[Math] How is $F=ma$ a differential equation? (Confirmation)

ordinary differential equationsphysics

Just wanna make sure I have this right. The derivative of position is velocity, and the derivative of velocity is acceleration

so if $$F = ma$$

where
$$a=\frac{d}{dx} v(t)\\
v(t)=\frac{d}{dx} s(t)$$ where $s(t)$ is the position in time.

This means that $$a = s''(t)$$
which means $$F = ms''(t)$$

and its an ordinary differential equation because it contains ordinary derivatives and it doesn't have the weird partial derivative symbol anywhere?

Is everything above right? Thanks.

Best Answer

Just expand a little on what everyone has already said: In general, assuming the mass $m$ and velocity $\mathbf{v}$ are functions of time only: $$ \mathbf{F}= \frac{d}{dt}\left(m\mathbf{v}\right) = m\frac{d \mathbf{v}}{dt}+ \frac{dm}{dt}\mathbf{v}$$ The above results follows from the fact that force is the rate of change of momentum with time, and momentum is the product of mass and velocity.

Now, if the mass $m$ is constant, then $\mathbf{v} =\frac{d \mathbf{s}}{dt}$ and $$\mathbf{F}= m\frac{d \mathbf{v}}{dt} = m\mathbf{a}$$ Finally (again assuming that $m$ is constant), if $\mathbf{s}$ is the displacement vector as a function of time, then $\mathbf{v} =\frac{d \mathbf{s}}{dt}$, which implies that $$\mathbf{F}= m\frac{d}{dt}\left(\frac{d \mathbf{s}}{dt}\right) = m\left[\frac{d^2}{{dt}^2}\mathbf{s}(t)\right] = m\mathbf{a}$$