Question:

Theratio of the magnitude of the kinetic energy to the potential energy of an electron in the 5th excited state of a hydrogen atom is:

Updated On: Nov 3, 2025
  • 4
  • \( \frac{1}{4} \)
  • \(\frac{1}{2}\)
  • 1
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The Correct Option is C

Approach Solution - 1

The problem asks for the ratio of the magnitude of the kinetic energy to the potential energy of an electron in the 5th excited state of a hydrogen atom.

Concept Used:

In the Bohr model of the hydrogen atom, the total energy of an electron in the \(n^{th}\) orbit is the sum of its kinetic energy (K.E.) and potential energy (P.E.). The relationships between these energies are derived from the balance between the electrostatic force and the centripetal force.

The centripetal force required for circular motion is provided by the electrostatic attraction between the nucleus and the electron:

\[ \frac{mv^2}{r} = \frac{1}{4\pi\epsilon_0} \frac{e^2}{r^2} \]

From this, we can derive the expressions for K.E. and P.E.:

Kinetic Energy (K.E.):

\[ K.E. = \frac{1}{2}mv^2 = \frac{1}{8\pi\epsilon_0} \frac{e^2}{r} \]

Potential Energy (P.E.):

\[ P.E. = -\frac{1}{4\pi\epsilon_0} \frac{e^2}{r} \]

By comparing the expressions, we can establish a direct relationship between K.E. and P.E.:

\[ P.E. = -2 \times (K.E.) \]

This relationship is valid for any orbit \(n\).

Step-by-Step Solution:

Step 1: Write down the standard expressions for the kinetic energy (K.E.) and potential energy (P.E.) of an electron in any orbit \(n\) of a hydrogen atom.

The kinetic energy is given by:

\[ K.E. = \frac{1}{2}mv^2 \]

From the force balance equation, \(mv^2 = \frac{e^2}{4\pi\epsilon_0 r}\), so:

\[ K.E. = \frac{e^2}{8\pi\epsilon_0 r} \]

The electrostatic potential energy is given by:

\[ P.E. = -\frac{e^2}{4\pi\epsilon_0 r} \]

Step 2: Find the magnitude of the potential energy, \(|P.E.|\).

\[ |P.E.| = \left| -\frac{e^2}{4\pi\epsilon_0 r} \right| = \frac{e^2}{4\pi\epsilon_0 r} \]

Step 3: Form the ratio of the magnitude of the kinetic energy to the magnitude of the potential energy.

The kinetic energy is always positive, so its magnitude is just K.E. The required ratio is:

\[ \frac{K.E.}{|P.E.|} = \frac{\frac{e^2}{8\pi\epsilon_0 r}}{\frac{e^2}{4\pi\epsilon_0 r}} \]

Step 4: Simplify the expression for the ratio.

The common terms \( \frac{e^2}{4\pi\epsilon_0 r} \) cancel out:

\[ \frac{K.E.}{|P.E.|} = \frac{1/2}{1} = \frac{1}{2} \]

This shows that the ratio of the kinetic energy to the magnitude of the potential energy is constant for any energy level of the hydrogen atom. The fact that the electron is in the 5th excited state (which corresponds to the principal quantum number \(n=6\)) does not change this fundamental ratio.

Final Computation & Result:

The ratio is calculated as:

\[ \frac{\text{Magnitude of Kinetic Energy}}{\text{Magnitude of Potential Energy}} = \frac{K.E.}{|P.E.|} = \frac{1}{2} \]

The ratio is 1:2.

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Approach Solution -2

For an electron in a hydrogen atom (Bohr model):

\[ |PE| = 2 \times KE \]

So,

\[ \frac{KE}{|PE|} = \frac{1}{2} \]

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Concepts Used:

Bohr's Model of Hydrogen Atom

Niels Bohr introduced the atomic Hydrogen model in 1913. He described it as a positively charged nucleus, comprised of protons and neutrons, surrounded by a negatively charged electron cloud. In the model, electrons orbit the nucleus in atomic shells. The atom is held together by electrostatic forces between the positive nucleus and negative surroundings.

Read More: Bohr's Model of Hydrogen Atom

Bohr's Theory of Hydrogen Atom and Hydrogen-like Atoms

A hydrogen-like atom consists of a tiny positively-charged nucleus and an electron revolving around the nucleus in a stable circular orbit. 

Bohr's Radius: 

If 'e,' 'm,' and 'v' be the charge, mass, and velocity of the electron respectively, 'r' be the radius of the orbit, and Z be the atomic number, the equation for the radii of the permitted orbits is given by r = n2 xr1, where 'n' is the principal quantum number, and r1 is the least allowed radius for a hydrogen atom, known as Bohr's radius having a value of 0.53 Å. 

Limitations of the Bohr Model

The Bohr Model was an important step in the development of atomic theory. However, it has several limitations.

  1. Bohr’s model of the atom failed to explain the Zeeman Effect (effect of magnetic field on the spectra of atoms).
  2. It failed to explain the Stark effect (effect of electric field on the spectra of atoms).
  3. The spectra obtained from larger atoms weren’t explained.
  4. It violates the Heisenberg Uncertainty Principle.