Physics Asked by i2Witty on March 6, 2021
I’m having trouble properly conceptualizing a question.
The question is:
"Suppose you are driving down a steep hill (5 degrees, 8.7%, which is fairly steep for roads), on a rainy day ($mu$ = .5) at a reckless 30 $frac{m}{s}$. The stoplight at the bottom of the high turns red. It is 75 meters in front of you. (You can neglect reaction time, because you saw it turn yellow, so you were ready to put on breaks.) Can you stop before the light? If so, what is your stopping distance?"
So far, I was able to find out the acceleration in the x distance.
$sum{}^{}F_x = F_b-F_f
ma_x = mgsin5 – .5mgcos5 $
The masses cancel out so we are left with:
$a_x = (9.8)sin5 – .5(9.8)cos5 = -4.03 frac{m}{s^2} $
I have no idea where to continue from here. Any help is appreciated. Thanks.
If you have the acceleration $a$, you can calculate the distance traveled $s$ using the equation
$v^2 = u^2 + 2as$
You have your initial velocity which is $u = 30 ms^{-1}$ and you need your final velocity to be $v = 0$.
And if this distance is shorter than the distance to the traffic light you will have your answer.
Answered by joseph h on March 6, 2021
The trick to this question is to realize there is no need for a complicated dynamic rules. You took your time to evaluate the friction force acting on a car
$$F = mg sin(alpha) - mu mg cos(alpha) $$
and you can see that this force is contants, therefore your acceleration $a = F/m = g( sin(alpha) - mu cos(alpha))$ is also constant. Now you can work with uniformly accelerated motion. You know (for $t_f$ being final time)
$$s = v_0t_f + frac 12 a t_f^2, qquad 0 = v_0 + at_f$$
which leads to the time of breaking $t_f = -v_0/a$ and therefore the distance of breaking
$$ s = -frac{v_0^2}a + frac 12 a left( frac{v_0}a right)^2 = -frac{v_0^2}{2a}. $$
You can see that the minus is fine, because acceleration is negative in this notation.
Answered by Jimmy Found on March 6, 2021
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