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183_notes:grav_and_spring_pe [2014/10/10 15:58] – caballero | 183_notes:grav_and_spring_pe [2014/10/14 13:20] – [Examples] caballero | ||
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===== Types of Potential Energy ===== | ===== Types of Potential Energy ===== | ||
+ | [[183_notes: | ||
==== (Near Earth) Gravitational Potential Energy ==== | ==== (Near Earth) Gravitational Potential Energy ==== | ||
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$$W_{s} = -\dfrac{1}{2}k_s\left(s_f^2-s_i^2\right)$$ | $$W_{s} = -\dfrac{1}{2}k_s\left(s_f^2-s_i^2\right)$$ | ||
+ | If you include the spring in your system, so that the system is now the spring and the object, then potential energy shared spring-object system is given by, | ||
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+ | - System: object+spring; | ||
+ | - Initial state: object at $s_i=0$; Final state: object at $s_f=s$ | ||
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+ | $$\Delta U_{s} = - W_{s} = +\dfrac{1}{2}k_s\left(s_f^2-s_i^2\right)$$ | ||
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+ | The spring potential energy depends on the spring constant ($k_s$) and how stretch changes ($s_f-s_i$). | ||
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+ | ==== Conservative Forces ==== | ||
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+ | Both of the examples above (local gravitational force and spring force) are examples of [[http:// | ||
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+ | Dissipative forces such as friction and air drag are non-conservative forces. The path that an object takes matters very much when non-conservative forces are present. Moreover, these dissipative forces cannot be associated with any construct like potential energy. | ||
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+ | ==== Examples ==== | ||
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+ | [[183_notes: | ||
+ | [[183_notes: |