An electron is moving along positive x direction in xy plane, magnetic field points in negative z direction, then the force due to magnetic field on electron points in the direction
j
-j
k
-k
To determine the direction of the force on an electron moving in a magnetic field, we use the principle of the magnetic force acting on a charged particle, given by the Lorentz force formula:
\(\mathbf{F} = q(\mathbf{v} \times \mathbf{B})\)
where:
We need to determine the cross product \(\mathbf{v} \times \mathbf{B}\). Given:
The cross product is calculated as follows:
\(\mathbf{v} \times \mathbf{B} = (v \mathbf{i}) \times (-B \mathbf{k}) = vB (\mathbf{i} \times -\mathbf{k})\).
Using the right-hand rule for cross products, \(\mathbf{i} \times \mathbf{k} = \mathbf{j}\). Therefore:
\(\mathbf{v} \times \mathbf{B} = vB (-\mathbf{j}) = -vB \mathbf{j}\).
Now, since the electron has a negative charge (\(q = -e\)), the direction of the force \(q(\mathbf{v} \times \mathbf{B})\) is opposite to the direction of \(\mathbf{v} \times \mathbf{B}\):
\(\mathbf{F} = -e(-vB \mathbf{j}) = evB \mathbf{j}\).
This means the direction of the force on the electron is in the negative y-direction (\(-\mathbf{j}\)).
Thus, the force due to the magnetic field on the electron points in the negative y-direction, corresponding to the option -j.
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.