# Editing 2034: Equations

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:<math>E=K_{0}t+\frac{1}{2}\rho{}vt^2</math> | :<math>E=K_{0}t+\frac{1}{2}\rho{}vt^2</math> | ||

;All kinematics equations | ;All kinematics equations | ||

− | Most kinematics equations tend to make heavy use of constants, addition, powers, and multiplication. This specific equation resembles the actual kinematics equation d = vt + 1/2at^2, but replaces a (acceleration) with v (velocity | + | Most kinematics equations tend to make heavy use of constants, addition, powers, and multiplication. This specific equation resembles the actual kinematics equation d = vt + 1/2at^2, but replaces a (acceleration) with v (velocity) and replaces velocity with "K<sub>0</sub>", which is not a term used in kinematics. |

:<math>K_{n}=\sum_{i=0}^{\infty}\sum_{\pi=0}^{\infty}(n-\pi)(i+e^{\pi-\infty})</math> | :<math>K_{n}=\sum_{i=0}^{\infty}\sum_{\pi=0}^{\infty}(n-\pi)(i+e^{\pi-\infty})</math> |