The minimum wavelength of X-rays produced by electrons accelerated by a potential difference of V volt is equal to 

1. $\frac{eV}{hc}$ 

2. $\frac{eh}{cV}$ 

3. $\frac{hc}{eV}$ 

4. $\frac{cV}{eh}$

The graph between the square root of the frequency of a specific line of the characteristic spectrum of X-rays and the atomic number of the target will be:

1.
2.
3.
4.

The wavelength of $K_{\alpha }$ X-rays for lead isotopes $P{b}^{208},<mspace\; width="1em"></mspace>P{b}^{206},<mspace\; width="1em"></mspace>P{b}^{204}<mspace\; width="1em"></mspace>are<mspace\; width="1em"></mspace>{\lambda }_1,<mspace\; width="1em"></mspace>{\lambda }_2<mspace\; width="1em"></mspace>and<mspace\; width="1em"></mspace>{\lambda }_3$ respectively. Then

1. ${\lambda }_1={\lambda }_2>{\lambda }_3$   

2. ${\lambda }_1>{\lambda }_2>{\lambda }_3$

3. ${\lambda }_1<{\lambda }_2<{\lambda }_3$ 

4. ${\lambda }_2={\lambda }_1={\lambda }_3$

which of the following is positively charged?

1.  $\mathrm{\alpha }-\mathrm{particles}<mspace\; width="1em"></mspace><mspace\; width="1em"></mspace>$

2.  $\mathrm{\beta }-\mathrm{particles}<mspace\; width="1em"></mspace><mspace\; width="1em"></mspace>$

3.  $\mathrm{\gamma }-\mathrm{rays}<mspace\; width="1em"></mspace><mspace\; width="1em"></mspace>$

4.  $\mathrm{X}-\mathrm{rays}$

A X-ray tube operates at an accelerating potential of 20 kV. Which of the following wavelength will be absent in the continuous spectrum of X-rays?

1.  12 pm

2.  75 pm

3.  65 pm

4.  95 pm

The longest and shortest wavelength of the Lyman series are (respectively)

1.  $1215<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}},<mspace\; width="1em"></mspace>500<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}}<mspace\; width="1em"></mspace><mspace\; width="1em"></mspace><mspace\; width="1em"></mspace>$

2.  $1215<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}},<mspace\; width="1em"></mspace>912<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}}<mspace\; width="1em"></mspace><mspace\; width="1em"></mspace>$

3.  $912<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}},<mspace\; width="1em"></mspace>500<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}}<mspace\; width="1em"></mspace><mspace\; width="1em"></mspace><mspace\; width="1em"></mspace>$

4. $<mspace\; width="1em"></mspace>912<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}},<mspace\; width="1em"></mspace>700<mspace\; width="1em"></mspace>\stackrel{0}{\mathrm{A}}$

Bragg's law for X-rays is:

1. dsin$\theta$ = 2n$\lambda$ 

2. 2dsin$\theta$ = n$\lambda$

3. nsin$\theta$ = 2$\lambda$d

4. None of these

To explain his theory, Bohr used

1. conservation of linear momentum

2. conservation of angular momentum

3. conservation of quantum  frequency

4. conservation of energy

In an experiment to determine the e/m value for an electron using Thomson's method the electrostatic deflection plates were 0.01 m apart and had a potential difference of 200 volts applied. Then the electric field strength between the plates is 

1. $1\times {10}^4<mspace\; width="1em"></mspace>V/m$ 

2. $2\times {10}^4<mspace\; width="1em"></mspace>V/m$

3. $4\times {10}^4<mspace\; width="1em"></mspace>V/m$ 

4. $5\times {10}^5<mspace\; width="1em"></mspace>V/m$