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: \( 8.0 \times 10^{-19} \, \text{C} \).
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.