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PLZ ANSWER 2 MY QUES..

passage..

Although Neils Bohr `s atom model is supposed to b based on non-relativistic theory, rearranging the formula for energy, one finds dat

En= - Z/n2[1/2mc2.a2] where alpha is fine srtucture constant and mc2 is the relativistic energy.

a(ie..alpha) =

Ques. Assuming dat the kinetic energy is half the potential energy of orbiting electron, the velo of the e on 1st orbit of hydrogen atom is

a)137c b)/137

c)(c/2)137

plz solve this toooo...

Which of the following statements will be true in light of above ques.

a)This is a non relativisticc energy region and hence relativistic correction is not necessary.

b)alpha is to be relativistically corrected

c) m0c2 used in the formula shud b corrected to mc2.realtivistic correction is 4 mass.

Kevin Nash , 12 Years ago
Grade upto college level
anser 1 Answers
Askiitians Tutor Team

To tackle your question about the energy of an electron in the hydrogen atom and the implications of relativistic corrections, let's break it down step by step. We’ll start by analyzing the given information and then derive the velocity of the electron in the first orbit of a hydrogen atom.

Understanding the Energy Relationships

In the Bohr model of the hydrogen atom, the total energy (E) of the electron in orbit can be expressed as the sum of its kinetic energy (K) and potential energy (U). The relationship you mentioned states that the kinetic energy is half of the potential energy:

  • K = 1/2 U

For an electron in a circular orbit, the potential energy (U) is given by:

  • U = - (k * e^2) / r

Where:

  • k is Coulomb's constant,
  • e is the charge of the electron, and
  • r is the radius of the orbit.

The kinetic energy (K) can be expressed as:

  • K = (1/2) m v^2

Relating Kinetic and Potential Energy

From the relationship K = 1/2 U, we can substitute U into this equation:

  • 1/2 m v^2 = - (1/2) (k * e^2) / r

From this, we can derive the velocity of the electron. In the Bohr model, the radius of the first orbit (n=1) is given by:

  • r = (4 * π * ε₀ * h^2) / (m * e^2)

Calculating the Velocity

Now, we can express the velocity (v) of the electron in the first orbit. Using the relationship between kinetic and potential energy, we can derive:

  • v = sqrt(k * e^2 / (m * r))

Substituting the expression for r gives us:

  • v = sqrt((k * e^2 * m * e^2) / (4 * π * ε₀ * h^2))

Now, using the fine structure constant (α), we can express this velocity in terms of the speed of light (c). The fine structure constant is defined as:

  • α = (k * e^2) / (ħ * c)

After some algebra, we find that the velocity of the electron in the first orbit can be approximated as:

  • v ≈ (α * c)

Choosing the Correct Option

Now, let's analyze the options provided in your question regarding the velocity:

  • a) 137c
  • b) (1/137)c
  • c) (c/2) * 137

Since we derived that the velocity is approximately (α * c), and α is about 1/137, the correct answer is:

  • **b) (1/137)c**

Evaluating the Statements

Now, let’s evaluate the statements regarding relativistic corrections:

  • a) This is a non-relativistic energy region and hence relativistic correction is not necessary.
  • b) α is to be relativistically corrected.
  • c) m₀c² used in the formula should be corrected to mc². Relativistic correction is for mass.

Given that the velocity we calculated is a fraction of the speed of light, we are indeed in a non-relativistic regime for the hydrogen atom. Therefore:

  • The first statement (a) is true. Relativistic effects are negligible at this speed.
  • The second statement (b) is not necessary since α is already defined in a way that incorporates relativistic effects.
  • The third statement (c) is also not applicable here since we are not dealing with significant relativistic speeds.

In summary, the velocity of the electron in the first orbit of the hydrogen atom is approximately (1/137)c, and the correct interpretation of the energy region indicates that relativistic corrections are not necessary in this case.

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