# The work-energy theorem

Well here's the question.

From some previous excercises we know that from \begin{align} A&=\int F\;ds,\\ &=\int ma\;ds, &&(F=ma)\\ &=\int m \frac{dv}{dt}\;ds, &&(a=dv/dt)\\ &=m \int_{v_1}^{v_2}v\; dv,\\ &=m \frac{v_2^2}{2}-m \frac{v_1^2}{2},\\ &=W_2-W_1, &&(W_i=\frac12mv_i^2)\\ &=\Delta W. \end{align} Meanwhile for potential energy we have the shown figure \begin{align} A&= \int m a\;ds,\\ &= \int m \frac{dv}{dt}\;ds, \end{align} Here the professor did something like: $$ds \times \cos \alpha =-dh$$ and then the equation goes \begin{align} A&=- \int m \frac{dv}{dt}\;dh,\\ &=- \int m v \;dv,\\ &=-m \int v \text{ }dv \end{align} and up to

$$A=-\Delta W_p$$

Now what I'd like to understand from you is one logic explanation for

$$ds \times \cos \alpha=-dh$$

I'd be very grateful! • Could you help to specify the problem more? For example, how is $F$ defined? Is this a 2D problem? If 2D, is $F$ a force acting tangential to the path of motion? If $F$ doesn't, then should there not be any vector notation? What exactly do all the variables represent, etc? Dec 21, 2014 at 0:40

The height $h$ is probably the vertical displacement pointing downwards. Therefore: $$h = \left(-\mathbf{\hat j}\right)\cdot\mathbf s = -|\mathbf{\hat j}||\mathbf s|\cos\alpha = -s\cos\alpha$$
Now we can derive: $$\frac{dh}{ds} = -\frac{d}{ds}\left(s\cos\alpha\right) = -\cos\alpha \quad\Longrightarrow\quad \frac{dh}{ds} = -\cos\alpha$$
Therefore, multiplying both sides by $ds$, we get: $$dh = -\cos\alpha ds$$