Available energy (particle collision)

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For a discussion about the meaning of the term in classical thermodynamics, see Exergy.

In particle physics, the available energy is the energy in a particle collision available to produce new matter from the kinetic energy of the colliding particles. Since the conservation of momentum must be held, a system of two particles with a net momentum may not convert all their kinetic energy into mass - and thus the available energy is always less than or equal to the kinetic energy of the colliding particles. The available energy for a system of one stationary particle and one moving particle is defined as:

 E_a = \sqrt{2 E_t E_k + (m_t c^2)^2 + (m_k c^2)^2}

where

 E_t is the total energy of the target particle,
 E_k is the total energy of the moving particle,
 m_t is the mass of the stationary target particle,
 m_k is the mass of the moving particle, and
 c is the speed of light.

Derivation[edit]

This derivation will use the fact that:

 (mc^2)^2 = E^2-P^2c^2

From the principle of the conservation of linear momentum:

 P_a = P_k

Where  P_a  and  P_k  are the momentums of the created and the initially moving particle respectively. From the conservation of energy:

 E_T= E_t+E_k

Where  E_T  is the total energy of the created particle. We know that after the collision:

 (E_a)^2=(E_T)^2-(P_a)^2 c^2
 (E_a)^2=(E_t+E_k)^2-(P_k)^2 c^2
 (E_a)^2=(E_t)^2 +(E_k)^2 + 2 E_t E_k-(P_k)^2 c^2

Donating this last equation (1). But

 (m_k)^2 c^4=(E_k)^2-(P_k)^2 c^2

and since the stationary particle has no momentum

 (m_t)^2 c^4=(E_t)^2

Therefore from (1) we have

 (E_a)^2=(m_k)^2 c^4+(m_t)^2 c^4 + 2 E_t E_k

Square rooting both sides and we get

 E_a = \sqrt{ (m_t c^2)^2 + (m_k c^2)^2+2 E_t E_k}

See also[edit]

References[edit]

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