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Atomic and Nuclear Physics

The Bohr Model of the Atom

Bohr proposed that the “quantum” of angular momentum, L, possessed by the electron in a hydrogen atom is h/(2PI).

Therefore, the “angular momentum levels” are given by

where n is an integer. So, in the lowest level L = h/2PI, in the next level L = 2h/2PI, etc

mass of electron = m
charge on electron = e
speed of electron = v

Angular momentum,  L = mvr

So, we have

 
     
and so           

equation 1

The force acting on the electron is given by

If the electron orbits in a circular path, the force is also equal to

so, the speed, v, of the electron is given by

Substituting this into equation 1 allows us to calculate the radii of the allowed orbits

 

equation 2

The K.E. of the electron  ½mv2 which gives

The potential, V, at a point a distance r away from a proton is given by

Therefore the potential energy possessed by an electron at a distance r away from a proton is given by

The total energy (K.E. + P.E.) is therefore

 

equation 3

Substituting for r from equation 2, we have


Where En is the total energy (K.E.+P.E.) possessed by the electron when it is in level n.

We see that En is proportional to 1/n2 where the constant of proportionality is FORMULA16

If an electron falls from one energy level, ninitial to a lower level, nfinal, then the energy of the quantum of electro-magnetic radiation emitted is equal to the difference between the two levels and is therefore given by


The energy of a quantum of e.m. radiation, E = hc/DELTASMRED
So, we can write (ignoring the minus sign)

which has the same form as the Balmer series if we put nfinal = 2

and

 

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