Sigma Percentile
JEE Main 2021
LEVELJEE Main

Animated Solution for Chemistry - Atomic Structure: The kinetic energy of an electron in the second Bohr orbit of a hydrogen atom is equal to . The value of is ……… . ( is radius of Bohr's orbit) (Nearest integer) [Given, ]

Enter Numerical Value:

Visualized Solution

  • \text{Hydrogen atom, } Z=1
  • \text{Second Bohr orbit, } n=2

  • mvr = \frac{nh}{2\pi}

  • v = \frac{nh}{2\pi mr}

  • KE = \frac{1}{2}mv^2

  • KE = \frac{1}{2}m \left(\frac{nh}{2\pi mr}\right)^2
  • KE = \frac{n^2h^2}{8\pi^2mr^2}

  • r = a_0 \frac{n^2}{Z}
  • \text{For H atom, } Z=1
  • \text{For 2nd orbit, } n=2
  • r = a_0 \frac{2^2}{1} = 4a_0

  • KE = \frac{(2)^2 h^2}{8\pi^2m(4a_0)^2}

  • KE = \frac{4h^2}{8\pi^2m(16a_0^2)}
  • KE = \frac{h^2}{32\pi^2ma_0^2}

  • \text{Given: } KE = \frac{h^2}{xma_0^2}
  • \therefore x = 32\pi^2
  • 10x = 320\pi^2
  • 10x = 320 \times (3.14)^2
  • 10x = 3155.072 \approx 3155

\text{Energy Relations}

  • TE = -KE
  • PE = -2KE

The Sigma Insight: Bohr's Model

Solution Diagram

Visualizing the Bohr Atom

Imagine you are looking at a hydrogen atom. At the center, we have the positively charged nucleus. Revolving around it in the second orbit, where , is our electron. This is the classic Bohr model setup, and it provides a beautiful, semi-classical way to understand atomic energy levels.

The Quantization of Angular Momentum

According to Bohr's famous postulate, the angular momentum of this revolving electron is not arbitrary; it is strictly quantized. It must be an integral multiple of . This gives us our first master equation:
From this equation, we can easily isolate the velocity . We just move the mass and the radius to the denominator on the right side. This gives us the velocity of the electron purely in terms of its orbit radius:

Deriving the Kinetic Energy

Now, the question asks for the kinetic energy of this electron. We know the classic formula for kinetic energy is:
Let's substitute our expression for velocity into the kinetic energy formula. Squaring the terms inside the bracket gives us . Multiplying by simplifies it beautifully:

The Bohr Radius Connection

We need our final answer in terms of the Bohr radius, . Remember, the radius of the -th orbit is given by the formula:
For a hydrogen atom, the atomic number is , and here we are dealing with the second orbit, so is . Therefore, the radius is simply:

The Final Calculation

Now, let's bring it all together. We substitute and back into our kinetic energy equation.
Let's simplify this carefully. Squaring gives . The in the numerator cancels partially with the in the denominator, leaving a . Two times sixteen is thirty-two. So we get:
Comparing our result with the given expression , we can clearly see that is exactly .
The question asks for the value of . Multiplying by ten and substituting , we get:
Rounding to the nearest integer, our final answer is 3155.

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Comprehension Passage

Consider the Bohr's model of a one-electron atom where the electron moves around the nucleus. In the following List-I contains some quantities for the orbit of the atom and List-II contains options showing how they depend on . \begin{array}{ll} \textbf{List-I} & \textbf{List-II} \\ \text{(I) Radius of the } n^{\text{th}} \text{ orbit} & \text{(P) } \propto n^{-2} \\ \text{(II) Angular momentum of the electron in the } n^{\text{th}} \text{ orbit} & \text{(Q) } \propto n^{-1} \\ \text{(III) Kinetic energy of the electron in the } n^{\text{th}} \text{ orbit} & \text{(R) } \propto n^0 \\ \text{(IV) Potential energy of the electron in the } n^{\text{th}} \text{ orbit} & \text{(S) } \propto n^1 \\ & \text{(T) } \propto n^2 \\ & \text{(U) } \propto n^{1/2} \end{array}
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