \times 9.8}} \times 3 \times 216 \pi \times (1.8 \times 10^{-5} \times 2 \times 10^{-3})^3 \)
Therefore, the value of \( q \) is: \( 8.0 \times 10^{-19} \, \text{C} \).
Two charges, \( q_1 = +3 \, \mu C \) and \( q_2 = -4 \, \mu C \), are placed 20 cm apart. Calculate the force between the charges.
The electrostatic potential is also known as the electric field potential, electric potential, or potential drop is defined as “The amount of work that is done in order to move a unit charge from a reference point to a specific point inside the field without producing an acceleration.”
SI unit of electrostatic potential - volt
Other units - statvolt
Symbol of electrostatic potential - V or φ
Dimensional formula - ML2T3I-1
The electric potential energy of the system is given by the following formula:
U = 1/(4πεº) × [q1q2/d]
Where q1 and q2 are the two charges that are separated by the distance d.