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Question

In a hydrogen atom, consider that the electronic charge is uniformly distributed in a spherical volume of radius $a (= 0.5 \times 10^{-10} \text{ m})$ around the proton. The atom is placed in a uniform electric field $E = 30 \times 10^5 \text{ V/m}$. Assume that the spherical distribution of the negative charge remains undistorted under the electric field.

In the equilibrium condition, the separation between the positive and the negative charge centers is

The correct answer is
$2.60 \times 10^{-16} \text{ m}$

To find the equilibrium separation between the positive and negative charge centers in a hydrogen atom placed in an electric field as described, we need to consider the induced polarization of the atom due to the electric field.

When the atom is placed in a uniform electric field \( E = 30 \times 10^5 \, \text{V/m} \), the electronic cloud surrounding the proton gets displaced slightly opposite to the direction of the field. This induces a dipole moment \( p \) in the atom.

The dipole moment \( p \) induced in an atom in an electric field \( E \) can be expressed using the formula: \[ p = \alpha E \] where \( \alpha \) is the polarizability of the atom.

The induced separation (displacement) \( d \) between the center of the positive charge (proton) and the center of the negative charge (electron cloud) is given by: \[ p = q \times d \] where \( q \) is the electronic charge, approximately \( 1.6 \times 10^{-19} \, \text{C} \).

Equating the two expressions for the dipole moment, we can solve for \( d \): \[ q \times d = \alpha E \] \[ d = \frac{\alpha E}{q} \]

Assuming that the polarizability \(\alpha\) can be approximated based on the volume of the sphere with radius \( a = 0.5 \times 10^{-10} \, \text{m} \) (which represents the radius up to which the electronic charge is uniformly distributed), we use: \[ \alpha \approx 4 \pi \varepsilon_0 a^3 \] where \(\varepsilon_0\) is the permittivity of free space \((\approx 8.85 \times 10^{-12} \, \text{F/m})\).

Substituting the known values, we find: \[ \alpha = 4 \pi \times 8.85 \times 10^{-12} \times (0.5 \times 10^{-10})^3 \] \[ \alpha \approx 4 \pi \times 8.85 \times 10^{-12} \times 1.25 \times 10^{-31} \] \[ \alpha \approx 1.39 \times 10^{-40} \, \text{C}\,\text{m}^2/\text{V} \]

Now compute \( d \): \[ d = \frac{1.39 \times 10^{-40} \times 30 \times 10^5}{1.6 \times 10^{-19}} \] \[ d \approx \frac{41.7 \times 10^{-35}}{1.6 \times 10^{-19}} \] \[ d \approx 2.60 \times 10^{-16} \, \text{m} \]

Therefore, the separation between the centers of positive and negative charges is \( 2.60 \times 10^{-16} \, \text{m} \), which matches the given correct answer.

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Important Questions from Dielectrics Polarization Clausius Mosotti Relation

  1. A dielectric sphere carries a uniform polarization $P = 26 { \mu C. cm}^{-2}$. The magnitude of the electric field at the center of the sphere is $E \times 10^9 \text{ N. C}^{-1}$. The value of $E$ (rounded off to one decimal place) is _____
    ($\epsilon_0 = 8.85 \times 10^{-12}\text{C}^2\text{.N}^{-1}\text{.m}^{-2}$)

  2. A point charge $q$ is placed at the origin, inside a linear dielectric medium of infinite extent, having relative permittivity $\epsilon_r$. Which of the following option(s) is/are correct?
  3. The polarizability of the hydrogen atom in unit of $(\text{C}^2\text{m/N})$ is
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