The Coulomb Acceleration in Bohr’s Model of the Hydrogen Atom
Coulomb's
law states that the electrical force between two charged objects is directly
proportional to the product of the quantity of charge on the objects and
inversely proportional to the square of the separation distance between the two
objects. Mathematically, this law can be stated as
FC = keq1q2/R2 … (1)
where ke is the Coulomb constant (= 8,988 × 109 N m2 C-2)[1], q1 is the charge of the first object, q2 is the charge of another object and R is the distance between these objects. FE is the electrostatic force.
We will apply the expression (1) in the case of the proton and electron of the hydrogen atom. The proton has a positive charge equal in magnitude to a unit of electron charge e (= 1.60 × 10-19 C). In the ground state of hydrogen atom, its Bohr radius a0 = 5.3 × 10-11 m.
The Coulomb force of hydrogen atom is attractive and can cause the electron to deflect from a straight-line path to a circular path (Bohr’s orbit) around the proton. We assume that the electron moves one-dimensionally along the line joining them and that it directly reaches Bohr’s radius without any deflection from a straight-line path.
The Coulombic force FC between these two charges is at a distance R would be
FC = kee2/R2.
According
to Newton’s second law of motion, the acceleration of the electron at R would
be equal to the Coulombic force divided by the rest mass of electron me
(= 9.11 × 10-31 kg). This can be represented
by the equation
aC = (FC/me) = kee2/meR2 … (2).
An electron at a distance from the proton equal to Bohr’s radius a0 (= 5.3 × 10-11 m)[1] would reach an acceleration of about 1030 m sec-2 [by employing eqn. (2)]. With this average acceleration the electron would reach the speed of light c (= 299792 km sec-1 ≈ 3 × 105 km sec-1) for Δt ≈ 3 × 10-22 sec.
The quantum
mechanical expression for the energy-time uncertainty is
ΔEΔt ≈ h … (3).
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