Understating the acceleration equation in terms of velocity

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Sorry if this is considered a ‘basic’ question, but I’ve been stuck on this for a while now and can’t find much help. I know $\frac{d}{dx} \left(\frac{1}{2} v^2\right) =$ acceleration. But I do not understand what is wrong with my working out.

$$\left(\frac{d}{dt}\right)\left(\frac{dx}{dt}\right) = \left(\frac{d}{dx}\right)\left(\frac{dx}{dt}\right)\left(\frac{dx}{dt}\right) = \frac{d}{dx} (v^2)$$ I don’t know why I am missing the half that is in the original equation. I have seen the proof for it, but I do not exactly know what wrong assumption I am making. Thank you.

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Your working should go like this:

$a = \frac{dv}{dt}= \frac{dv}{dx} \cdot \frac {dx} {dt} = v\frac{dv} {dx}$

and at this point observe that $d(v^2) = 2vdv$, which allows you to rewrite the final expression as:

$ \frac{d(\frac 12 v^2)}{dx}$ as required.

Your error was in thinking $\frac {d}{dx} (\frac{dx} {dt})$ is a multiplication. It is not. It is differentiation of the velocity with respect to the displacement.

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Just to add to Deepak's answer, the result he quotes in the first line actually holds for total derivatives as well. Perhaps this proof is useful to the OP

$$\frac{d v(x, t)}{dt} = \frac{\partial v}{\partial t} + \frac{\partial v}{\partial x} \frac{dx}{dt} = \frac{\partial v}{\partial t} + \frac{\partial v}{\partial x} v $$

$$\frac{d v(x, t)}{dx} = \frac{\partial v}{\partial x} + \frac{\partial v}{\partial t} \frac{dt}{dx} = \frac{\partial v}{\partial x} + \frac{\partial v}{\partial t} \frac{1}{v} $$

Multiplying lower equation by $v$ and subtracting the two yields

$$\frac{dv}{dt} = v \frac{dv}{dx}$$