Given: an electron (mass \(m\), charge \(-e\)) enters a uniform magnetic field \(\vec{B}=B\hat{j}\) with initial velocity \(\vec{v}=\vec{v_0}\) (where \(v_0>0\)). The de-Broglie wavelength initially is \(\lambda_0\). We need to find its wavelength after time \(t\).
The magnetic field exerts a force on the moving electron given by the Lorentz force:
\[ \vec{F} = -e(\vec{v}\times\vec{B}). \]
This force changes the direction of velocity but not its magnitude (since the magnetic force is perpendicular to \(\vec{v}\)). Hence, the speed remains constant.
The de-Broglie wavelength is given by:
\[ \lambda = \frac{h}{p} = \frac{h}{mv}. \] Since \(v\) (the magnitude of velocity) is unchanged, the de-Broglie wavelength also remains constant in time.
Step 1: Write the equation of motion:
\[ m\frac{d\vec{v}}{dt} = -e(\vec{v}\times\vec{B}). \]
The magnetic field causes circular motion with angular frequency (cyclotron frequency):
\[ \omega = \frac{eB}{m}. \]
Step 2: The magnitude of velocity remains \(v_0\), only its direction changes with time. Therefore, momentum magnitude \(p=mv_0\) remains constant.
Step 3: Hence, the de-Broglie wavelength at time \(t\) is:
\[ \lambda = \frac{h}{mv_0} = \lambda_0. \]
\[ \boxed{\lambda(t)=\lambda_0.} \]
The de-Broglie wavelength of the electron remains unchanged with time.
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:

An infinite wire has a circular bend of radius \( a \), and carrying a current \( I \) as shown in the figure. The magnitude of the magnetic field at the origin \( O \) of the arc is given by:
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
The major product (A) formed in the following reaction sequence is
