Determine the radius, momentum, and energy of the nth orbital of hydrogen or any other atom
Derivation of Radius, Velocity, and Energy Equations for the n-th Orbit of Hydrogen and Hydrogen-like Atoms
1. Determination of the Radius of the n-th Orbit:
Let the total positive charge in the nucleus of a hydrogen or any hydrogen-like atom be = Ze (where Z = atomic number and e = charge of a proton or an electron). In a hydrogen atom, a single electron revolves around the nucleus in a circular orbit of radius r with a velocity v.
According to Coulomb’s law, the electrostatic force of attraction exerted by the nucleus on the electron (i.e., the inward centripetal force) is—
Again, for the electron revolving with a velocity v, the outward centrifugal force is—
[Here, m = mass of the electron and r = radius of the orbit]
The essential condition for an electron to remain in a stable circular orbit is that the centripetal force and centrifugal force must be perfectly balanced and equal to each other. Therefore—
or,
or, mv2r = Ze2
or, v2 =
Furthermore, according to Bohr’s postulate, the angular momentum of an electron in a stable stationary orbit is given by—
or, v =
or, v2 =
Equating expressions (iii) and (iv), we get—
or, Ze2 =
or, Ze2 · 4π2mr = n2h2
or, r =
Equation (v) is used to determine the radius of any specific stationary orbit of a revolving electron.
2. Determination of the Velocity of an Electron Revolving in a Bohr Orbit:
According to the principles of Bohr’s atomic model—
or, r =
Again, we know that the radius of the orbit is given by—
From equations (i) and (ii), we get—
or,
or, v =
For a hydrogen atom (Z = 1), the orbital velocity of the electron in different orbits is—
3. Determination of the Total Energy Expression of an Electron in the n-th Orbit:
The total energy (En) of an electron in the n-th orbit of an atom is equal to the sum of its Potential Energy and Kinetic Energy.
or, En =
[From equation (iii) of the radius derivation, we know: mv2 =
or, En =
or, En =
or, En =
or, En =
Now, substituting the expression for radius r from equation (v), we get—
For a hydrogen atom (Z = 1), the total energy in the n-th orbit is given by—
Values of Essential Constants for Determining Radius, Velocity, and Energy:
| Sl. No. | Constant / Parameter | Symbol | C.G.S Unit System | M.K.S / S.I Unit System |
|---|---|---|---|---|
| 1 | Velocity of Light | c | 3 × 1010 cm s-1 | 3 × 108 m s-1 |
| 2 | Planck’s Constant | h | 6.626 × 10-27 erg s | 6.626 × 10-34 J s |
| 3 | Mass of Electron | m | 9.108 × 10-28 g | 9.108 × 10-31 kg |
| 4 | Charge of Electron | e | 4.8 × 10-10 e.s.u | 1.602 × 10-19 C |
| 5 | Rydberg Constant | RH | 109678 cm-1 | 10967800 m-1 |
| 6 | Energy of 1 eV Electron | E | 1.6 × 10-12 erg | 1.6 × 10-19 J |
| 7 | Radius (1st Orbit of H) | r | 5.292 × 10-9 cm | 5.292 × 10-11 m |
| 8 | Velocity (1st Orbit of H) | v | 2.18 × 108 cm s-1 | 2.18 × 106 m s-1 |
| 9 | Total Energy (1st Orbit of H) | En | -2.18 × 10 Granger-11 erg | -2.18 × 10-18 J |
1 erg = 1 g cm2 s-2 | 1 e.s.u = 1 g1/2 cm3/2 s-1
(i) 1 m = 102 cm (or, 1 cm = 10-2 m) (ii) 1 cm s-1 = 10-2 m s-1 (iii) 1 erg = 10-7 J (or, 1 J = 107 erg)
Task: Determine the radius of the first orbit, and the velocity and total energy of the electron in that orbit, for H, He+, Li2+, and Be3+.
Derivation of the Rydberg Equation (From Bohr’s Corollaries):
When an electron transitions (de-excites) from a higher orbit (n2) to a lower orbit (n1), the frequency of the emitted electromagnetic radiation is ν. According to Bohr’s theory, it can be written as:
or, h ·
or,
or,
or,
or,
The Rydberg Equation
1. For Hydrogen atom (Z = 1), the Rydberg equation is expressed as:
2. For Hydrogen-like ions (e.g., He+, Li2+, Be3+, etc.), the equation becomes:
Theoretical Determination of the Rydberg Constant (RH)
According to Bohr’s theory, the formula for the Rydberg constant is:
The experimentally determined actual value of the Rydberg constant is 109,678 cm-1. Since the value calculated theoretically using Bohr’s postulates is exceptionally close to the experimental value, it conclusively demonstrates that Bohr’s atomic model is highly realistic, valid, and accurate.
