183_notes:examples:relativemotion

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183_notes:examples:relativemotion [2014/07/11 02:36] caballero183_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://lmgtfy.com/?q=top+speed+of+747|found online]] (920 kmh or vp/a=255dfracms).+  * The top speed of a Boeing 747 is unknown, but can be [[http://lmgtfy.com/?q=top+speed+of+747|found online]] (920 kmh or $v_{p/a} = 255 \dfrac{m}{s}$).
  
 === 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</WRAP>+{{ 183_notes:planerelativemotion.png?350 }}
   * 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's velocity relative to the ground should only have a negative x-component. So the equation above becomes (in 2D), 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's velocity relative to the ground should only have a negative x-component. So the equation above becomes (in 2D),
  
-$$\vec{v}_{plane/ground\langle -|v_{p/g}|,\rangle= |v_{p/a}|\hat{v}_{p/a} + \langle 0, -|v_{a/g}|\rangle$$+$$\langle -|v_{p/g}|,0 \rangle = |v_{p/a}|\hat{v}_{p/a\langle 0, -|v_{a/g}|\rangle$$ 
 + 
 +We can break this vector equation into two scalar equations: 
 + 
 +$$-|v_{p/g}|=|v_{p/a}|{v}_{p/a,x}$$ 
 +$$0=|v_{p/a}|{v}_{p/a,y}-|v_{a/g}|$$ 
 + 
 +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. 
 + 
 +$${v}_{p/a,x}^2 {v}_{p/a,y}^2 = 1$$ 
 + 
 +You can rewrite the above equation by using what the unit vector components are equal to (in the previous two equations), 
 + 
 + 
 +$$\left(-\dfrac{|v_{p/g}|}{|v_{p/a}|}\right)^2+\left(\dfrac{|v_{a/g}|}{|v_{p/a}|}\right)^2= 1$$ 
 +|vp/g|2+|va/g|2=|vp/a|2
 
 + 
 +Sothe speed that the plane has with respect to the ground is slower than its air speed, which agrees with the representation above. 
 +$${|v_{p/g}|}= \sqrt({|v_{p/a}|}^2-{|v_{a/g}|}^2) = \sqrt{(255 \dfrac{m}{s})^2 - (10 \dfrac{m}{s})^2} = 225 \dfrac{m}{s}$$ 
 + 
 +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=tan1(|va/g||vp/g|)=tan1(10ms225ms)=2.5
 
 + 
 +which is 2.5 north of west or 177.5 from east measured counterclockwise. 
 + 
 + 
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