Relative velocities: braking car

In summary: Ok. So you have xc(t) - v0t =-1/6*c*(t-t1)3. That is valid at t=t1.But let's be clear about what xc(t) means. At time t, how far behind the car is the cyclist? The cyclist must travel a total of 17+12+4=33 meters. The cyclist is 17 meters behind the car at the start. At time t1, the cyclist is behind the car by some distance. How much? If you add that to the 17 meters, you get the total distance the cyclist has traveled at time t1. So the equation at t=t1 should be:xc(t1) - v0t
  • #1
Poetria
267
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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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  • #2
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.
 
  • #3
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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  • #4
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.
 
  • #5
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)
 
  • #6
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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  • #7
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:
  • #8
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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  • #9
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. :)
 

What is relative velocity?

Relative velocity is the velocity of an object in relation to another object. It takes into account the motion of both objects and their direction of movement.

How does relative velocity affect a braking car?

When a car is braking, its velocity decreases. However, if there is another car or object in motion nearby, the relative velocity of the braking car will be affected by the velocity of the other object. This can result in a change in the overall direction and speed of the car.

Can relative velocity be negative?

Yes, relative velocity can be negative. This occurs when the two objects are moving in opposite directions, resulting in a negative value for the relative velocity.

What factors affect the relative velocity of a braking car?

The relative velocity of a braking car can be affected by the velocity and direction of other objects in motion, as well as external forces such as friction and wind resistance. It can also be influenced by the mass and velocity of the braking car itself.

How is relative velocity calculated?

Relative velocity can be calculated using vector addition. The velocity of one object is added to the velocity of the other object, taking into account their direction of movement. The resulting vector represents the relative velocity of the two objects.

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