To solve this problem, we must understand the photoelectric effect, where radiation incident on a metallic surface can cause the emission of electrons, known as photoelectrons.
The key elements involved in this scenario are:
According to Einstein's photoelectric equation, the maximum kinetic energy (\(K_{\text{max}}\)) of emitted photoelectrons is calculated by:
\[K_{\text{max}} = hν - hν_0\]
Substituting the given frequencies:
\[K_{\text{max}} = h \times 2ν_0 - hν_0 = hν_0\]
This calculation shows that the maximum kinetic energy of the emitted photoelectrons is \(hν_0\). Therefore, the correct statement is:
"Maximum kinetic energy of photoelectrons emitted can be \(hν_0\)."
An alpha particle moves along a circular path of radius 0.5 mm in a magnetic field of \( 2 \times 10^{-2} \, \text{T} \). The de Broglie wavelength associated with the alpha particle is nearly
(Planck’s constant \( h = 6.63 \times 10^{-34} \, \text{Js} \))