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Question: The wavelength of \({K_\alpha }\) line for an element of atomic number 43 is ‘\(\lambda \)’. Then th...

The wavelength of Kα{K_\alpha } line for an element of atomic number 43 is ‘λ\lambda ’. Then the wavelength of Kα{K_\alpha } line for an element of atomic number 29 is
A) 94λ\dfrac{9}{4}\lambda .
B) 4329λ\dfrac{{43}}{{29}}\lambda .
C) 49λ\dfrac{4}{9}\lambda .
D) 4228λ\dfrac{{42}}{{28}}\lambda .

Explanation

Solution

The formula of Moseley’s law for k alpha line can be used for the calculation for the correct answer for this problem. The formula for Moseley’s law for the k alpha line contains constants a and b, which has the value b=1. The value of constants a and b depends on the series.

Formula: The formula for Moseley’s law for k alpha line is λ1(Zb)2\lambda \propto \dfrac{1}{{{{\left( {Z - b} \right)}^2}}} where λ\lambda is the wavelength, ZZ is the atomic number and bb is constant having value of b=1b = 1 for k alpha line.

Step by step solution:
Step 1.
As the Moseley’s law for alpha line is λ1(Zb)2\lambda \propto \dfrac{1}{{{{\left( {Z - b} \right)}^2}}} where λ\lambda is the wavelength, ZZ is the atomic number and bb is constant having value of b=1b = 1 for k alpha line.
For atomic number 43
λ1(Zb)2 λ431(431)2 λ431(42)2  \lambda \propto \dfrac{1}{{{{\left( {Z - b} \right)}^2}}} \\\ {\lambda _{43}}\propto \dfrac{1}{{{{\left( {43 - 1} \right)}^2}}} \\\ {\lambda _{43}}\propto \dfrac{1}{{{{\left( {42} \right)}^2}}} \\\ ………eq.(1)
Step 2.
As the Moseley’s law for alpha line is λ1(Zb)2\lambda \propto \dfrac{1}{{{{\left( {Z - b} \right)}^2}}} where λ\lambda is the wavelength, ZZ is the atomic number and bb is constant having value of b=1b = 1 for k alpha line.
For atomic number 29
λ1(Zb)2 λ291(291)2 λ291(28)2  \lambda \propto \dfrac{1}{{{{\left( {Z - b} \right)}^2}}} \\\ {\lambda _{29}}\propto \dfrac{1}{{{{\left( {29 - 1} \right)}^2}}} \\\ {\lambda _{29}}\propto \dfrac{1}{{{{\left( {28} \right)}^2}}} \\\ ………eq.(2)
Step 3.
We can get the value of λ29{\lambda _{29}} by dividing equation 2nd by equation 1st
Therefore applying(2)(1)\dfrac{{\left( 2 \right)}}{{\left( 1 \right)}},
λ29λ43=(42)2(28)2 λ29=(4228)2λ43  \dfrac{{{\lambda _{29}}}}{{{\lambda _{43}}}} = \dfrac{{{{\left( {42} \right)}^2}}}{{{{\left( {28} \right)}^2}}} \\\ {\lambda _{29}} = {\left( {\dfrac{{42}}{{28}}} \right)^2} \cdot {\lambda _{43}} \\\ ………eq.(3)
As the wavelength of atomic number 43 is λ\lambda
So,
λ43=λ{\lambda _{43}} = \lambda
Replacing λ43=λ{\lambda _{43}} = \lambda in equation (3).
λ29=(4228)2λ43 λ29=(4228)2λ  {\lambda _{29}} = {\left( {\dfrac{{42}}{{28}}} \right)^2} \cdot {\lambda _{43}} \\\ {\lambda _{29}} = {\left( {\dfrac{{42}}{{28}}} \right)^2} \cdot \lambda \\\ ………eq.(4)
Step 4.
Solving the equation (4) we get
λ29=(4228)2λ λ29=94λ  {\lambda _{29}} = {\left( {\dfrac{{42}}{{28}}} \right)^2} \cdot \lambda \\\ {\lambda _{29}} = \dfrac{9}{4} \cdot \lambda \\\
So the correct answer for this problem is λ29=94λ{\lambda _{29}} = \dfrac{9}{4} \cdot \lambda i.e. option A.

Option A is correct

Note: While solving this question students should know that Moseley’s law says that λ=ca2(Zb)2\lambda = \dfrac{c}{{{a^2}{{\left( {Z - b} \right)}^2}}} where cc is speed of light aa and bb are constants and ZZ is the atomic number the value of bb is b=1b = 1 for k alpha line. Also the values of aa and bb are independent of the material but depends on the X-ray series.