X-ray is produced in a Coolidge tube at a given accelerating voltage. The wavelength of continuous X-rays has values from :

1.  Zero

2.  ${\lambda }_{min}\text{ to infinity and }{\lambda }_{min}>0$

3.  ${\lambda }_{min}\text{ to }{\lambda }_{max}\text{ and }0<{\lambda }_{min}<{\lambda }_{max}<\mathrm{\infty }$

4.  $\mathrm{Zero} \mathrm{to} {\mathrm{\lambda }}_{max}\text{ and }{\mathrm{\lambda }}_{max}<\mathrm{\infty }$

The continuous part of the X-ray spectrum is a result of the:

1. Photoelectric effect

2. Raman effect

3. Compton effect

4. Inverse photoelectric effect

When an electron moves from 2E level to E level, a photon of wavelength $\lambda$ is emitted. The wavelength of photon produced during its transition from $\frac{4E}{3}$ level to E level is:

1.  $\frac{\lambda }{3}$

2.  $\frac{3\lambda }{4}$

3.  $\frac{4\lambda }{3}$

4.  $3\lambda$

If an X-ray tube operates at the voltage of 10 kV, find the ratio of the de-Broglie wavelength of the incident electrons to the shortest wavelength of X-rays produced. [Given:The specific charge of the electron is $1.8\times {10}^{11}$ C/Kg]

1. 1

2. 0.1

3. 1.8

4. 1.2

When a electron in hydrogen atom  falls to the ground state from n = 2 , 10.2 eV of energy is emitted. What is the wavelength of this radiation? (Note: 1 eV = $1.60 \times {10}^{-19}$J and h = $6.626 \times {10}^{-34}$J-s)

1.  $5.76 \times {10}^{-9}m$

2.  $1.22 \times {10}^{-7}m$

3.  $3.45 \times {10}^{-7}m$

4.  $2.5 \times {10}^{15}m$

Electrons of mass m with de- Broglie wavelength λ fall on the target in an X-ray tube. The cut off wavelength (λ_o) of the emitted X-ray is :

1.  ${\mathrm{\lambda }}_0=\frac{2{\mathrm{mc\lambda }}^2}{\mathrm{h}}$

2.  ${\mathrm{\lambda }}_0=\frac{2\mathrm{h}}{\mathrm{mc}}$

3.  ${\mathrm{\lambda }}_0=\frac{2{\mathrm{m}}^2{\mathrm{c}}^2{\mathrm{\lambda }}^2}{{\mathrm{h}}^2}$

4.  ${\mathrm{\lambda }}_0=\mathrm{\lambda }$

An electron of mass m with an initial velocity $\overrightarrow{v}={\mathrm{v}}_0\hat{i}({\mathrm{v}}_0>0)$enters in an electric field $\overrightarrow{\mathrm{E}}=-E_0\hat{i}$ (E_o = constant >0) at t = 0. If ${\mathrm{\lambda }}_0$, is its de-Broglie wavelength initially, then its de-Broglie wavelength at time t is:-

1. $\frac{{\mathrm{\lambda }}_0}{\left(1+{\displaystyle \frac{{\mathrm{eE}}_0}{{\mathrm{mv}}_0}}\mathrm{t}\right)}$

2. ${\mathrm{\lambda }}_0\left(1+\frac{{\mathrm{eE}}_0}{{\mathrm{mv}}_0}\mathrm{t}\right)$

3. ${\mathrm{\lambda }}_0\mathrm{t}$

4. ${\mathrm{\lambda }}_0$

When light of frequency 2$\nu$_o (where $\nu$_o is threshold frequency), is incident on a metal plate, the maximum velocity of electrons emitted is ${\mathrm{v}}_1$. When the frequency of the incident radiation is increased to 5$\nu$_o, the maximum velocity of electrons emitted from the same plate is ${\mathrm{v}}_2$. The ratio of ${\mathrm{v}}_1$ to ${\mathrm{v}}_2$ is

1. 1: 2

2. 1: 4

3. 4: 1

4. 2: 1