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Lorentz transformation

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TheLorentz transformations is a set of equations that describe a lineartransformation between a stationary reference frame and a reference frame inconstant velocity. The equations are given by:

x=xvt1v2c2{\displaystyle x'={\frac {x-vt}{\sqrt {1-{\frac {v^{2}}{c^{2}}}}}}} ,y=y{\displaystyle y'=y} ,z=z{\displaystyle z'=z} ,t=tvxc21v2c2{\displaystyle t'={\frac {t-{\frac {vx}{c^{2}}}}{\sqrt {1-{\frac {v^{2}}{c^{2}}}}}}}

wherex{\displaystyle x'}represents the new x co-ordinate,v{\displaystyle v} represents the velocity of the other reference frame,t{\displaystyle t} representing time, andc{\displaystyle c} thespeed of light.

On aCartesian coordinate system, with the vertical axis being time (t), the horizontal axis being position in space along one axis (x), the gradients represent velocity (shallowergradient resulting in a greater velocity). If the speed of light is set as a 45° or 1:1 gradient, Lorentz transformations can rotate and squeeze other gradients while keeping certain gradients, like a 1:1 gradient constant. Points undergoing a Lorentz transformations on such a plane will be transformed along lines corresponding tot2x2=n2{\displaystyle t^{2}-x^{2}=n^{2}} where n is some number

Points undergoing a Lorentz transformation follow the green, conjugate hyperbola, where the vertical axis represents time,y2x2=n2{\displaystyle y^{2}-x^{2}=n^{2}}


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