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expressed as t ′ = γ ( t − v x c2 ) x ′ = γ ( x − v t ) y ′ = y z ′ = z {\displaystyle {\begin{aligned}t'&=\gamma \left(t-{\frac {vx}{c^{2}}}\right)\\x'&=\gamma
the expression is instead B ν ( T ) = 2 ν 2 k B Tc2 . {\displaystyle B_{\nu }(T)={\frac {2\nu ^{2}k_{\text{B}}T}{c^{2}}}.} The Rayleigh–Jeans law agrees
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