For the Balmer series, \(n_i = 2\).
Thus, the expression of wave number is given by,
\(\bar v = [ \frac {1}{(2)^2}-\frac {1}{n_f^2}] (1.097×10^7 m^{-1})\)
Wavenumber is inversely proportional to wavelength of transition. Hence, for the longest wavelength transition, Wavenumber has to be the smallest. For Wavenumber to be minimum, \(n_f\) should be minimum.
For the Balmer series, a transition from \(n_i = 2\) to \(n_f = 3\) is allowed.
Hence, taking \(n_f = 3\), we get:
\(\bar v = (1.097×10^7)[\frac {1}{2^2} - \frac {1}{3^2}]\)
\(\bar v = (1.097×10^7)[\frac {1}{4} - \frac {1}{9}]\)
\(\bar v = (1.097×10^7)[\frac {9-4}{36}]\)
\(\bar v = (1.097×10^7)(\frac {5}{36})\)
\(\bar v = 1.5236×10^6 \ m^{-1}\)
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.