Relative velocities: braking car

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Homework Help Overview

The problem involves a bicycle rider and a car, where the car is initially moving and then comes to rest while the cyclist attempts to catch up. The car's acceleration is defined in two phases, and the cyclist's speed needs to be determined based on the distances traveled by both during these phases.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the implications of the car's varying acceleration and question the validity of using standard equations of motion. There are attempts to integrate the acceleration to find velocity and position functions. Some participants express confusion over the integration limits and the interpretation of distance traveled.

Discussion Status

The discussion is ongoing, with participants exploring different methods of integration and clarifying the relationships between the variables involved. Some guidance has been offered regarding the integration process, but multiple interpretations and calculations are still being examined.

Contextual Notes

There are indications of confusion regarding the setup of the problem, particularly concerning the time intervals and the distances involved. Participants are also addressing the assumptions made about the distances covered by the car and the cyclist during the different phases of motion.

Poetria
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Homework Statement



A bicycle rider is riding at a constant speed of v(b) and at t=0 is 17m behind the car. The cyclist reaches the car when the car just comes to rest.
The car is moving with an acceleration:for 0<t<t(1)
a(c)=0

for t(1)<t<t(2)
a(c)= -c(t-t(1))

where its initial component of the velocity is v0=12m/s, t(1)=1s and c=6m/s^3. The car comes to rest at t(2).

Find the speed of the bicycle.

Homework Equations


[/B]
for t(1)<t<t(2)
v_c(t)=v_0-1/2*c*(t-t_1)^2
x_c(t)=v_0*(t)-1/6*c*(t-t_1)^3

The Attempt at a Solution


[/B]
Car: distance -
for 0<t<t(1) 12m
for t(1)<t<t(2) 4m

the time when car stops: 0=12-1/2*6*(t-1)^2 I got t(2)=3

x_c(t)=12-1/6*6*(3-1)^3

The speed of cyclist: (17+12+4)/3

Well, there is a mistake somewhere. :(
 
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This statement: a(c)= -c(t-t(1)) tells me that acceleration varies with time. If that is the case, then the formula x = V0*t + (1/2)*a*t2 is not valid, because that only holds for constant acceleration.
 
You must integrate the expression for acceleration, to find v(t), then integrate that to find x(t). When acceleration is constant, then you get the typical equations of motion that you are familiar with.
 
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scottdave said:
You must integrate the expression for acceleration, to find v(t), then integrate that to find x(t). When acceleration is constant, then you get the typical equations of motion that you are familiar with.

Ok, I will try. Many thanks.
 
Integral for v(t)
v_0-1/2*c*(t-t_1)^2

Integral for x(t)
v_0*(t)-1/6*c*(t-t_1)^3

Is it correct to evaluate it as follows:
(12*3-1/6*6*(3-1)^3)-(12-1/6*6*(1-1)^3)
 
If you integrate c*(t - k)dt where c and k are constants, then you get c*(t2/2 - k*t) + Integration_constant. The integration constant will equal the initial velocity, in this case. And k is equal to your t(1).
 
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scottdave said:
c*(t2/2 - k*t)
and then for x I would get:
v_0*t-c*(t^3/6 - k*t^2/2)

Well, this is weird, you know. This problem has two parts and at first I thought like you, I mean I integrated c*(t_1) as c*t_1*t but this wasn't accepted. On the other hand, I can't solve the second part.

So I will use your integrals:
12-6*(t^2/2 - 1*t)=0
t_2=1+sqrt(5)

(12*(1+sqrt(5))-6*((1+sqrt(5))^3/6 - (1+sqrt(5))^2/2))-(12-6*(1^3/6 - 1^2/2))=10*sqrt(5)

Speed of the cyclist:
(17+12+10*sqrt(5))/(1+sqrt(5))
 
Last edited:
Poetria said:
12-6*(t^2/2 - 1*t)=0
Looks like you integrated over 0 to t2 instead of t1 to t2.
 
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Poetria said:
and then for x I would get:
v_0*t-c*(t^3/6 - k*t^2/2)

Well, this is weird, you know. This problem has two parts and at first I thought like you, I mean I integrated c*(t_1) as c*t_1*t but this wasn't accepted. On the other hand, I can't solve the second part.

So I will try to evaluate: v_0*t-c*(t^3/6 - k*t^2/2)

(12*3-6*(3^3/6 - 3^2/2))-(12-6*(1^3/6 - 1^2/2))=22

speed of the cyclist: 51/3
haruspex said:
Looks like you integrated over 0 to t2 instead of t1 to t2.
haruspex said:
Looks like you integrated over 0 to t2 instead of t1 to t2.

