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    Special Relativity: Dynamics

    Physics

    • Title Home
    • Study Guide
    • Topics
      • Introduction to Relativistic Dynamics
      • Energy and Momentum
      • Problems on Energy and Momentum
      • Four-vectors
      • Problems on Four-vectors
      • Force and Acceleration
      • Problems on Forces and Acceleration
    • Terms and Formulae for Relativistic Dynamics

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    Special Relativity: Dynamics Terms and Formulae for Relativistic Dynamics

    Terms and Formulae for Relativistic Dynamics

    Special Relativity: Dynamics Terms and Formulae for Relativistic Dynamics

      Terms

    • Relativistic energy

      In Special Relativity the concept of total energy in the absence of a potential E = 1/2mv2 is replaced with another conserved quantity E = γmc2, where m is the mass or rest mass of the object. This quantity is conserved in all collisions and decays. Where there is a potential involved it is the total energy γmc2 + V which is conserved. Notice that an object at rest still has an amount of energy proportional to its mass Ev=0 = mc2.

    • Relativistic momentum

      The quantity that is conserved in all collisions in relativity is not p = mv but p = γmv. This is called the relativistic momentum. When v < < c then γ 1 and pmv.

    • 4-vector

      A vector with four components that, under a Lorentz transformation, transforms as (cdt, dx, dy, dz) does. That is, for A = (A0, A1, A2, A3) the 4-vector in another frame must be:


      A0 = γ(A0' + (v/c)A1')    
      A1 = γ(A1' + (v/c)A0')    
      A2 = A2'    
      A3 = A3'    

      Only those vectors for which the result of the above transformation is equal to the transformation of the individual coordinates under the Lorentz transformations are 4-vectors. The velocity 4-vector (γv, γbfv) and the energy-momentum 4-vector (E/c, are the most common.

    • Proper time

      The proper time interval between any two events is defined as:

      Δτ =    

      This is a particularly useful quantity because it is in independent of the frame in which it is measured.

    • Inner product invariance

      The inner product of two 4-vectors is defined as:

      AƒB = A0B0 - A1B1 - A2B2 - A3B3    

      Note that the minus signs make this inner product different from the usual dot product in 3-space. When defined in this way, the inner product of any two 4-vectors is a constant, independent of frame (that is, it is independent of the frame in which the vectors are written).

    • Relativistic units

      Are units in which c, the speed of light is given the value 1. This can be done in any number of ways; setting the unit of distance equal to 3×108 meters is one way. Setting the unit of distance as approximately 1 foot and the unit of time to 1 nanosecond also does the trick since the speed of light is approximately 1 foot/nanosecond. This simplifies calculations immensely. If you need to find an exact answer it is always possible to put the right number of factors of c back in at the end of a calculation by looking at the units and working out where factors of m/s are missing.

    • Formulae

       
      Lorentz Transformations for Energy and Momentum


      E = γ(E' + vp')    
      p = γ(p' + vE'/c2)    

       
      Formula for Velocity in terms of Energy and Momentum

      =    

       
      Relativistic relationship between mass, energy, and momentum. (Specifically, this equation states that the square of the energy-momentum 4-vector is equal to m2c4.) The formula reduces to the familiar E = mc2 when the momentum p is zero.

      E2 - |    

       
      Lorentz transformations for force undergoing a boost in the y-direction.


      Fx = Fx'    
      Fy =     

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