We need to analyze the given position vector, determine the trajectory, velocity, acceleration, and energy of the particle to determine the correct statements.
Step 1: Determine the Trajectory
The position vector is given by: \[\vec{r} = b \cos(\omega t) \hat{i} + b \sin(\omega t) \hat{j}\] Let \(x = b \cos(\omega t)\) and \(y = b \sin(\omega t)\). Then, \[x^2 + y^2 = b^2 \cos^2(\omega t) + b^2 \sin^2(\omega t) = b^2 (\cos^2(\omega t) + \sin^2(\omega t)) = b^2\] Since \(x^2 + y^2 = b^2\), the trajectory is a circle of radius \(b\) centered at the origin.
Step 2: Calculate Velocity
The velocity vector is the time derivative of the position vector: \[\vec{v} = \frac{d\vec{r}}{dt} = -b\omega \sin(\omega t) \hat{i} + b\omega \cos(\omega t) \hat{j}\]
The speed \(v\) is the magnitude of the velocity vector: \[v = \sqrt{(-b\omega \sin(\omega t))^2 + (b\omega \cos(\omega t))^2} = \sqrt{b^2 \omega^2 (\sin^2(\omega t) + \cos^2(\omega t))} = b\omega\]
So, the speed is constant.
Step 3: Calculate Acceleration
The acceleration vector is the time derivative of the velocity vector: \[\vec{a} = \frac{d\vec{v}}{dt} = -b\omega^2 \cos(\omega t) \hat{i} - b\omega^2 \sin(\omega t) \hat{j} = -\omega^2 (b \cos(\omega t) \hat{i} + b \sin(\omega t) \hat{j}) = -\omega^2 \vec{r}\]
The magnitude of the acceleration is: \[a = |\vec{a}| = \omega^2 |\vec{r}| = \omega^2 b\]
Step 4: Calculate Energy
Since we are not given any potential energy, we can assume the total energy \(E\) is the kinetic energy: \[E = \frac{1}{2} mv^2 = \frac{1}{2} m (b\omega)^2 = \frac{1}{2} m b^2 \omega^2\]
Therefore, \[\frac{E}{\omega} = \frac{\frac{1}{2} m b^2 \omega^2}{\omega} = \frac{1}{2} m b^2 \omega\]
Since m and b are constant as well as w, \(\frac{E}{\omega}\) is proportional to omega. Hence first statement seems incorrect. Recalculating the statement one. Kinetic energy = 1/2 mv^2. Since speed = bw. KE is 1/2 * m * b^2 * w^2. \(\frac{E}{w} = 1/2 m b^2 w \) Since b is constant, w is constant then this value is constant.
Step 5: Analyze the Statements
Conclusion
The correct statements are:
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).