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In the Thomson model of hydrogen atom, the nuclear charge is distributed uniformly over a sphere of radius R. The average potential energy of an electron confined within this atom can be taken as V = - (e ^ 2)/(4pi*epsilon_{0}*R) Taking the uncertainty in position to be the radius of the atom, the minimum value of R for which an electron will be confined within the atom is estimated to be f * 10 ^ - 11 m. The value of f is?
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In the Thomson model of hydrogen atom, the nuclear charge is distribut...
Thomson Model of Hydrogen Atom

The Thomson model of the hydrogen atom, proposed by J.J. Thomson in 1904, assumes that the nuclear charge is uniformly distributed over a sphere of radius R. In this model, the electron orbits around the nucleus without any consideration of quantum mechanics.

Average Potential Energy of an Electron

The average potential energy of an electron confined within the Thomson model of the hydrogen atom can be given by the equation:

V = - (e^2) / (4πε₀R)

Where:
- V is the average potential energy of the electron
- e is the elementary charge
- ε₀ is the vacuum permittivity
- R is the radius of the sphere representing the atom

Minimum Value of R for Electron Confinement

To estimate the minimum value of R for which an electron will be confined within the atom, we can consider the uncertainty principle. According to the uncertainty principle, there is a fundamental limit to the precision with which certain pairs of physical properties of a particle, such as position and momentum, can be known simultaneously.

In this case, we can consider the uncertainty in position to be equal to the radius of the atom. Therefore, we have:

Δx ≈ R

From the uncertainty principle, we know that the uncertainty in position (Δx) and the uncertainty in momentum (Δp) are related by the equation:

Δx * Δp ≥ h/ (4π)

Where:
- Δp is the uncertainty in momentum
- h is the Planck's constant

Since we are considering the uncertainty in position to be equal to R, we can rewrite the equation as:

R * Δp ≥ h/ (4π)

To estimate the minimum value of R, we need to determine the minimum value of Δp. According to de Broglie's hypothesis, the momentum of a particle can be related to its wavelength (λ) by the equation:

p = h/λ

Therefore, we can rewrite the inequality as:

R * h/λ ≥ h/ (4π)

Rearranging the equation, we get:

λ ≤ 4πR

Since we are considering the hydrogen atom, the wavelength of the electron can be related to its energy (E) using the equation:

λ = h / √ (2πmE)

Where:
- m is the mass of the electron

Substituting this in the inequality, we get:

h / √ (2πmE) ≤ 4πR

Simplifying the equation, we get:

E ≥ (h^2) / (32π^3mR^2)

The minimum value of R occurs when the energy is at its minimum value, which is the ground state energy of the hydrogen atom. Therefore, we can rewrite the equation as:

E₀ = (h^2) / (32π^3mR₀^2)

Where:
- E₀ is the ground state energy of the hydrogen atom
- R₀ is the minimum value of R for electron confinement

Comparing this equation with the equation for the average potential energy (V), we get:

V = - (e^2) / (4πε₀R)

E₀ = - V

Equating these two equations, we get:

(e^2) / (4πε₀R₀
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In the Thomson model of hydrogen atom, the nuclear charge is distributed uniformly over a sphere of radius R. The average potential energy of an electron confined within this atom can be taken as V = - (e ^ 2)/(4pi*epsilon_{0}*R) Taking the uncertainty in position to be the radius of the atom, the minimum value of R for which an electron will be confined within the atom is estimated to be f * 10 ^ - 11 m. The value of f is?
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