Problem 6.24 — Bohr Orbital Periods

Problem Statement

Solve the gravitation problem: Solve the gravitation problem: Find orbital periods for $n=1,2,3$ in hydrogen and compare to classical emission frequency. $T_n = 2\pi r_n/v_n = 2\pi n^3a_0/v_1 = n^3T_1$ $$T_1 = 2\pi a_0/v_1 = 2\pi\times0.529\times10^{-10}/2.19\times10^6 = 1.52\times10^{-16} \text{ s}$$ $T_1 = 1.52\times10^{-16}$ s

Given Information

  • Masses $M$ (planet/star) and $m$ (object/satellite)
  • Orbital radius $r$ or altitude $h$
  • $G = 6.674\times10^{-11}\,\text{N m}^2\text{kg}^{-2}$

Physical Concepts & Formulas

Newton’s Law of Universal Gravitation $F = GMm/r^2$ states that every mass attracts every other mass. For circular orbits, gravity provides the centripetal force: $GMm/r^2 = mv^2/r$, giving orbital speed $v = \sqrt{GM/r}$ — independent of the satellite’s mass. Kepler’s third law $T^2 \propto r^3$ follows directly. Escape velocity is found by setting kinetic energy equal to gravitational PE: $v_e = \sqrt{2GM/R}$. Inside a uniform sphere, $g$ decreases linearly with depth.

  • $F = \dfrac{GMm}{r^2}$ — Newton’s Law of Gravitation
  • $v_{\text{orbit}} = \sqrt{GM/r}$ — circular orbital speed
  • $T = 2\pi\sqrt{r^3/GM}$ — orbital period (Kepler III)
  • $v_e = \sqrt{2GM/R}$ — escape velocity from surface
  • $g = GM/R^2$ — surface gravitational acceleration

Step-by-Step Solution

Step 1 — Centripetal force = Gravitational force:

$$\frac{mv^2}{r} = \frac{GMm}{r^2} \implies v = \sqrt{\frac{GM}{r}}$$

Step 2 — Period:

$$T = \frac{2\pi r}{v} = \frac{2\pi r}{\sqrt{GM/r}} = 2\pi\sqrt{\frac{r^3}{GM}}$$

Step 3 — Escape velocity (set $KE = PE$):

$$\frac{1}{2}mv_e^2 = \frac{GMm}{R} \implies v_e = \sqrt{\frac{2GM}{R}}$$

Worked Calculation

Substituting all values with units:

Earth: $M = 5.97\times10^{24}\,\text{kg}$, $R = 6.37\times10^6\,\text{m}$:

$$v_e = \sqrt{\frac{2\times6.674\times10^{-11}\times5.97\times10^{24}}{6.37\times10^6}} = \sqrt{\frac{7.97\times10^{14}}{6.37\times10^6}} = \sqrt{1.25\times10^8} \approx 11.2\,\text{km/s}$$

Answer

$$\boxed{v_e = \sqrt{2GM/R} \approx 11.2\,\text{km/s}}$$

Physical Interpretation

11.2 km/s ≈ 40,000 km/h is the escape speed from Earth. The Moon’s escape speed is 2.38 km/s — much lower because of its smaller mass. That is why the Moon has no atmosphere: thermal gas molecules at the Moon’s surface easily exceed this speed. Rockets do not need to reach escape velocity instantly — they can use continuous thrust, effectively integrating the Tsiolkovsky equation.


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