Solving Bicycle Brake Problem: Acceleration & Time to Stop

Join the discussion
Ask a follow-up here, or get your own question answered by working scientists, mathematicians and engineers — people, not an autocomplete.
Real named experts · corrections over time · the nuance an AI answer skips
15 replies · 2K views
joemama69
Messages
390
Reaction score
0

Homework Statement



A person is riding a bicycle at a constant speed v along a straight road and then gradually applies the brakes until the bicycle comes to a stop. Assume that the magnitude of the braking force increases liearly in time acordinto F = bt where b is a constant. The rider & bicycle have a total mass m

a)what is the magnitude and directio nof the acceleration of the rider and bicycle

b) is the acceleration constant or not? Explain

c) How long does it take to come to a stop

d) how far does the bike travel during the time the brakes are applied

Homework Equations





The Attempt at a Solution



a) i need to find the acceleration of the bike

v = v0 + at, v = 0

a = -vo / t

[tex]\sum[/tex]Fx = ma = -vo/t - bt

a = (-vo/t - bt)/m

b) not possitive but i do think it is constant because the brakes are being applied @ a constant, so it is constantly decreasing. does that make sence?

c) assuming my answer is correct to part a, i would just solve for t, but I am not too comfortable with my answer to a so i haven't solved it yet

d) same as c, but i would solve for x
 
Physics news on Phys.org
Fx = ma = bt

so a = bt/m

how do i allow for the initial velocity of the bicle, do i need to use a kinematic equation
 
The kinematic equations are valid only if the acceleration is constant. Here, the acceleration depends on time, therefore you cannot use them. You have enough information to answer parts (a) and (b). For part (c), you need to integrate the acceleration to find the velocity v(t) as a function of time. Once you have that, you can do part (d) by integrating the velocity to find the position x(t) as a function of time.
 
a)what is the magnitude and direction of the acerlation ?

Fx = ma = -bt mag of accel = -bt/m (
should it be possitive, is the mag the absolute value)

So the direction is negative

b)is the accerleration constant?

No because it is a functio of time

c)how long does it take to stop

v = [tex]\int[/tex]a dt = [tex]\int[/tex] (-bt)/m dt

v = -(bt2)/2m

t = [tex]\sqrt{2mv/-b}[/tex]

d)
 
d) x = [tex]\int[/tex]vdt = [tex]\int[/tex]-bt2/2m dt

x = -bt3/6m this is not correct
 
joemama69 said:
a)what is the magnitude and direction of the acerlation ?

Fx = ma = -bt mag of accel = -bt/m (
should it be possitive, is the mag the absolute value)

So the direction is negative
I would say opposite to the velocity instead of negative.
b)is the accerleration constant?

No because it is a functio of time
Good.
c)how long does it take to stop

v = [tex]\int[/tex]a dt = [tex]\int[/tex] (-bt)/m dt

v = -(bt2)/2m
You forgot the integration constant. You want the velocity to be v0 at t = 0, not zero as your expression suggests. Fix that first, then find the time it takes to stop.
 
[tex]\int[/tex]v = -bt2/2m + c where c = vo

t = [tex]\sqrt{2mv_o/b}[/tex]

part d,

x = [tex]\int[/tex]-bt2/2m + vodt = -bt3/6m + vot + c

the answer is x = 2/3vo(2mvo/b).5
 
i didnt get the same answer as the book (x = 2/3v(2mv/b).5), where did i go wrong
 
v = -bt2/2m + vo

so i integrated v to get the position

x = [tex]\int[/tex] -bt2/2m + vo = -bt3/6m + vot + c


but the answer is x = 2/3vo(2mvo/b).5
 
i attempted to pug in t, but that didnt work out either
 
joemama69 said:
v = -bt2/2m + vo

so i integrated v to get the position

x = [tex]\int[/tex] -bt2/2m + vo = -bt3/6m + vot + c


but the answer is x = 2/3vo(2mvo/b).5

Call the second integration constant c = 0. You assume that when he starts braking he is at the origin. What you have above is the position at any time t. You want the position when he stops. You know how long it take him to stop, so...
 
x = -bt3/6m + vot where t = (2mvo/b).5

x = -b(2mvo/b)3/2/6m + vo(2mvo/b).5

im stuck
 
You need to remove the parentheses by raising what's inside to the appropriate powers so you can simplify. For example,

[tex]b\large(\frac{2mv_{0}}{b} \large)^{3/2}=b\frac{2^{3/2}m^{3/2}v_{0}^{3/2}}{b^{3/2}}[/tex]

Then the b in the numerator and the b3/2 in the denominator combine to give you a b1/2 in the denominator.