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Total: 20 pts) A car is braking hard. There are two significant resistive forces acting on it, a quadratic (cv2) air drag, an

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Given that:

A car is braking hard.There are two significant resistive force acting on it, a quadratic (cv2) air drag , and a constant (\mu mg)frictional force.

a) First we write down the equation of motion for the car

m = -cu2 – umg (1) dt

The minus sign means that the forces are resistive. Dividing by m and using the chain rule as mentioned in the question , we get

do a 04+ 402 = -(2) drm

Multiplying equation (2)  by 2, we get

20 +2-1+ = -2ug → dcm v e-2) = -2uge — (3) m m

Integrating equation (3)om both sides

- 2c - 22, 2c mg 2c ve- = - umga er +D= Dex= 12 + m

D is the integration constant that we can determine by the condition that before the car hits breaks its velocity is v0 and x=0 . This gives us

umg D = 3 +

To find Xmax we set v=0 in equation (4).

buri ш el mar 2c Dº phim

Defining A² = pang equation (5)becomes

x_{max}=\frac{m}{2c}In\left ( \frac{A^{2}+v_{0}^{2}}{A^{2}} \right )=\frac{A^{2}}{2\mu g}In \left ( \frac{A^{2}+v_{0}^{2}}{A^{2}} \right )(6)

b)The initial velocity of the car is v0 =300km/hr =83.33ms-1 , the constant is

22 0.7 * 1200kg 9.8ms-1 0.86kgm-1 -=9572m2-2

Hence, using equation (6), xmax =380m.If there was no air drag the equation of motion will be

du V dr =-ug gx = D -

Again using x = 0 when v = v0 ,we get

6117

putting in the given values we get xmax =506m. As expected the distance required to stop the car without the air drag is large.

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