Virtual laboratory/Physics/Astrophysics/Cosmic velocities (I and II)

Cosmic velocities (I and II)

To stay in a circular orbit just above the surface, a body must reach the first cosmic velocity v_I=√(GM/R). To escape the gravitational field, it needs the second cosmic velocity v_II=√(2GM/R), which is always √2 times larger than the first. Change the mass and radius of the celestial body.

Cosmic velocities (I and II)
Physics · Astrophysics · Cosmic velocities (FIZ.ASTR)
Mass MM (Earth masses)1.00 M⊕
Radius RR (Earth radii)1.00 R⊕
How many times larger is the escape velocity (II) than the orbital one (I)?
mass M
1.00 M⊕
radius R
1.00 R⊕
v₁ orbital
7.91 km/s
v₂ escape
11.18 km/s
🎯 Challenge: tune MM and RR to hit the escape velocity

What just happened?

You changed the mass of the celestial body — both velocities grew, but the escape velocity stayed exactly 2\sqrt{2} times larger than the orbital one. This ratio does not depend on the planet.

Cosmic velocities:

vI=GMR,vII=2GMR=vI2v_I=\sqrt{\dfrac{GM}{R}}, \quad v_{II}=\sqrt{\dfrac{2GM}{R}}=v_I\sqrt{2}

vIv_I — first cosmic velocity: the minimum speed to stay in a circular orbit just above the surface. vIIv_{II} — second cosmic velocity: the minimum speed to escape the gravitational field entirely. G — gravitational constant, M — mass of the body, R — its radius.

Why do they depend on M and R?

A larger mass M pulls harder → you must travel faster. A larger radius R moves you farther from the centre, weaker gravity at the surface → the velocities drop. For Earth vI≈7.9v_I\approx 7.9 km/s, and vII≈11.2v_{II}\approx 11.2 km/s.

Why is it easier to lift off from the Moon?

The Moon has a small mass and radius, so both velocities are several times smaller than on Earth (vII≈2.4v_{II}\approx 2.4 km/s). That is why the lander needed far less fuel to launch back up. It is the same physics as universal gravitation.

Why you need this for the exam:

The formulas vI=GM/Rv_I=\sqrt{GM/R} and vII=vI2v_{II}=v_I\sqrt{2} solve most problems about satellites and escape. The trick: compute vIv_I, and you get the second velocity by multiplying by 2\sqrt{2}.

Remember: the escape velocity is always 2\sqrt{2} times larger than the orbital one — no matter which planet you launch from.

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Theory & formulas

First cosmic velocity

The smallest horizontal speed for a circular orbit just above the surface — gravity acts as the centripetal force: vI=GMRv_I = \sqrt{\dfrac{GM}{R}}

Second cosmic velocity

The escape velocity from the gravitational field (from the energy balance 12mv2=GMmR\tfrac12 mv^2 = \tfrac{GMm}{R}): vII=2GMR=vI2v_{II} = \sqrt{\dfrac{2GM}{R}} = v_I\sqrt{2} Always 2≈1.41\sqrt{2}\approx1.41 times larger than the first.

For Earth

vI≈7.9 km/sv_I\approx7.9\ \mathrm{km/s}, vII≈11.2 km/sv_{II}\approx11.2\ \mathrm{km/s}. A smaller mass and radius of the body → smaller cosmic velocities.

Symbols: GG — gravitational constant, MM — mass of the body, RR — its radius, vI,vIIv_I,v_{II} — first and second cosmic velocity.

Frequently asked questions

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What is the first cosmic velocity?

The smallest horizontal speed at which a body orbits in a circular path just above the surface (for Earth ≈ 7.9 km/s).

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When does a rocket escape a planet?

When it reaches the second cosmic velocity v_II=√(2GM/R) (for Earth ≈ 11.2 km/s) — then it overcomes the gravitational field.

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Why is it easier to lift off from the Moon?

Because the Moon has a much smaller mass and radius than Earth, so its cosmic velocities are much smaller.

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