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--- 183_notes:grav_and_spring_pe [2014/10/10 15:58] – caballero
+++ 183_notes:grav_and_spring_pe [2021/03/12 02:45] (current) – [Types of Potential Energy] stumptyl
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+Section 6.8 and 7.2 in Matter and Interactions (4th edition)
 ===== Types of Potential Energy =====
+[[183_notes:potential_energy|Potential energy]] is the energy associated with interactions between pairs of objects. **In these notes, you will read about two particular types of potential energy: the energy associated with the gravitational interaction and the energy associated with a spring-mass system.**
 ==== (Near Earth) Gravitational Potential Energy ====
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 [{{ 183_notes:potential_energy.006.png?400|A spring-mass system (spring constant,  $k_s$ ) is stretched through a distance ( $\Delta s$ ).}}]
-To determine the potential energy associated with a spring-mass system, consider the work done by a spring on an object (mass,  $m$ ) attached to its end. The spring is stretched through a displacement ( $\Delta \vec{s}$ ). The displacement and the gravitational force are in opposite directions.
+To determine the potential energy associated with a spring-mass system, consider the work done by a spring on an object (mass,  $m$ ) attached to its end. The spring is stretched through a displacement ( $\Delta \vec{s}$ ). The displacement and the spring force are in opposite directions.
 To calculate the work that the spring does, consider the object as the system. Remember that the [[183_notes:springmotion|spring force changes with displacement]], and thus we must use the [[183_notes:work_by_nc_forces|integral formulation to calculate the work]].
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  $W_{s} = -\dfrac{1}{2}k_s\left(s_f^2-s_i^2\right)$
+If you include the spring in your system, so that the system is now the spring and the object, then the potential energy shared between the spring-object system is given by,
+  - System: object+spring; Surroundings: Nothing
+  - Initial state: object at  $s_i=0$ ; Final state: object at  $s_f=s$
+ $\Delta U_{s} = - W_{s} = +\dfrac{1}{2}k_s\left(s_f^2-s_i^2\right)$
+The spring potential energy depends on the spring constant ( $k_s$ ) and how stretch changes ( $s_f-s_i$ ).
+==== Conservative Forces ====
+Both of the examples above (local gravitational force and spring force) are examples of [[http://en.wikipedia.org/wiki/Conservative_force|conservative forces]]. Conservative forces are those for which we can associate a potential energy. The energy associated with conservative forces does not depend on the path that the objects take but only their separation. That is, for conservative forces, only the initial and final locations of the objects matter not the path they took to get from one place to another. Forces that only depend on position tend to be conservative.((We say "tend to" because there is an additional condition that the force have [[http://en.wikipedia.org/wiki/Curl_(mathematics)|no curl]].))
+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.
+==== Examples ====
+  * [[183_notes:examples:sledding|Sledding down a hill]]
+  * [[183_notes:examples:the_jumper|The Jumper]]