<aside> <img src="https://s3-us-west-2.amazonaws.com/secure.notion-static.com/724202a9-05cb-4ba9-96f8-0c0ba9b496ce/Potential_Energy.png" alt="https://s3-us-west-2.amazonaws.com/secure.notion-static.com/724202a9-05cb-4ba9-96f8-0c0ba9b496ce/Potential_Energy.png" width="40px" /> Definition: Potential Energy is the energy stored by an object because of its position relative to other π objects, πΎ stresses within itself, β‘ its electrical charge, or other factors. For gravity:
$$ \text{General: } U_\text{grav}=-\frac{GmM_E}{r} \quad\text{For: }R\approx R_{earth}\;\rightarrow\; U_{grav}=mgh $$
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<aside> <img src="https://s3-us-west-2.amazonaws.com/secure.notion-static.com/5fea9ed9-4148-4a2e-a2b7-b2ee1ecd5e08/Notation.png" alt="https://s3-us-west-2.amazonaws.com/secure.notion-static.com/5fea9ed9-4148-4a2e-a2b7-b2ee1ecd5e08/Notation.png" width="40px" /> Notation:
$$ U=E_p \quad;\quad K=E_k $$
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$$ W_{tot}=W_\text{grav}+W_\text{el}+W_\text{all other}=\Delta K=K_\text{2}-K_\text{1} $$
Using this we can derive:
$$ W_\text{other}=(K_2+U_{2})-(K_1+U_{1}) \quad \text{where:} \\ U_1=\text{initial }E_p \; ; \; U_2=\text{final }E_p \; ; \; K_1=\text{initial }E_k \; ; \; K_2=\text{final }E_k $$
Definition: The work done by all forces other than the gravitational and elastic forces equals the change in the total mechanical energy of the system.
<aside> <img src="https://s3-us-west-2.amazonaws.com/secure.notion-static.com/7735cf07-6323-4721-a80c-43337d1e6cfa/Consergvative_force.png" alt="https://s3-us-west-2.amazonaws.com/secure.notion-static.com/7735cf07-6323-4721-a80c-43337d1e6cfa/Consergvative_force.png" width="40px" /> Definition: A conservative force is a force where the total mechanical energy of the system is conserved Example: gravity β ; elastic force β ; friction πβ Properties:
From this we can deduce:
$$ W_\text{tot}=W_\text{cons}+W_\text{non-cons}=\Delta K $$
For conservative forces: $U(x)$ potential energy depends only on position
$$ \Delta U=-\int^{x_2}_{x_1}F(x)\,dx $$
if we take $x_1=0$ then we can find the initial formulas:
In this case we can do it the other way around and deduce:
$$ F(x)=-\frac{\text{d}U}{\text{d}x} \\ \left . \begin{array}{ll} \bullet \;\; \text{if }F(x)>0\rightarrow U(x) \downarrow \\ \bullet \;\; \text{if }F(x)<0\rightarrow U(x) \uparrow \end{array} \right \}\text{ conservative force push system to low potential energy} $$