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MY NOTES ASK YOUR TEACHER PRA If a car takes a banked curve at less than the ideal speed, friction is needed to keep it from
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Z Ncos e 0 N sin бш

A)

Here, radius of curve, r = 105 m

banking angle, θ = 15º

free-fall acceleration, g = 9.8 m/s2

We have to find out the ideal speed v (the speed for which no friction is required between the car's tires and the surface)

From the free-body diagram for the car:-

Fnet centripetal

mg*tan(\theta) = \frac{mv^2}{r}

g*tan(\theta) = \frac{v^2}{r}

21 9.8 * tan(15°) = 105

v^2 = 275.72

v = 16.6\ m/s

If the car has a speed of about 16.6 m/s, it can negotiate the curve without any friction.

B)

Now if, friction is present then, equilibrium about vertical direction:

N*cos(\theta) + f*sin(\theta) = mg

Also, in horizontal direction:

f*cos(\theta) - N*sin(\theta) = \frac{mv^2}{r}

Also,

f = \mu N, where mu is the coefficient of friction.

putting value of f in vertical direction equilibrium:

N*cos(\theta) + \mu N*sin(\theta) = mg

N = \frac{mg}{cos(\theta) + \mu*sin(\theta)}

Putting value of N in horizontal direction equilibrium:

\mu* \frac{mg}{cos(\theta) + \mu*sin(\theta)}*cos(\theta) - \frac{mg}{cos(\theta) + \mu*sin(\theta)} * sin(\theta) = \frac{mv^2}{r}

\mu* g*cos(\theta) - g * sin(\theta) = \frac{v^2}{r}*(cos(\theta) + \mu*sin(\theta))

\mu*cos(\theta) - sin(\theta) = \frac{v^2}{rg}*(cos(\theta) + \mu*sin(\theta))

Dividing whole equation by mu * cos θ:

1 - \frac{tan(\theta)}{\mu} = \frac{v^2}{rg}*(\frac{1}{\mu} + tan(\theta))

Substituting values of θ, r and g:

1 - \frac{0.268}{\mu} = \frac{48.1636}{1029}*(\frac{1}{\mu} + 0.268)

\mu - 0.268 =0.0468*(1 + 0.268*\mu)

\mu - 0.268 =0.0468 + 0.0125424 * \mu

\mu - 0.0125424 * \mu=0.0468 + 0.268

0.9874576*\mu=0.3148

\mu = 0.3188

The minimum coefficient of friction needed is 0.3188

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