Speed at Infinity When Launched Above Escape Velocity

Physics · Gravitation · NEET

If a body is launched with speed u that is greater than the escape velocity ve, it does not fall back and still has left-over speed when it reaches infinity. That leftover speed is v(inf) = sqrt(u^2 - ve^2). Memory hook: escape velocity is the "toll" the body pays to leave Earth; whatever kinetic energy is left after paying the toll becomes the speed at infinity.
Earthlaunch u > vedistance from Earth increasesinfinityv(inf) = sqrt(u^2 - ve^2)Energy: (1/2)u^2 = (1/2)ve^2 + (1/2)v(inf)^2leftover speed never reaches zero when u > ve
A body launched at u greater than escape velocity ve keeps a leftover speed v(inf) = sqrt(u^2 - ve^2) at infinity; energy conservation shows the launch KE minus the escape KE equals the KE remaining far away.

Your doubts, answered

If a body is thrown at exactly escape velocity, what is its speed at infinity?

Exactly zero. Escape velocity ve is defined as the minimum speed for which the body just reaches infinity with zero speed. Put u = ve into v(inf) = sqrt(u^2 - ve^2) and you get sqrt(0) = 0. The body escapes but arrives at infinity with no speed left. Only when u is greater than ve does it arrive with a real, non-zero speed.

Why is the speed at infinity NOT simply u - ve?

Because energy adds as the square of speed (KE = (1/2)mv^2), not linearly. Conservation of energy gives (1/2)u^2 = (1/2)ve^2 + (1/2)v(inf)^2, so the SQUARES subtract: v(inf)^2 = u^2 - ve^2. If u = 2ve, the answer is sqrt(4-1)*ve = sqrt(3)*ve, which is about 1.73 ve, not (2-1) = 1 ve. Subtracting the plain speeds is the most common mistake.

What is the difference between escape velocity and velocity at infinity?

Escape velocity ve is the launch speed you need at Earth's surface to just barely escape (about 11.2 km/s). Velocity at infinity v(inf) is the speed that is actually LEFT OVER when the body is very far away, after gravity has done negative work on it all the way out. If you launch at exactly ve, v(inf) = 0. If you launch above ve, v(inf) is positive.

Does the body keep moving at infinity or does it slow to a stop?

When u is greater than ve, the total energy is positive, so the body never stops. It keeps slowing as it climbs, but its speed approaches a fixed non-zero value v(inf) = sqrt(u^2 - ve^2). It coasts away forever at that speed. Only for u equal to or below ve does gravity eventually win.

⚠️ The NEET trap
For u = 2ve, students write v(inf) = 2ve - ve = ve = 11.2 km/s (option A).
Energy conserves, so the squares subtract: v(inf)^2 = u^2 - ve^2 = (2ve)^2 - ve^2 = 3ve^2, giving v(inf) = sqrt(3)*11.2 = 11.2*sqrt(3) km/s.
🧠 Never subtract the speeds directly. Kinetic energy uses v^2, so always subtract the SQUARES first, then take the square root.

Real NEET questions

NEET 2023

The escape velocity of a body from the earth's surface is 11.2 km/s. If the same body is projected upward with velocity 22.4 km/s, its velocity at infinite distance from the centre of the earth will be:

A · 11.2 km/s
B · 11.2 sqrt(3) km/s
C · 11.2 sqrt(2) km/s
D · Zero
Solution: Use energy conservation with PE = 0 at infinity. At the surface: (1/2)m u^2 - (1/2)m ve^2 = (1/2)m v(inf)^2 (the -(1/2)ve^2 term is the gravitational PE at the surface written as an escape term). Here u = 22.4 = 2 ve and ve = 11.2 km/s. So v(inf)^2 = u^2 - ve^2 = (2ve)^2 - ve^2 = 4ve^2 - ve^2 = 3 ve^2. Taking the square root: v(inf) = sqrt(3) * ve = 11.2 * sqrt(3) km/s. This matches option B. The trap answer 11.2 km/s comes from wrongly doing 22.4 - 11.2.

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Frequently asked

What is the formula for velocity at infinity above escape velocity?

v(inf) = sqrt(u^2 - ve^2), where u is the launch speed at Earth's surface and ve is the escape velocity (about 11.2 km/s). It is valid only when u is greater than ve.

If projected with 3 times escape velocity, what is the speed at infinity?

v(inf)^2 = (3ve)^2 - ve^2 = 9ve^2 - ve^2 = 8ve^2, so v(inf) = sqrt(8)*ve = 2*sqrt(2)*ve, which is about 2.83 times the escape velocity.

Why does escape velocity get subtracted as a square?

Energy conservation is written in terms of kinetic energy (1/2)mv^2, which depends on v^2. The launch KE splits into the KE spent escaping (linked to ve^2) and the leftover KE at infinity (linked to v(inf)^2), so the squares subtract.

Does the answer depend on the mass of the body?

No. The mass m cancels from every term in the energy equation, so v(inf) depends only on u and ve, not on how heavy the body is.

Is this the same as the maximum height problem?

They use the same energy equation, but here u is greater than ve so the body never comes back (there is no maximum height, only a leftover speed). Below ve, the body stops at a finite maximum height instead.