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183_notes:constantf [2021/02/18 20:52] – [Predicting the Motion] stumptyl | 183_notes:constantf [2023/01/13 19:59] (current) – hallstein | ||
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Depending on how you select your coordinate system, it might mean that more than one component of the momentum vector changes. Often, it is convenient to select a coordinate system where the net force is aligned with a coordinate direction, then only one momentum vector component changes in time. | Depending on how you select your coordinate system, it might mean that more than one component of the momentum vector changes. Often, it is convenient to select a coordinate system where the net force is aligned with a coordinate direction, then only one momentum vector component changes in time. | ||
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From this equation, you can determine the arithmetic average velocity, which in this case is equal to the average velocity. | From this equation, you can determine the arithmetic average velocity, which in this case is equal to the average velocity. | ||
- | + | $$v_{avg,x} = \dfrac{v_{ix} + v_{fx}}{2} = \dfrac{ v_{ix} + v_{ix} + \dfrac{F_{net, | |
- | $$v_{avg,x} = \dfrac{v_{xi} + v_{xf}}{2} = \dfrac{ v_{xi} + v_{ix} + \dfrac{F_{net, | + | = \dfrac{2v_{ix}}{2}+ \dfrac{\dfrac{F_{net, |
- | = \dfrac{2v_{xi}}{2}+ \dfrac{\dfrac{F_{net, | + | |
By using this average velocity in the [[183_notes: | By using this average velocity in the [[183_notes: | ||
- | $$x_{f} = x_{i} + v_{avg,x} \Delta t = x_{i} + v_{xi} \Delta t + \dfrac{1}{2}\dfrac{F_{net, | + | $$x_{f} = x_{i} + v_{avg,x} \Delta t = x_{i} + v_{ix} \Delta t + \dfrac{1}{2}\dfrac{F_{net, |
In physics, the information about the system prior to predicting its motion is called the " | In physics, the information about the system prior to predicting its motion is called the " | ||
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==== Connection to Energy ==== | ==== Connection to Energy ==== | ||
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+ | ==== Summary of Constant Force ==== | ||
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+ | The relationship between force and acceleration (even for a variable net force): →Fnet=m→a OR →a=→Fnetm. | ||
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+ | The following 1D equations are valid ONLY if the net force (and therefore, the acceleration) is constant. | ||
+ | xf=xi+vavg,xΔt | ||
+ | vfx=vix+Fnet,xmΔt | ||
+ | vavg,x=vix+vfx2=vix+12Fnet,xmΔt | ||
+ | xf=xi+vixΔt+12Fnet,xmΔt2 | ||
+ | v2xf=v2xi+2Fnet,xmΔx | ||
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==== Constant Force in 3D ==== | ==== Constant Force in 3D ==== | ||