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Question: The wavelength of the first line of Lyman series for the hydrogen atom is equal to that of the secon...

The wavelength of the first line of Lyman series for the hydrogen atom is equal to that of the second line of the Balmer series for hydrogen-like ions. The atomic number Z of hydrogen-like ion is
A. 3
B. 4
C. 1
D. 2

Explanation

Solution

The atomic number of an element is the number of protons found in the nucleus of every atom of that element.
The Balmer series is a part of atomic physics which is a set of six named series describing the spectral line emission of hydrogen atoms calculated by using the Balmer formula. Balmer series of hydrogen lines the Balmer series of atomic hydrogen. These lines are emitted when electrons of hydrogen atom transitions from the n=3.
Lyman series is a hydrogen spectral series of transitions and resulting ultraviolet emission lines from the hydrogen atom as electrons go from n0n \geqslant 0 to n=1n = 1, the lowest energy level of the electrons.
In this question it is given that the wavelength of the first line of Lyman series for the hydrogen atom is equal to that of the second line of the Balmer series for hydrogen, then find the atomic number by equating the formula.

Complete step by step answer:
The first line of the Lyman series for the hydrogen atom is given as
1λLyman=R(1n121n22)\dfrac{1}{{{\lambda _{Lyman}}}} = R\left( {\dfrac{1}{{n_1^2}} - \dfrac{1}{{n_2^2}}} \right)
The atom of hydrogen is transiting from line 1 to line 2
n1=1{n_1} = 1
n2=2{n_2} = 2
So we can write

1λ=R(1n121n22) 1λ=R(112122) =R(1114) =R(414) 1λ=34R(i)  \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{n_1^2}} - \dfrac{1}{{n_2^2}}} \right) \\\ \dfrac{1}{\lambda } = R\left( {\dfrac{1}{{{1^2}}} - \dfrac{1}{{{2^2}}}} \right) \\\ = R\left( {\dfrac{1}{1} - \dfrac{1}{4}} \right) \\\ = R\left( {\dfrac{{4 - 1}}{4}} \right) \\\ \dfrac{1}{\lambda } = \dfrac{3}{4}R - - - (i) \\\

Now the second line of the Balmer series for the hydrogen atom is given as
1λBalmer=RZ2(1n121n22)\dfrac{1}{{{\lambda _{Balmer}}}} = R{Z^2}\left( {\dfrac{1}{{n_1^2}} - \dfrac{1}{{n_2^2}}} \right)
The atom of hydrogen is transiting from line 2 to line 4
n1=2{n_1} = 2
n2=4{n_2} = 4
By putting

1λ=RZ2(1n121n22) 1λ=RZ2(122142) =RZ2(14116) =RZ2(4116) 1λ=316Z2R(ii)  \dfrac{1}{\lambda } = R{Z^2}\left( {\dfrac{1}{{n_1^2}} - \dfrac{1}{{n_2^2}}} \right) \\\ \dfrac{1}{\lambda } = R{Z^2}\left( {\dfrac{1}{{{2^2}}} - \dfrac{1}{{{4^2}}}} \right) \\\ = R{Z^2}\left( {\dfrac{1}{4} - \dfrac{1}{{16}}} \right) \\\ = R{Z^2}\left( {\dfrac{{4 - 1}}{{16}}} \right) \\\ \dfrac{1}{\lambda } = \dfrac{3}{{16}}{Z^2}R - - - (ii) \\\

Since the wavelength of the first line of Lyman series for the hydrogen atom is equal to that of the second line of Balmer series, so we can write equation (i) = equation (ii), therefore

34R=316Z2R Z2=4 Z=2  \dfrac{3}{4}R = \dfrac{3}{{16}}{Z^2}R \\\ {Z^2} = 4 \\\ Z = 2 \\\

Hence the atomic number Z of the hydrogen atom=2 = 2

So, the correct answer is “Option D”.

Note:
Students should not get confused with the levels of the atoms shifting, the term 1λLyman=R(1n121n22)\dfrac{1}{{{\lambda _{Lyman}}}} = R\left( {\dfrac{1}{{n_1^2}} - \dfrac{1}{{n_2^2}}} \right) should always be positive when the atoms shifts from lower level to the higher level whereas 1λLyman=R(1n121n22)\dfrac{1}{{{\lambda _{Lyman}}}} = R\left( {\dfrac{1}{{n_1^2}} - \dfrac{1}{{n_2^2}}} \right) will be negative when the atoms shifts from higher level to the lower level.