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QJEEAdv24Ph29ab: JEE Advanced 2024 Physics - Class 12 JEEAdv24Ph29ab Solution: A metal target with atomic number is bombarded with a high…

A metal target with atomic number Z=46Z=46 is bombarded with a high energy electron beam. The emission of X-rays from the target is analyzed. The ratio rr of the wavelengths of the KαK_\alpha -line and the cut-off is found to be r=2r=2 . If the same electron beam bombards another metal target with Z=41Z=41 , the value of rr will be

Multiple Choice Options

  • A 2.53
  • B 1.27
  • C 2.24
  • D 1.58

Step-by-Step Verified Solution

To solve this problem, we need to understand the relationship between the atomic number ZZ , the characteristic X-ray wavelengths, and the cut-off wavelength in X-ray spectra.

The cut-off wavelength, also known as the minimum wavelength ( λmin\lambda_{\text{min}} ), corresponds to the maximum energy of the X-rays produced and can be related to the accelerating voltage used in the X-ray tube. The characteristic X-rays, such as the KαK_\alpha -line, correspond to specific electron transitions in the atom and are dependent on the atomic number ZZ of the target material.

The wavelength of the KαK_\alpha -line is given by Moseley's Law, which can be approximated as:

λKα∝1(Z−1)2\lambda_{K_\alpha} \propto \frac{1}{(Z - 1)^2}

The cut-off wavelength is given by the relationship between the energy of the incident electrons and the X-ray produced:

λmin=hceV\lambda_{\text{min}} = \frac{hc}{eV}

Now, given the ratio rr for the first metal target with Z=46Z = 46 :

r=λKαλmin=2r = \frac{\lambda_{K_\alpha}}{\lambda_{\text{min}}} = 2

For the second metal target with Z=41Z = 41 , let's denote the new ratio as r2r_2 . We assume the same cutoff wavelength since the same electron beam is used.

The ratio for Z=41Z = 41 can be calculated using the relationship between the KαK_\alpha -line wavelenghts:

λKα(1)λKα(2)=(Z2−1Z1−1)2\frac{\lambda_{K_\alpha (1)}}{\lambda_{K_\alpha (2)}} = \left( \frac{Z_2 - 1}{Z_1 - 1} \right)^2

Substituting Z1=46Z_1 = 46 and Z2=41Z_2 = 41 :

λKα(1)λKα(2)=(41−146−1)2=(4045)2=(89)2=6481\frac{\lambda_{K_\alpha (1)}}{\lambda_{K_\alpha (2)}} = \left( \frac{41 - 1}{46 - 1} \right)^2 = \left( \frac{40}{45} \right)^2 = \left( \frac{8}{9} \right)^2 = \frac{64}{81}

Let λKα(1)=2λmin\lambda_{K_\alpha (1)} = 2 \lambda_{\text{min}} because r=2r = 2 . Therefore:

λKα(2)=λKα(1)⋅8164=2λmin⋅8164\lambda_{K_\alpha (2)} = \lambda_{K_\alpha (1)} \cdot \frac{81}{64} = 2 \lambda_{\text{min}} \cdot \frac{81}{64}

Thus, the new ratio r2r_2 is:

r2=λKα(2)λmin=2⋅8164=16264=2.53r_2 = \frac{\lambda_{K_\alpha (2)}}{\lambda_{\text{min}}} = 2 \cdot \frac{81}{64} = \frac{162}{64} = 2.53

So, the value of rr for the second metal target with Z=41Z = 41 is:

Option A: 2.53

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