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183_notes:examples:relativemotion [2014/07/11 02:36] – caballero | 183_notes:examples:relativemotion [2014/11/16 08:05] (current) – pwirving | ||
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=== Lacking === | === Lacking === | ||
- | * The top speed of a Boeing 747 is unknown, but can be [[http:// | + | * The top speed of a Boeing 747 is unknown, but can be [[http:// |
=== Approximations & Assumptions === | === Approximations & Assumptions === | ||
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* The velocities of the plane relative to the air, the air relative to the ground, and the plane relative to the ground are represented in the following diagram. | * The velocities of the plane relative to the air, the air relative to the ground, and the plane relative to the ground are represented in the following diagram. | ||
- | <WRAP todo>Add vector addition diagram</ | + | {{ 183_notes: |
* The relative velocity equation for three objects is: →vA/C=→vA/B+→vB/C where →vA/C is the velocity of object A with respect to object C, etc. | * The relative velocity equation for three objects is: →vA/C=→vA/B+→vB/C where →vA/C is the velocity of object A with respect to object C, etc. | ||
- | |||
==== Solution ==== | ==== Solution ==== | ||
The problem can be described vectorially using the relative velocity equation: | The problem can be described vectorially using the relative velocity equation: | ||
- | $$\vec{v}_{plane/ground} = \vec{v}_{plane/air} + \vec{v}_{air/ground}$$ | + | $$\vec{v}_{p/g} = \vec{v}_{p/a} + \vec{v}_{a/g}$$ |
The pilot requires that the velocity of the plane with respect to the ground be directed due west. If you measure positive θ counterclockwise with respect to the east, the plane' | The pilot requires that the velocity of the plane with respect to the ground be directed due west. If you measure positive θ counterclockwise with respect to the east, the plane' | ||
- | $$\vec{v}_{plane/ground} = \langle -|v_{p/ | + | $$\langle -|v_{p/ |
+ | |||
+ | We can break this vector equation into two scalar equations: | ||
+ | |||
+ | $$-|v_{p/g}|=|v_{p/ | ||
+ | $$0=|v_{p/ | ||
+ | |||
+ | where vp/a,x and vp/a,y are the components of the unit vector in the direction of the velocity of the plane with respect to the air. Thus, they satisfy this equation. | ||
+ | |||
+ | $${v}_{p/ | ||
+ | |||
+ | You can rewrite the above equation by using what the unit vector components are equal to (in the previous two equations), | ||
+ | |||
+ | |||
+ | $$\left(-\dfrac{|v_{p/ | ||
+ | |vp/g|2+|va/g|2=|vp/a|2 | ||
+ | |||
+ | So, the speed that the plane has with respect to the ground is slower than its air speed, which agrees with the representation above. | ||
+ | $${|v_{p/ | ||
+ | |||
+ | The angle the compass should read can be determined from the above representation. The tangent of the angle (as measured from the negative x-axis is given by, | ||
+ | |||
+ | tanθ=|va/g||vp/g| | ||
+ | |||
+ | Hence, | ||
+ | |||
+ | θ=tan−1(|va/g||vp/g|)=tan−1(10ms225ms)=2.5∘ | ||
+ | |||
+ | which is 2.5∘ north of west or 177.5∘ from east measured counterclockwise. | ||
+ | |||
+ |