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Exercises · 12.10

Q.In accordance with the Bohr's model, find the quantum number that characterises the earth's revolution around the sun in an orbit of radius 1.5×1011 m1.5 \times 10^{11}\ \text{m} with orbital speed 3×104 m/s3 \times 10^{4}\ \text{m/s}. (Mass of earth =6.0×1024 kg= 6.0 \times 10^{24}\ \text{kg}.)

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Bohr’s angular momentum quantization condition mvr=nℏmvr = n\hbar is applied to Earth’s orbit. Plugging in the given values gives n≈2.6×1074n \approx 2.6 \times 10^{74}, an astronomically large quantum number — showing that classical physics emerges from quantum mechanics for macroscopic systems.

The Bohr model was originally proposed for the hydrogen atom, where the electron’s angular momentum around the nucleus is quantized in integer multiples of ℏ=h/2π\hbar = h/2\pi. The key insight is that this quantization condition — mvr=nℏmvr = n\hbar — is not limited to atoms. It can be applied to any orbiting system, including Earth around the Sun. The result tells us how “quantum” the orbit is: a small nn means the system is truly quantum, while a huge nn (like here) means the orbit behaves classically, because the spacing between adjacent quantum levels becomes vanishingly small.

Let’s work through the numbers step by step.

  1. Write down the quantization condition. Bohr’s postulate for angular momentum is:

mvr=nℏm v r = n \hbar

where mm is the mass of the orbiting body (Earth), vv is its orbital speed, rr is the orbital radius, nn is the quantum number (an integer), and ℏ=h2π\hbar = \frac{h}{2\pi} with h=6.626×10−34 J⋅sh = 6.626 \times 10^{-34}\ \text{J·s}.

  1. Identify the given values.

    • r=1.5×1011 mr = 1.5 \times 10^{11}\ \text{m}
    • v=3×104 m/sv = 3 \times 10^{4}\ \text{m/s}
    • m=6.0×1024 kgm = 6.0 \times 10^{24}\ \text{kg}
    • h=6.626×10−34 J⋅sh = 6.626 \times 10^{-34}\ \text{J·s}, so ℏ=h2π≈1.0546×10−34 J⋅s\hbar = \frac{h}{2\pi} \approx 1.0546 \times 10^{-34}\ \text{J·s}
  2. Calculate the left-hand side: Earth’s angular momentum.

L=mvr=(6.0×1024)×(3×104)×(1.5×1011)L = m v r = (6.0 \times 10^{24}) \times (3 \times 10^{4}) \times (1.5 \times 10^{11})

Multiply stepwise:

6.0×3=186.0 \times 3 = 18, and 1024×104=102810^{24} \times 10^{4} = 10^{28}, so mv=18×1028=1.8×1029 kg⋅m/sm v = 18 \times 10^{28} = 1.8 \times 10^{29}\ \text{kg·m/s}.

Then L=(1.8×1029)×(1.5×1011)=2.7×1040 kg⋅m2/sL = (1.8 \times 10^{29}) \times (1.5 \times 10^{11}) = 2.7 \times 10^{40}\ \text{kg·m}^2/\text{s}.

  1. Solve for nn. From L=nℏL = n \hbar, we have: …

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