Both sides previous revision Previous revision Next revision | Previous revision | ||
basic_notions:energy [2018/04/12 16:49] bogumilvidovic [Concrete] |
basic_notions:energy [2018/04/12 16:51] (current) bogumilvidovic [Concrete] |
||
---|---|---|---|
Line 26: | Line 26: | ||
-->Proof the the total energy is conserved# | -->Proof the the total energy is conserved# | ||
- | [[equations:newtons_second_law|Newton's second law]] $F = ma$ implies | + | For a system with a conservative force the relationship between force and potential energy is given by $ |
+ | \nabla V \equiv - F$. | ||
+ | |||
+ | In addition, [[equations:newtons_second_law|Newton's second law]] $F = ma$ implies | ||
\[ | \[ | ||
\begin{split} | \begin{split} | ||
\frac{d}{dt}\left[K(t)+V(q(t))\right] &= F(q(t))\cdot v(t) + | \frac{d}{dt}\left[K(t)+V(q(t))\right] &= F(q(t))\cdot v(t) + | ||
- | \grad V(q(t))\cdot v(t) \\ | + | \nabla V(q(t))\cdot v(t) \\ |
- | &= 0, \qquad\text{(because $F=-\grad V$)}. | + | &= 0, \qquad\text{(because $F=-\nabla V$)}. |
\end{split} | \end{split} | ||
\] | \] | ||
Line 71: | Line 74: | ||
$ | $ | ||
- | \grad V \equiv - F,$ | + | \nabla V \equiv - F,$ |
where $F$ denotes the force. | where $F$ denotes the force. |