Consider a beam of electrons (each electron with energy \(E_0\)) incident on a metal surface kept in an evacuated chamber. Then:
1. | no electrons will be emitted as only photons can emit electrons. |
2. | electrons can be emitted but all with energy, \(E_0.\) |
3. | electrons can be emitted with any energy, with a maximum of \({E}_0-\phi\) (\(\phi\) is the work function). |
4. | electrons can be emitted with any energy, with a maximum \(E_0.\) |
(a) | The particle could be moving in a circular orbit with the origin as the centre. |
(b) | The particle could be moving in an elliptic orbit with origin as its focus. |
(c) | When the de-Broglie wavelength is \(λ_1,\) the particle is nearer the origin than when its value is \(λ_2.\) |
(d) | When the de-Broglie wavelength is \(λ_2,\) the particle is nearer the origin than when its value is \(λ_1.\) |
Choose the correct option from the given ones:
1. | (b) and (d) only |
2. | (a) and (c) only |
3. | (b), (c), and (d) only |
4. | (a), (c), and (d) only |
(a) | decreases with increasing \(n,\) with \(\nu\) fixed |
(b) | decreases with \(n\) fixed, \(\nu\) increasing |
(c) | remains constant with \(n\) and \(\nu\) changing such that \(n\nu=\) constant |
(d) | increases when the product \(n\nu\) increases |
Choose the correct option:
1. | (b), (d) | 2. | (a), (c), (d) |
3. | (a), (d) | 4. | (a), (b), (c) |
(a) | \(\lambda = 10~\text{nm}\) | (b) | \(\lambda = 10^{-1}~\text{nm}\) |
(c) | \(\lambda = 10^{- 4}~\text{nm}\) | (d) | \(\lambda = 10^{- 6}~\text{nm}\) |
Choose the correct option:
1. (a), (c)
2. (a), (d)
3. (c), (d)
4. (a), (b)
The figure shows the stopping potential \(V_0\) (in volts), as a function of frequency \(\nu,\) for a sodium emitter. From the data plotted in the graph, what is the work function of sodium?
(Given: Planck’s constant, \(h=\) \(6.63\times 10^{-34}~\text{J-s}\) and the charge of an electron, \(e=1.6\times 10^{-19}~\text{C}\))
1. | \(1.95~\text{eV}\) | 2. | \(2.12~\text{eV}\) |
3. | \(1.82~\text{eV}\) | 4. | \(1.66~\text{eV}\) |
The stopping potential for electrons emitted from a photosensitive surface illuminated with light of wavelength \(491~\text{nm}\) is \(0.710~\text{V}.\) When the wavelength of the incident light changes, the stopping potential increases to \(1.43~\text{V}.\) The new wavelength is approximately:
1. \(329~\text{nm}\)
2. \(309~\text{nm}\)
3. \(382~\text{nm}\)
4. \(400~\text{nm}\)
1. | \(\dfrac{\lambda{P}}{h c} f\) | 2. | \(\dfrac{2\lambda{P}}{h c} f\) |
3. | \(\dfrac{\lambda{P}}{h c} f e\) | 4. | \(\dfrac{2\lambda{P}}{h c} f e\) |
1. | a straight line passing through the origin. |
2. | a circle. |
3. | an ellipse. |
4. | a parabola. |
1. | \(\dfrac{h \omega_{1}}{2 \pi}\) or \(\dfrac{h \omega_{2}}{2 \pi}\) | Either
2. | \(\left(\dfrac{h \omega_{1}}{2 \pi}-h \nu_{0}\right)\) or \(\left(\dfrac{h \omega}{2 \pi}-h \nu_{0}\right)\) | Either
3. | \(\dfrac{h\left(\omega_{1}+\omega_{2}\right)}{2 \pi}-h \nu_{0}\) |
4. | Both \(\dfrac{h\left(\omega_{1}+\omega_{2}\right)}{2 \pi}-h \nu_{0}\) and \(\dfrac{h\left |\omega_{1}-\omega_{2}\right|}{2 \pi}-h \nu_{0}\) |
1. | does not depend on \(v\) |
2. | increases as \(v\) increases |
3. | decreases as \(v\) increases |
4. | first increases and then decreases as \(v\) is increased |