The total force acting on a charged particle moving in combined electric and magnetic fields (Lorentz force) is given by:
F ⃗ = q ( E ⃗ + v ⃗ × B ⃗ ) \vec{F} = q(\vec{E} + \vec{v} \times \vec{B}) F = q ( E + v × B )
Given data:
Charge, q = 10 − 9 C q = 10^{-9} \text{ C} q = 1 0 − 9 C
Electric field, E ⃗ = 0.4 j ^ N/C \vec{E} = 0.4\hat{j} \text{ N/C} E = 0.4 j ^ N/C
Magnetic field, B ⃗ = 4 × 10 − 3 k ^ T \vec{B} = 4 \times 10^{-3}\hat{k} \text{ T} B = 4 × 1 0 − 3 k ^ T
Net force, F ⃗ = ( 4 i ^ + 2 j ^ ) × 10 − 10 N \vec{F} = (4\hat{i} + 2\hat{j}) \times 10^{-10} \text{ N} F = ( 4 i ^ + 2 j ^ ) × 1 0 − 10 N
Since the particle is moving in the x - y x\text{-}y x - y plane, its velocity vector can be represented as:
v ⃗ = v x i ^ + v y j ^ \vec{v} = v_x \hat{i} + v_y \hat{j} v = v x i ^ + v y j ^
First, compute the magnetic force term per unit charge:
v ⃗ × B ⃗ = ( v x i ^ + v y j ^ ) × ( 4 × 10 − 3 k ^ ) \vec{v} \times \vec{B} = (v_x \hat{i} + v_y \hat{j}) \times (4 \times 10^{-3}\hat{k}) v × B = ( v x i ^ + v y j ^ ) × ( 4 × 1 0 − 3 k ^ )
Using the cross product relations i ^ × k ^ = − j ^ \hat{i} \times \hat{k} = -\hat{j} i ^ × k ^ = − j ^ and j ^ × k ^ = i ^ \hat{j} \times \hat{k} = \hat{i} j ^ × k ^ = i ^ :
v ⃗ × B ⃗ = 4 × 10 − 3 v y i ^ − 4 × 10 − 3 v x j ^ \vec{v} \times \vec{B} = 4 \times 10^{-3} v_y \hat{i} - 4 \times 10^{-3} v_x \hat{j} v × B = 4 × 1 0 − 3 v y i ^ − 4 × 1 0 − 3 v x j ^
Now, substitute E ⃗ \vec{E} E and v ⃗ × B ⃗ \vec{v} \times \vec{B} v × B into the Lorentz force equation:
F ⃗ q = E ⃗ + v ⃗ × B ⃗ \frac{\vec{F}}{q} = \vec{E} + \vec{v} \times \vec{B} q F = E + v × B
Substitute the given values:
( 4 i ^ + 2 j ^ ) × 10 − 10 10 − 9 = 0.4 j ^ + ( 4 × 10 − 3 v y i ^ − 4 × 10 − 3 v x j ^ ) \frac{(4\hat{i} + 2\hat{j}) \times 10^{-10}}{10^{-9}} = 0.4\hat{j} + \left(4 \times 10^{-3} v_y \hat{i} - 4 \times 10^{-3} v_x \hat{j}\right) 1 0 − 9 ( 4 i ^ + 2 j ^ ) × 1 0 − 10 = 0.4 j ^ + ( 4 × 1 0 − 3 v y i ^ − 4 × 1 0 − 3 v x j ^ )
0.4 i ^ + 0.2 j ^ = ( 4 × 10 − 3 v y ) i ^ + ( 0.4 − 4 × 10 − 3 v x ) j ^ 0.4\hat{i} + 0.2\hat{j} = \left(4 \times 10^{-3} v_y\right)\hat{i} + \left(0.4 - 4 \times 10^{-3} v_x\right)\hat{j} 0.4 i ^ + 0.2 j ^ = ( 4 × 1 0 − 3 v y ) i ^ + ( 0.4 − 4 × 1 0 − 3 v x ) j ^
Equating the i ^ \hat{i} i ^ and j ^ \hat{j} j ^ components on both sides:
For the i ^ \hat{i} i ^ -component:
4 × 10 − 3 v y = 0.4 4 \times 10^{-3} v_y = 0.4 4 × 1 0 − 3 v y = 0.4
v y = 0.4 4 × 10 − 3 = 100 m/s v_y = \frac{0.4}{4 \times 10^{-3}} = 100 \text{ m/s} v y = 4 × 1 0 − 3 0.4 = 100 m/s
For the j ^ \hat{j} j ^ -component:
0.4 − 4 × 10 − 3 v x = 0.2 0.4 - 4 \times 10^{-3} v_x = 0.2 0.4 − 4 × 1 0 − 3 v x = 0.2
4 × 10 − 3 v x = 0.2 4 \times 10^{-3} v_x = 0.2 4 × 1 0 − 3 v x = 0.2
v x = 0.2 4 × 10 − 3 = 50 m/s v_x = \frac{0.2}{4 \times 10^{-3}} = 50 \text{ m/s} v x = 4 × 1 0 − 3 0.2 = 50 m/s
Thus, the velocity of the particle at that instant is:
v ⃗ = 50 i ^ + 100 j ^ m/s \vec{v} = 50\hat{i} + 100\hat{j} \text{ m/s} v = 50 i ^ + 100 j ^ m/s
This corresponds to Option A.