Step 1: The unit vector \( \mathbf{v} \) in the XY-plane making an angle of \( 45^\circ \) with \( \hat{i} + \hat{j} \) is given by:
\[ \mathbf{v} = \hat{i} \cos(45^\circ) + \hat{j} \sin(45^\circ) \]
Step 2: The angle between \( \mathbf{v} \) and the vector \( 3\hat{i} - 4\hat{j} \) is \( 60^\circ \). Using the dot product formula:
\[ \mathbf{v} \cdot (3\hat{i} - 4\hat{j}) = |\mathbf{v}| \cdot |3\hat{i} - 4\hat{j}| \cdot \cos(60^\circ) \]
Step 3: Solving this system of equations gives the components of the unit vector \( \mathbf{v} \).
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).