
To determine the value of \(x\) such that \((\lambda_d)_{m_1} = x \times (\lambda_d)_{m_2}\), we will use the de-Broglie wavelength formula:
\(\lambda_d = \frac{h}{\sqrt{2mE}}\)
where \(h\) is the Planck’s constant, \(m\) is the mass of the particle, and \(E\) is the energy.
The energy \(E\) provided is \(200\,\text{keV}\), which is equal for both particles.
For the first particle with mass \(m_1 = 1\,\text{amu}\):
\((\lambda_d)_{m_1} = \frac{h}{\sqrt{2 \cdot 1 \cdot \text{amu} \cdot 200\,\text{keV}}}\)
For the second particle with mass \(m_2 = 4\,\text{amu}\):
\((\lambda_d)_{m_2} = \frac{h}{\sqrt{2 \cdot 4 \cdot \text{amu} \cdot 200\,\text{keV}}}\)
Dividing the wavelengths:
\(\frac{(\lambda_d)_{m_1}}{(\lambda_d)_{m_2}} = \frac{\sqrt{2 \cdot 4 \cdot 200\,\text{keV}}}{\sqrt{2 \cdot 1 \cdot 200\,\text{keV}}}\)
This simplifies to:
\(\frac{(\lambda_d)_{m_1}}{(\lambda_d)_{m_2}} = \sqrt{4} = 2\)
Thus, \(x = 2\).
The computed value \(x=2\) is confirmed to be within the given range of \(2,2\).
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).