40 m/s
40\(\sqrt{2}\) m/s
50 m/s
50\(\sqrt{3}\) m/s
100\(\sqrt{2}\)m/s
Given parameters:
Lorentz force equation: \[ \vec{F} = q(\vec{v} \times \vec{B}) \]
Velocity components: \[ (4\hat{i} - 3\hat{j}) \times 10^{-12} = 10^{-9}(\vec{v} \times 10^{-4}\hat{k}) \] \[ \vec{v} \times \hat{k} = (4\hat{i} - 3\hat{j}) \times 10 \]
Solve for velocity: \[ \vec{v} = 40\hat{j} + 30\hat{i} \] \[ |\vec{v}| = \sqrt{30^2 + 40^2} = 50 \, \text{m/s} \]
Thus, the correct option is (C): 50 m/s.
1. Recall the magnetic force equation:
The magnetic force (F) on a charged particle moving in a magnetic field (B) is given by:
\[\vec{F} = q(\vec{v} \times \vec{B})\]
where:
2. Define the given information:
\[\vec{B} = 10^{-4}\hat{k} \, T\]
\[\vec{F} = (4\hat{i} - 3\hat{j}) \times 10^{-12} \, N\]
\[q = 10^{-9} \, C\]
3. Set up the equation and solve for the velocity:
Let \(\vec{v} = v_x\hat{i} + v_y\hat{j} + v_z\hat{k}\). Substituting into the magnetic force equation:
\[(4\hat{i} - 3\hat{j}) \times 10^{-12} = 10^{-9}((v_x\hat{i} + v_y\hat{j} + v_z\hat{k}) \times 10^{-4}\hat{k})\]
Calculate the cross product:
\[(4\hat{i} - 3\hat{j}) \times 10^{-12} = 10^{-9} \times 10^{-4}(v_x(\hat{i} \times \hat{k}) + v_y(\hat{j} \times \hat{k}) + v_z(\hat{k} \times \hat{k}))\]
\[(4\hat{i} - 3\hat{j}) \times 10^{-12} = 10^{-13}(-v_x\hat{j} + v_y\hat{i})\]
Equate the components:
\[4 \times 10^{-12} = 10^{-13}v_y \implies v_y = 40 \, m/s\]
\[-3 \times 10^{-12} = -10^{-13}v_x \implies v_x = 30 \, m/s\]
The velocity vector is \(\vec{v} = 30\hat{i} + 40\hat{j}\) (the z-component is indeterminate as \(v_z\) disappears in the cross product).
4. Calculate the speed:
The speed is the magnitude of the velocity vector:
\[|\vec{v}| = \sqrt{v_x^2 + v_y^2} = \sqrt{30^2 + 40^2} = \sqrt{900 + 1600} = \sqrt{2500} = 50 \, m/s\]
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
The magnetic field is a field created by moving electric charges. It is a force field that exerts a force on materials such as iron when they are placed in its vicinity. Magnetic fields do not require a medium to propagate; they can even propagate in a vacuum. Magnetic field also referred to as a vector field, describes the magnetic influence on moving electric charges, magnetic materials, and electric currents.