Problem About Change in Momentum/Impulse

  • Thread starter Thread starter gibberingmouther
  • Start date Start date
  • Tags Tags
    Change
Click For Summary

Homework Help Overview

The discussion revolves around a problem involving the change in momentum and impulse of two carts with different masses being pushed by equal forces over a distance of 1 meter. The participants explore how the momentum of a 0.2 kg plastic cart compares to that of a 20 kg lead cart after traveling the same distance from rest.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of impulse and momentum equations, questioning the derivation of relationships between momentum and final velocity. Some express confusion over the use of kinematic equations and the implications of their results.

Discussion Status

There are ongoing clarifications regarding the definitions and relationships of momentum and force. Some participants have provided insights into the proportionality of momentum to velocity, while others have pointed out potential misunderstandings in the application of equations. The discussion is active, with various interpretations being explored.

Contextual Notes

Participants note the importance of correctly applying LaTeX notation and the implications of using average versus instantaneous quantities in their calculations. There is also mention of external resources that may influence understanding.

gibberingmouther
Messages
120
Reaction score
15

Homework Statement


A 0.2 kg plastic cart and a 20 kg lead cart can both roll without friction on a horizontal surface. Equal forces are used to push both carts forward for a distance of 1 m, starting from rest.

After traveling 1 m, is the momentum of the plastic cart greater than, less than, or equal to the momentum of the lead cart?

Homework Equations


##J = \Delta p = Favg \times \Delta t##
##\Delta x = (\Delta p \times \Delta t)/ m##
(from the equation for impulse and change in momentum: \Delta x / \Delta t = v_f because the carts start at rest)
##\Delta x = v_i \times \Delta t + .5 \times a_x \times \Delta t^2##
##\Delta x = .5 \times (v_i + v_f) \times \Delta t##

The Attempt at a Solution


I did algebra using delta x and tried both kinematics equations. The entire reason I posted this is because, using both kinematics equations, I derived the statement ##\Delta p = .5 \times \Delta p##. So I must have made a mistake somewhere but I can't figure out where. The acceleration is constant so I should be able to use the kinematics equations.

I think there are solutions to this problem on the Internet, but the main reason I posted this is because of the momentum equals half of itself solutions I got. But if someone wants to help me with the solution to the actual problem as well, that would be appreciated. I messed around with equations and tried to figure out the behavior of the two carts compared to each other, but wasn't yet able to find a solution to how they compare at 1 m.

edit: sorry for the messed up Latex before this edit, i had an appointment to go to so i didn't have time to fix it before i left after i saw it was wrong
 
Last edited:
Physics news on Phys.org
gibberingmouther said:
##J = \Delta p = F_avg x \Delta t##
Please do not use x for multiplication in LaTeX. Use \times.
gibberingmouther said:
##\Delta x = (\Delta p \times \Delta t)/ m##
mΔx/Δt will give average momentum, not change in momentum.
gibberingmouther said:
\Delta x / \Delta t = v_f because the carts start at rest)
Δx/Δt does not give final velocity.
 
  • Like
Likes   Reactions: gibberingmouther
haruspex said:
Please do not use x for multiplication in LaTeX. Use \times.

mΔx/Δt will give average momentum, not change in momentum.

Δx/Δt does not give final velocity.

haruspex said:
Please do not use x for multiplication in LaTeX. Use \times.

mΔx/Δt will give average momentum, not change in momentum.

Δx/Δt does not give final velocity.
Oops! I see my mistake now. Thanks!
 
Okay, I figured it out.

I managed to derive that the momentum will be inversely proportional to the final velocity, so since the smaller cart has a bigger velocity its final momentum will be less.

But I also looked at another physics forum post and saw that you can apply the version of Newton's second law that says the definite integral of the force over a time interval is equal to the rate of change of momentum over that interval. So, since the time interval for the faster accelerating cart is shorter, its integral is smaller, thus the change in momentum is less! That's the best way to answer this problem. Cool!
 
gibberingmouther said:
Okay, I figured it out.

I managed to derive that the momentum will be inversely proportional to the final velocity, so since the smaller cart has a bigger velocity its final momentum will be less.
The above statement makes me want to say, "Whoa there! Momentum is given as mv thus it's proportional to velocity."

Yes, I know that in this case the numbers work out so that ratio of velocities (small : large) is 10 : 1 and the ratio of momenta is 1 : 10 .

The analysis you give below is significantly better.

But I also looked at another physics forum post and saw that you can apply the version of Newton's second law that says the definite integral of the force over a time interval is equal to the rate of change of momentum over that interval. So, since the time interval for the faster accelerating cart is shorter, its integral is smaller, thus the change in momentum is less! That's the best way to answer this problem. Cool!
 
  • Like
Likes   Reactions: gibberingmouther
gibberingmouther said:
definite integral of the force over a time interval is equal to the rate of change of momentum over that interval.
You are conflating two forms of statement there, leading to an extra level of integration/differentiation.
The definite integral of the force over a time interval is equal to the change of momentum over that interval.
The force at an instant is equal to the rate of change of momentum.
 
  • Like
Likes   Reactions: gibberingmouther
haruspex said:
You are conflating two forms of statement there, leading to an extra level of integration/differentiation.
The definite integral of the force over a time interval is equal to the change of momentum over that interval.
The force at an instant is equal to the rate of change of momentum.
Thank you for clarifying! That actually came up during class today.

Am I right then that dp/dt would be equal to (N*s)/s then?
 
gibberingmouther said:
Thank you for clarifying! That actually came up during class today.

Am I right then that dp/dt would be equal to (N*s)/s then?
Yes, assuming that you are referring to units. Of course, 1 Newton*second/second is 1 Newton .

Newton's 2nd Law is often given briefly as ##\ F=ma\ ## or ##\ \displaystyle a = \frac F m \,.\ ## But, it is sometimes given as ##\ \displaystyle F = \frac {dp}{dt} \,,\ ## which I've been told, is the form in which Newton presented it.
 
Quantitatively:

## p_1=Ft_1 ##

and

##p_2=Ft_1\sqrt{\frac{m_2}{m_1}}##
 

Similar threads

Replies
19
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 5 ·
Replies
5
Views
972
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 2 ·
Replies
2
Views
3K
Replies
23
Views
2K
Replies
8
Views
1K