OMG, I will fix it. Many thanks.
 
  • #10
Is it correct:

(12-6*(t^2/2 - 1*t))-(12-6*(1^2/2 - 1*1))

t_2 = 2 ?

(12*2-6*(2^3/6 - 1*2^2/2))-(12*1-6*(1^3/6 - 1*1^2/2))

the speed of the cyclist:
(17+12+14)/2
 
  • #11
Poetria said:
(12-6*(t^2/2 - 1*t))-(12-6*(1^2/2 - 1*1))
No. The v0t term is from 0 to t2. It's just the integral with the factor c that is from t1 to t2.
 
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  • #12
haruspex said:
No. The v0t term is from 0 to t2. It's just the integral with the factor c that is from t1 to t2.

Thanks for your patience.
The next try:

v_c(t)-v_0=-1/2*6*(t-1)^2+1/2*6*(1-1)^2
v_c(t)=12-3 (-1 + t)^2
0=12-3 (-1 + t_2)^2
t_2=3

x_c(t) - v_0*(t) =-1/6*c*(t-t_1)^3+1/6*c*(t-t_1)^3
x_c(t) - 12*3 = -1/6*6*(3-1)^3+1/6*6*(1-1)^3
x_c(t) = -8+36

(17+12+28)/3
 
  • #13
Poetria said:
t_2=3
Yes.
Poetria said:
x_c(t) - v_0*(t) =-1/6*c*(t-t_1)^3+1/6*c*(t-t_1)^3
Isn't the right hand side of that equation obviously zero? (But should not be.)
Poetria said:
x_c(t) = -8+36
That I agree with, but I don't understand how you then get:
Poetria said:
(17+12+28)/3
 
  • #14
haruspex said:
Yes.

Isn't the right hand side of that equation obviously zero? (But should not be.)

That I agree with, but I don't understand how you then get:

Oh yes, this is for t_1<t<t_2

x_c(t) - v_0*(t) =-1/6*c*(t_2-t_1)^3+1/6*c*(t_1-t_1)^3

The bike is 17 m behind the car

for 0<t<t_1 acceleration of the car is 0
distance traveled by the car is 12m

and for t_1<t<t_2
distance traveled by the car is 28

To reach the car the bike has to travel 17+12+28 in three seconds?
 
  • #15
Poetria said:
x_c(t) - v_0*(t) =-1/6*c*(t_2-t_1)^3+1/6*c*(t_1-t_1)^3
Ok, and the last term is zero, so we can simplify that to x_c(t) - v_0*(t) =-1/6*c*(t_2-t_1)^3.
But that's not quite right either; you have t on the left and t2 on the right. So to be strictly correct it should be x_c(t) - v_0*(t) =-1/6*c*(t-t_1)^3, with t=t2 being a value of interest.

Now, let's be clear about what xc(t) means here. Is it only the distance the car has covered since t1 or is it the entire distance since t=0?
The equation should also be valid at t=t1. This gives xc(t1)=v0t1. So what exactly is xc(t)?
 
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  • #16
haruspex said:
Ok, and the last term is zero, so we can simplify that to x_c(t) - v_0*(t) =-1/6*c*(t_2-t_1)^3.
But that's not quite right either; you have t on the left and t2 on the right. So to be strictly correct it should be x_c(t) - v_0*(t) =-1/6*c*(t-t_1)^3, with t=t2 being a value of interest.

Now, let's be clear about what xc(t) means here. Is it only the distance the car has covered since t1 or is it the entire distance since t=0?
The equation should also be valid at t=t1. This gives xc(t1)=v0t1. So what exactly is xc(t)?

Yes, t_2, it was messy.

I understand there are two stages:

0<t<t_1
x_c(t)=v_0*t

and

t_1<t<t_2

x_c(t)=v_0*(t)-1/6*c*(t-t_1)^3

I thought this was a distance from t_1 to t_2.

I see I think now I was wrong. :(
 
  • #17
So it would be (17+28)/3.
 
  • #18
Poetria said:
So it would be (17+28)/3.
Which simplifies to...? And state the units.
 
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  • #19
haruspex said:
Which simplifies to...? And state the units.

15m/s

Round number.
 
  • #20
Poetria said:
15m/s

Round number.
... which is always reassuring.
 
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  • #21
haruspex said:
... which is always reassuring.

Many thanks. :) Now I understand everything. :)
 

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