Consider a uniform magnetic field B acting perpendicular to the plane of paper and directed into the paper. Let a charged particle +q enter the region of the magnetic field with velocity v and perpendicular to the direction of B.
Force acting on the charge +q due to the uniform magnetic field is given by
F = qvB sinθ
Where θ is the angle between v and B.
Since the charged particle moves at a right angle to the magnetic field, therefore θ = 900
⇒ F = qvB sin90 = qvB
This force always acts perpendicular to the direction of motion of the charged particle and magnetic field. Thus the path of the charged particle is Circular.
Now the necessary centripetal force required by the charged particle to move in a circular path is given by
FC = mv2/r
Where
This centripetal force is provided by the magnetic force F = qvB
Therefore,
mv2/r = qvB
⇒ r = mv / qB
Time period to complete a circle is given by
T = circumference of the circle/speed
⇒ T = 2πr/v
On substituting the value of v, we get
T = 2πm/qB
Frequency of the charged particle is given by
f = 1/T = qB/2πm
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).