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Question: Show that equation (2-36) follows from the arbitrary four-vector Lorentz transformation equations (2-35).

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Answer

Equation (2-36) follows from the arbitrary four-vector Lorentz transformation equations (2-35).

Step by step solution

01

Significance of the Lorentz transformation

The Lorentz transformation is described as a set of some equations which mainly relate to the time and space coordinates. This transformation is mainly done with the help of an inertial frame.

02

Determination of the equations

The equation of the invariant quantity in the plane is expressed as:

A'x=γvAx-vcAtA'x2=γv2Ax2- 2AxvcAt+v2c2At2 (1)

The equation of the invariant quantity in the plane is expressed as:

A't=γvAt-vcAxA't2=γv2At2- 2AtvcAx+v2c2Ax2 (2)

Subtracting equation (1) from equation (2).

A'x2-A't2=γv21-v2c2Ax2-1-v2c2At2

As , localid="1658808288943" γv2=11-v2c2then A'x2-A't2=Ax2-At2. Moreover,A'y2=Ay2 andA'z2=Az2

Finally, the above equation will become:

A't2-A'x2+A'y2+A'z2=At2-Ax2+Ay2+Az2

The above equation is the equation (2-36) which is in the time-space context.

Thus, equation (2-36) follows from the arbitrary four-vector Lorentz transformation equations (2-35).

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