Gravitation

Physics · Class 11

Lesson 9 of 11 · 10 min

Earth satellites

NCERT §7.9

On clear evenings Kavya sometimes sees a bright steady dot glide across the sky in a few minutes and fade out: the International Space Station, about 400 km up. It goes round the earth in about an hour and a half. What keeps it up?

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In short

A satellite is a body that revolves around the earth; Kepler's laws apply to it just as to planets around the sun. The Moon is the earth's only natural satellite, with a period of about 27.3 days.

For a circular orbit of radius R_E + h, gravity supplies the centripetal force: m v²/(R_E + h) = G M_E m / (R_E + h)², so v = √(G M_E / (R_E + h)), less for higher orbits.

Just above the surface (h ≈ 0) the orbital speed is v = √(g R_E) ≈ 7.9 km/s, and the escape speed is √2 times this.

Period: T = 2π (R_E + h)^(3/2) / √(G M_E), so T² = k (R_E + h)³ with k = 4π²/(G M_E). This is Kepler's third law for satellites.

For an orbit just above the surface, T₀ = 2π √(R_E/g) ≈ 85 minutes.

The same law weighs other planets. Phobos circles Mars in 7 h 39 min at 9.4 × 10³ km, which gives a Mars mass of about 6.48 × 10²³ kg; with its orbit 1.52 times the earth's, a Martian year is (1.52)^(3/2) × 365 ≈ 684 days.

An astronaut in orbit feels weightless not because gravity is small there, but because the astronaut and the craft are falling freely towards the earth together.

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Orbital speed and period derived

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Earth satellites | Gravitation | Lumi Learn