For He + ion, the wave number associated with the Balmer transition, n = 4 to n = 2 is given by :
v- = \(\frac{1}{\lambda}\) = RZ2 (\(\frac{1}{n_1^2}-\frac{1}{n_2^2}\))
Where, n1 = 2 ,n2 = 4 , Z = atomic number of helium
v- = \(\frac{1}{\lambda}\) = R (2)2 (\(\frac{1}{4}-\frac{1}{6}\)) = 4R (\(\frac{4-1}{16}\))
v- = \(\frac{1}{\lambda}\) = \(\frac{3R}{4}\) ⇒ λ = \(\frac{4}{3R}\)
According to the question, the desired transition for hydrogen will have the same wavelength as that of He+.
⇒ R(1)2[\(\frac{1}{n_1^2}-\frac{1}{n_2^2}\)] = \(\frac{3R}{4}\)
By hit and trail method, the equality given by equation (1) is true only when n1 = 1 and n2 = 2.
∴ The transition for n2 = 2 to n = 1 in the hydrogen spectrum would have the same wavelength as the Balmer transition n = 4 to n= 2 of He+ spectrum.
The atomic structure of an element refers to the constitution of its nucleus and the arrangement of the electrons around it. Primarily, the atomic structure of matter is made up of protons, electrons and neutrons.
Dalton proposed that every matter is composed of atoms that are indivisible and indestructible.
The following are the postulates of his theory:
Several atomic structures of an element can exist, which differ in the total number of nucleons.These variants of elements having a different nucleon number (also known as the mass number) are called isotopes of the element. Therefore, the isotopes of an element have the same number of protons but differ in the number of neutrons. For example, there exist three known naturally occurring isotopes of hydrogen, namely, protium, deuterium, and tritium.