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Bohr's Theory of Hydrogen Atom
Postulates
(i) Every atom consists of nucleus and suitable number of electrons revolved around the nucleus in circular orbits.
(ii) Electrons revolved only in certain non-radiating orbits called stationery orbits for which the total angular momentum is an integral multiple of h/2p where h is plank's constant.(iii) Radiation occurs when an electron jumps from one permitted orbit to another. It is emitted when electron jumps from higher orbit to a lower orbit
i.e., E2 - E1 = hf, where f is frequency of radiation.Derivation of Radius
Radii of orbits
According to Bohr's second postulate
Since
Where m is mass of electron, v is linear velocity, r is radius of orbit in which e revolves around the nucleus.
Now
[Because necessary centripetal force is provided by the electrostatic force of attraction between electron and nucleus] whose charge is Ze where Z is the atomic number of the atom.
Substituting for v,

On substituting the value h = 6.6x10-34 J-sec
n = 1K = 9 x 109Nm2/c2
m = 9.1 x 10-31kge = 1.6 x 10-19c, we get
r = 5.29 x 10-11mVelocity of electron in a stationary orbit substituting the expression for r in the equation.




The total energy (T.E) of the electron in stationary orbit
The energy of electron revolving in a stationery orbit is of two types. Kinetic energy due to velocity and potential energy due to the position of the electron.
Now

(-ve is for charge of an electron)
Now T.E = K.E + P.E
Spectral series of hydrogenations.







