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Bohr’s Atomic Model
Electron can revolve in certain non-radiating orbits called stationary or bits for which the angular momentum of electron is an integer multiple of (h / 2π)
mvr = nh / 2π
where n = I, 2. 3,… called principle quantum number.
The radiation of energy occurs only when any electron jumps from one permitted orbit to another permitted orbit.
Energy of emitted photon
hv = E2 – E1
where E1 and E2are energies of electron in orbits.
Radius of orbit of electron is given by
r = n2h2 / 4π2 mK Ze2 ⇒ r ∝ n2 / Z
where, n = principle quantum number, h = Planck’s constant, m = mass of an electron, K = 1 / 4 π ε, Z = atomic number and e = electronic charge.
Velocity of electron in any orbit is given by
v = 2πKZe2 / nh ⇒ v ∝ Z / n
Frequency of electron in any orbit is given by
v = KZe2 / nhr = 4π2Z2e4mK2 / n3 h3
⇒ v prop; Z3 / n3
Kinetic energy of electron in any orbit is given by
Ek = 2π2me4Z2K2 / n2 h2 = 13.6 Z2 / n2 eV
Potential energy of electron in any orbit is given by
Ep = – 4π2me4Z2K2 / n2 h2 = 27.2 Z2 / n2 eV
⇒ Ep = ∝ Z2 / n2
Total energy of electron in any orbit is given by
E = – 2π2me4Z2K2 / n2 h2 = – 13.6 Z2 / n2 eV
⇒ Ep = ∝ Z2 / n2
Wavelength of radiation emitted in the radiation from orbit n2 to n1 is given by
In quantum mechanics, the energies of a system are discrete or quantized. The energy of a particle of mass m is confined to a box of length L can have discrete values of energy given by the relation
En = n2 h2 / 8mL2 ; n < 1, 2, 3,…
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157 videos|452 docs|213 tests
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