- Statement I: This statement accurately reflects the Heisenberg Uncertainty Principle, which posits that simultaneously measuring a particle's precise position and momentum is impossible. This statement is valid.
- Statement II: The Heisenberg Uncertainty Principle establishes a relationship between the uncertainty in position (\( \Delta x \)) and momentum (\( \Delta p \)), defined by: \[ \Delta x \Delta p \geq \frac{h}{4\pi} \] For an electron, when the uncertainties in position and momentum are equivalent, the uncertainty in velocity \( \Delta v \) is quantifiable as: \[ \Delta v = \frac{\Delta p}{m} \geq \sqrt{\frac{h}{\pi}} \times \frac{1}{2m} \] This statement is also accurate.
Consequently, the correct choice is \( \boxed{(2)} \), indicating that both Statement I and Statement II are true.
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).