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basic_notions:energy [2018/04/12 16:45] bogumilvidovic [Concrete] |
basic_notions:energy [2018/04/12 16:51] (current) bogumilvidovic [Concrete] |
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In addition, energy is responsible for temporal translations. We say energy generates temporal translations. | In addition, energy is responsible for temporal translations. We say energy generates temporal translations. | ||
+ | |||
+ | The total energy is defined as | ||
+ | \begin{equation} | ||
+ | E(t) \equiv K(t) + V(q(t)), | ||
+ | \end{equation} | ||
+ | |||
+ | where $K$ denotes the kinetic energy and $V$ the potential energy. | ||
+ | |||
+ | -->Proof the the total energy is conserved# | ||
+ | |||
+ | 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 | ||
+ | \[ | ||
+ | \begin{split} | ||
+ | \frac{d}{dt}\left[K(t)+V(q(t))\right] &= F(q(t))\cdot v(t) + | ||
+ | \nabla V(q(t))\cdot v(t) \\ | ||
+ | &= 0, \qquad\text{(because $F=-\nabla V$)}. | ||
+ | \end{split} | ||
+ | \] | ||
+ | |||
+ | <-- | ||
---- | ---- | ||
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Kinetic energy is defined as | Kinetic energy is defined as | ||
\begin{equation} | \begin{equation} | ||
- | K(t) \defeq \frac{1}{2}m\,v(t)\cdot v(t). | + | K(t) \equiv \frac{1}{2}m\,v(t)\cdot v(t). |
\end{equation} | \end{equation} | ||
This quantity is useful because | This quantity is useful because | ||
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This tells us that the change of kinetic energy is equal to the __work__ done by the | This tells us that the change of kinetic energy is equal to the __work__ done by the | ||
force. The work is defined as the integral of $F$ along the trajectory. | force. The work is defined as the integral of $F$ along the trajectory. | ||
+ | |||
+ | ---- | ||
+ | |||
+ | **Potential Energy** | ||
+ | |||
+ | $ | ||
+ | \nabla V \equiv - F,$ | ||
+ | |||
+ | where $F$ denotes the force. | ||
<tabbox Abstract> | <tabbox Abstract> | ||