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Question: The limit of Ballmer series is \(3646\,\mathop A\limits^0 \) the wavelength to first member of this ...

The limit of Ballmer series is 3646A03646\,\mathop A\limits^0 the wavelength to first member of this series will be
(A) 6563A06563\,\mathop A\limits^0
(B) 3646A03646\,\mathop A\limits^0
(C) 7200A07200\,\mathop A\limits^0
(D) 1000A01000\,\mathop A\limits^0

Explanation

Solution

Use the formula of the wavelength of the Balmer series and substitute the assumed values to find the Rydberg constant. Substitute this in the wavelength formula again to find the value of the wavelength when the electron moves from the first member.

Useful formula:
The wavelength in the Balmer series is given by
1λ=R[1n121n22]\dfrac{1}{\lambda } = R\left[ {\dfrac{1}{{{n_1}^2}} - \dfrac{1}{{{n_2}^2}}} \right]
Where λ\lambda is the wavelength of the Balmer series, RR is the Rydberg constant , n1andn2{n_1}\,and\,{n_2} are the level of the orbit.

Complete step by step solution:
It is given that the
Limit of the Balmer series, λ=3646A0\lambda = 3646\,\mathop A\limits^0
It is known that the Balmer series have n1=2{n_1} = 2 and n2=3,4,........,{n_2} = 3,4,........,\infty
Use the formula of the wavelength and let us consider the value of the value of n1andn2{n_1}\,and\,{n_2} as 2and2\,and\,\infty respectively.
13646=R[12212]\dfrac{1}{{3646}} = R\left[ {\dfrac{1}{{{2^2}}} - \dfrac{1}{{{\infty ^2}}}} \right]
By simplifying the above equation, we get
13646=[R4]\dfrac{1}{{3646}} = \left[ {\dfrac{R}{4}} \right]
R=43646R = \dfrac{4}{{3646}}
Hence the value of the Rydberg constant is obtained as 43646\dfrac{4}{{3646}}.
Again using the same formula of the wavelength of the Balmers series.
1λ=R[1n121n22]\dfrac{1}{\lambda } = R\left[ {\dfrac{1}{{{n_1}^2}} - \dfrac{1}{{{n_2}^2}}} \right]
In the question, it is asked to find the wavelength of the first member. Hence the value of n1{n_1} is considered as 22 and the value of the n2{n_2} is considered as 33 . And also substituting the value of the Rydberg constant.
1λ=43646[1419]\dfrac{1}{\lambda } = \dfrac{4}{{3646}}\left[ {\dfrac{1}{4} - \dfrac{1}{9}} \right]
By simplifying the above equation,
λ=13125620\lambda = \dfrac{{131256}}{{20}}
By performing the basic arithmetic operations,
λ=6562.8A06563A0\lambda = 6562.8\,\mathop A\limits^0 \approx 6563\,\mathop A\limits^0

Thus the option (A) is correct.

Note: If the electrons from the higher levels move to the second orbit, it is the Balmer series. If the electron moves to the first orbit, then it is a Lyman series. It has to gain some energy to move from lower to higher orbitals and has to release energy when moving to lower energy orbitals.