Mechanics: Slope Friction Problem

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SUMMARY

The discussion focuses on solving a slope friction problem using energy conservation principles and differential equations. Participants clarify the relationship between potential energy, work done, and average force, emphasizing the importance of defining average force over distance rather than time. The conversation also touches on solving second-order differential equations related to simple harmonic motion (SHM) and the necessary substitutions to simplify integrals. Key insights include recognizing standard equations and employing variable changes to facilitate integration.

PREREQUISITES
  • Understanding of potential energy and kinetic energy concepts
  • Familiarity with work-energy principles in physics
  • Knowledge of differential equations, particularly second-order ODEs
  • Basic grasp of simple harmonic motion (SHM) and its mathematical representation
NEXT STEPS
  • Study energy conservation in mechanical systems, focusing on slope friction problems
  • Learn techniques for solving second-order differential equations
  • Explore variable substitution methods in integral calculus
  • Investigate the characteristics and equations of simple harmonic motion (SHM)
USEFUL FOR

Students and educators in physics, particularly those studying mechanics and differential equations, as well as anyone interested in applying energy conservation principles to real-world problems.

MathDestructor
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Homework Statement
Need Help with Work Energy Theorem
Relevant Equations
Attached Below.
1580838354321.png


So far, I have this:
1580838395802.png


For Part ii) I know that:

mgh = xmgsin(theta), but I don't know how to go further
 
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MathDestructor said:
For Part ii) I know that:

mgh = xmgsin(theta), but I don't know how to go further
You know how much potential energy the object started with. Presumably you realize that it started and ended at rest -- that is, with zero kinetic energy.

So you can easily calculate how much energy was expended over the course of the downward slide. The work done over a path is given by the length of the path times the average [over distance] force along the path.

Does that give you a start?

You can make a useful observation about average force, given the nice way that this force is defined.
 
jbriggs444 said:
You know how much potential energy the object started with. Presumably you realize that it started and ended at rest -- that is, with zero kinetic energy.

So you can easily calculate how much energy was expended over the course of the downward slide. The work done over a path is given by the length of the path times the average [over distance] force along the path.

Does that give you a start?

You can make a useful observation about average force, given the nice way that this force is defined.
Yes, except that "average force" is defined as average over time. You mean "average over distance".
 
haruspex said:
Yes, except that "average force" is defined as average over time. You mean "average over distance".
Which is why I specified an average over distance.

My intuition is also screaming that due to symmetry, the two averages will match in this case.
 
jbriggs444 said:
Which is why I specified an average over distance.
So you did - sorry.
 
jbriggs444 said:
My intuition is also screaming that due to symmetry, the two averages will match in this case.
Wouldn't it be SHM (until the bottom)? The two averages differ for that.

OTOH, looks like the question can be answered using a symmetry argument without needing to mention averages or perform integrals.
 
Last edited:
1580849197361.png


1580849216801.png


Is this correct? How do I take the integral in the next part?
 
MathDestructor said:
Is this correct? How do I take the integral in the next part?
For the first part, your two methods are effectively the same (and correct).
For the next part, I gave rather a large clue in post #6. Apart from the constant force of gravity, the force is proportional to what? Does that ring any bells?
 
haruspex said:
For the first part, your two methods are effectively the same (and correct).
For the next part, I gave rather a large clue in post #6. Apart from the constant force of gravity, the force is proportional to what? Does that ring any bells?

I don't understand sorry
 
  • #10
Is my equation for Q3 right? If so how do I go about solving it?
 
  • #11
MathDestructor said:
Is my equation for Q3 right? If so how do I go about solving it?
The easy way is to recognise your first equation in post #7 as being (almost) a well known standard equation, with ##\ddot x## on one side and a term proportional to -x on the other.

Failing that, your v(x) = equation in the middle if the second image can easily be turned into time = an integral of a function of x wrt x.
The first step in solving the integral is to get rid of the x term (as opposed to the x squared term) by a simple change of variable. That will give you a constant term instead. Post what you get.
Then think about another substitution to get rid of the square root. I'll let you have a go at that before any further hints.
 
  • #12
haruspex said:
The easy way is to recognise your first equation in post #7 as being (almost) a well known standard equation, with ##\ddot x## on one side and a term proportional to -x on the other.

Failing that, your v(x) = equation in the middle if the second image can easily be turned into time = an integral of a function of x wrt x.
The first step in solving the integral is to get rid of the x term (as opposed to the x squared term) by a simple change of variable. That will give you a constant term instead. Post what you get.
Then think about another substitution to get rid of the square root. I'll let you have a go at that before any further hints.

What change of variable are you referring to? Could you please start me off with the first step?
 
  • #13
1580944310044.png


I got to this, what's next?
 
  • #14
MathDestructor said:
View attachment 256660

I got to this, what's next?
A simple shift in x (adding a constant) can eliminate the linear term, giving an expression of the form ##A\sqrt{1-cx^2}##.
A multiplicative substitution gets rid of c.
Do you see what to do from there?
 
  • #15
Yeah i got it, thanks !
 
  • #16
MathDestructor said:
Yeah i got it, thanks !
Good.
Note that in the original problem if you take x as the displacement from the middle then you get the SHM ODE straight away.
 

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