Escape Velocity (College Board AP® Physics 1: Algebra-Based)

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Katie M

Written by: Katie M

Reviewed by: Caroline Carroll

Escape velocity

  • To escape the gravitational field of a central body, a satellite must travel at, or above, a minimum escape velocity

    • This is dependent on the mass and radius of the central body creating the gravitational field

    • Examples of central bodies include planets, moons, or even black holes

  • Escape velocity is defined as:

The minimum velocity that will allow an object to escape a gravitational field with no further energy input

  • The escape velocity of a satellite is such that the mechanical energy of the satellite–central-object system is equal to zero

  • If a satellite reaches escape velocity, it will:

    • move away from the central body

    • have a velocity of zero at an infinite distance from the central body

  • This is assuming that the only force exerted on the satellite is the gravitational attraction of the central object

Escape velocity of the Earth

A rocket leaving Earth's gravitational field, achieving escape velocity. Earth and the Moon are shown, with comets nearby. Labels include mass (M, m) and distance (r).
For a rocket to leave the Earth's gravitational field entirely, it would have to travel at a speed equal to or greater than the Earth's escape velocity
  • Rockets launched from the Earth's surface do not need to achieve escape velocity to reach an orbit

    • This is because the orbit would still be within Earth's gravitational field

    • Therefore, less work would be required to move to this position than to escape the Earth's gravitational field entirely

Derived equation

  • The escape velocity of a satellite from a central body of mass M is:

v subscript e s c end subscript space equals space square root of fraction numerator 2 G M over denominator r end fraction end root

  • This equation can be derived using energy conservation laws

Step 1: Identify the fundamental equations

  • The kinetic energy K of a satellite is:

K space equals space 1 half m v subscript e s c end subscript squared

  • The gravitational potential energy U subscript g of a satellite is:

U subscript g space equals space minus G fraction numerator M m over denominator r end fraction

  • Where:

    • m = mass of the satellite, in kg

    • v subscript e s c end subscript = escape velocity of the satellite, in straight m divided by straight s

    • G = Universal gravitational constant open parentheses 6.67 cross times 10 to the power of negative 11 end exponent space straight N times straight m squared divided by kg squared close parentheses

    • M = mass of the central object, in kg

    • r = distance between the satellite and the center of the central object, in straight m

Step 2: Apply the specific conditions

  • The escape speed of a satellite is the speed at which all its kinetic energy has been transferred to gravitational potential energy

K space equals space U subscript g

1 half m v subscript e s c end subscript squared space equals space fraction numerator G M m over denominator r end fraction

  • Since mass m is the same on both sides of the equation, it cancels out:

1 half v subscript e s c end subscript squared space equals space fraction numerator G M over denominator r end fraction

  • Multiplying both sides by 2 and taking the square root gives the following equation:

v subscript e s c end subscript space equals space square root of fraction numerator 2 G M over denominator r end fraction end root

  • This equation shows that escape velocity is the same for all masses occupying the same gravitational field

    • For example, on Earth, the value of escape velocity is the same for both a satellite and a tennis ball

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Katie M

Author: Katie M

Expertise: Physics

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.

Caroline Carroll

Author: Caroline Carroll

Expertise: Physics Subject Lead

Caroline graduated from the University of Nottingham with a degree in Chemistry and Molecular Physics. She spent several years working as an Industrial Chemist in the automotive industry before retraining to teach. Caroline has over 12 years of experience teaching GCSE and A-level chemistry and physics. She is passionate about creating high-quality resources to help students achieve their full potential.