alpha particle scattering experiment - observations
alpha particle scattering experiment - conclusions
distance of closest approach (d) =
(1/4πε)×(2Ze^2/KE)
Define Impact Parameter.
Impact parameter is defined as the perpendicular distance between the initial velocity vector of the alpha particle and the line passing through the center of nucleus.
Expressions for potential, kinetic and total energy based on rutherford’s model.
PE = (1/4πε)×(-e^2/r)
KE = (1/8πε)×(e^2/r)
Total energy = -(1/8πε)×(e^2/r)
Two limitations of Rutherford’s model
The 1st postulate of Bohr’s model of an atom
Electrons around the nucleus can continue revolving without radiating energy in certain specified orbits known as non-radiating orbits or stable orbits.
The 2nd postulate of Bohr’s model of an atom
Electrons whose angular momentum is an integral multiple of h/2π can revolve without radiating energy.
The 3rd postulate of Bohr’s model of an atom
Electrons deexciting from higher energy level to lower energy level radiate energy equal to the difference in the energy levels of initial and final orbits.
Expressions for potential, kinetic and total energy according to Bohr’s model
PE = (1/4πε)×(-me^4/n^2×h^2) KE = (1/8πε)×(me^e4/n^2×h^2) TE = -(1/8πε)×(me^4/n^2×h^2)
Expression for wavelength of photon emitted due to deexcitation of electron
1/λ = R((1/nf^2) - (1/ni^2))
for an electron to show stationary wave pattern, the circumference of the orbit =
nλ (where λ is the wavelength of electron in nth orbit/debroglie’s wavelength)
Debroglie’s wavelength =
h/mv
Limitations of Bohr’s Model
number of spectral lines emitted when an electron undergo deexcitation from level n =
n(n-1)/ 2
hydrogen spectrum, n = 1
Lymann series
UV region
E1 = -13.6 eV
hydrogen spectrum, n = 2
Balmer series
Visible region
E2 = -3.4 eV
hydrogen spectrum, n = 3
Paschen series
Infrared region
E3 = -1.51 eV
hydrogen spectrum, n = 4
Brackett series
Infrared region
E4 = -0.85 eV
hydrogen spectrum, n = 5
Pfund series
Infrared region
E5 = -0.54 eV