Kinetic Energy

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Kinetic energy represents the energy associated with the motion of an object.[1] It is defined as the work done by a force to accelerate that object from rest to some speed , in the absence of any other forces acting upon the object. Kinetic energy is a scalar and has the same units as work (i.e. Joule).

Classical mechanics

Translational kinetic energy

In classical mechanics, the translational kinetic energy of a ridid object,  , can be found as:

 

Where

  is the mass of the object
  is the velocity of the object

Rotational kinetic energy

The rotational kinetic energy of a rigid object is:

 

Where

  is the moment of inertia of the object
  is the angular velocity of the object

Work-Energy theorem

The change of kinetic energy is equal to the total work done on it by the resultant of all forces acting on it. For a point mass this can be expressed as:

 

Where

  is the initial speed
  is the final speed

Note that if the mass of an object is increased, the increase in kinetic energy increases linearly; if the velocity of an object is increased, the increase in kinetic energy increases quadratically. For example, doubling the mass of an object doubles its kinetic energy; doubling its velocity quadruples its kinetic energy.

Derivation of translational kinetic energy

The work done by a force accelerating an object from rest, which is the kinetic energy is:

 

From Newton's second law, the force,  , is  . Hence we can make the substitution and use the chain rule

 

This is the same as

 

In classical mechanics, momentum is given by  . Differentiating and substituting into the above equation results in

 

We want to integrate between 0 and the speed of the object,   as this defines kinetic energy. Performing the integration reveals that the kinetic energy is, as expected, the following:

 

A similar method may be used to derive the formula for rotational kinetic energy.

Kinetic Energy in Relativity

In relativity, kinetic energy can be expressed as:

 

where

  is the Lorentz factor
  is the rest mass
  is the speed of light

This can be shown to be equivalent to the classical equation for kinetic energy,  , by performing a binomial expansion on it. Using the result:

 

Expanding the Lorentz factor in this way, we see:

 

This simplifies to

 

For speeds encountered everyday, which are a lot less than that of [[speed of light|light] (such that  ), all terms apart from the first are very small and can be neglected. Hence, the formula reduces to:

 

which is the classical formula.

Derivation

The kinetic energy is the work done accelerating a particle from rest to some speed Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v} . Suppose the particle is at rest at Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x_1} and speed Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v} at position Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x_2} . Hence:

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle K = \int^{x_2}_{x_1} \vec{F} \dot d \vec{x}}

Since Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \vec{F} = \vec{F}_{\perp} + \vec{F}_{\parallel}} , and a perpendicular force does no work, we can ignore the perpendicular component and write:

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle K = \int^{x_2}_{x_1} F_{\parallel} dx = \int^{x_2}_{x_1} \gamma^3 m_0 a dx}

Since Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle a \, dx = \frac{dv_{\parallel}}{dt} dx = \frac{dx}{dt} dv} , we find the integral can be rewritten as:

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle K = \int^{v_2}_{v_1} \frac{mv}{(1- \frac{v^2}{c^2})} dv}

where Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v_1} is the initial speed and hence 0 by definition and Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle v_2} is the final speed.

Performing the integration reveals the kinetic energy as:

Failed to parse (MathML with SVG or PNG fallback (recommended for modern browsers and accessibility tools): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle K=(\gamma -1)m_0 c^2}

References

  1. ↑ Serway and Beichner, Physics for Scientists and Engineers, Fifth Edition