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183_notes:examples:finalloccf [2014/07/11 02:58] – [Example: Predicting the location of an object undergoing constant force motion] caballero | 183_notes:examples:finalloccf [2014/07/14 17:08] (current) – caballero | ||
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===== Example: Predicting the location of an object undergoing constant force motion ===== | ===== Example: Predicting the location of an object undergoing constant force motion ===== | ||
- | The fan cart in the video below is observed to [[183_notes: | + | The fan cart in the video below is observed to [[183_notes: |
=== Facts ==== | === Facts ==== | ||
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* the force applied by the track (directly upward) | * the force applied by the track (directly upward) | ||
* a frictional forces and air resistance that resist the motion | * a frictional forces and air resistance that resist the motion | ||
- | * The acceleration due to gravity is 9.8 $\dfrac{m}{s^2} and is directed downward. | + | * The acceleration due to gravity is 9.8 $\dfrac{m}{s^2}$ and is directed downward. |
=== Lacking === | === Lacking === | ||
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=== Approximations & Assumptions === | === Approximations & Assumptions === | ||
- | * Over the interval that we care about it, we will assume the net force is doesn' | + | * Over the interval that we care about it, we will assume the net force doesn' |
* As a result, the motion occurs only in the horizontal direction. | * As a result, the motion occurs only in the horizontal direction. | ||
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* The displacement of the fan cart in the x-direction can be written like this: xf−xi=vxiΔt+12Fnet,xmΔt2 | * The displacement of the fan cart in the x-direction can be written like this: xf−xi=vxiΔt+12Fnet,xmΔt2 | ||
+ | ==== Solution ==== | ||
+ | The displacement of the cart is given by, | ||
- | + | Δxcart=xcart,f−xcart,i=vcart,xiΔt+12Fnet,xmcartΔt2 | |
+ | |||
+ | We can compute this displacement, | ||
+ | |||
+ | Δxcart=(0ms)(2.2s)+120.45N0.3kg(2.2s)2=3.6m | ||
- | ==== Solution ==== |