Classical Mechanics-Inclined plane tricky problem

  • Thread starter Thread starter squareroot
  • Start date Start date
  • Tags Tags
    Classical Plane
Click For Summary
SUMMARY

The discussion centers on solving a classical mechanics problem involving an inclined plane with a friction coefficient defined by the equation μ = bx, where b is a constant and x is the distance traveled by a mass m. Participants emphasize the need to apply Newton's laws and concepts of simple harmonic motion (SHM) to derive the distance and time taken for the object to stop. The key equations discussed include F = ma and the period of oscillation T = 2π√(m/k), where k is derived from the forces acting on the mass. The solution involves recognizing the relationship between the forces and re-framing the problem in terms of SHM to find the stopping distance and time.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Basic knowledge of simple harmonic motion (SHM)
  • Familiarity with the concept of friction and its mathematical representation
  • Ability to manipulate algebraic equations and solve for variables
NEXT STEPS
  • Study the derivation of the equations of motion for simple harmonic oscillators
  • Learn about the work-energy theorem in classical mechanics
  • Explore differential equations and their applications in physics
  • Investigate the relationship between force, mass, and acceleration in various contexts
USEFUL FOR

Students studying physics, particularly those in high school or early college, who are tackling problems involving inclined planes, friction, and oscillatory motion. This discussion is also beneficial for educators seeking to clarify concepts related to classical mechanics.

  • #31
No.I'm really stuck with this one, i think I'm having the biggest mind block of my life so far. :))
 
Physics news on Phys.org
  • #32
squareroot said:
No.I'm really stuck with this one, i think I'm having the biggest mind block of my life so far. :))
What value of x makes mgsin(α)-bxmgcos(α) = 0?
We want to relocate the origin so as to be a measure of distance from that point.
 
  • #33
Well that would mean that mgsin(α)=bxmgcos(α) so do I write x=mgsin(α)/bmgcos(α) ?

"We want to relocate the origin so as to be a measure of distance from that point." I don t really get the meaning of this part.
 
  • #34
But if i take that expression and simplify it i get that x=sin(α)/bcos(α), and I've got to this expression earlier but my teacher said it s not good.
 
  • #35
squareroot said:
Well that would mean that mgsin(α)=bxmgcos(α) so do I write x=mgsin(α)/bmgcos(α) ?
No, you want to shift the origin of x by that much. I.e. instead of using x as the measure of displacement you use, say, u = x - tan(α)/b. The variable u should then satisfy the standard form for SHM.
 
  • #36
and where woud I use this u? this is a optional problem given by my teacher for those who want a deeper grasp of shm, i need it solved and then i need too study the solving method so that i get a deep understanding, not just fractals and pieces of information.If someone could solve this and explain it to me i think i woud have a better grasp of it.As i said this is a optional problem it s not worth any credits so it s not cheating, just satisfying my curiosity.

Thank you!
 
  • #37
squareroot said:
and where woud I use this u?
All this has done is measure x from a different point on the plane. Or to put it another way, we found the equilibrium position, which was not x=0. It is u=0.
 
  • #38
well yea, but what do i do with this u? and why is the equillibrium position at u=0?
 
  • #39
squareroot said:
well yea, but what do i do with this u?
You don't have to anything with it. Reformulating in terms of this u allows you to recognise the equation as being an exact fit for SHM. That allows you to figure out the frequency and amplitude in the usual way. Your problem was that extra constant term in the acceleration; rewriting it with u got rid of that.
and why is the equillibrium position at u=0?
Because that is where the acceleration will be 0.
 
  • #40
got it! but where do i use this u in equations?that s what i can t figure out.
 
  • #41
and why if i write it u like that, why does it the resemble a smh?
 
  • #42
what i want to say is how do i find k? with this u?
 
  • #43
Measuring x from the top you had:
F=mgsin(β)-b*x*mgcos(β)
which looks like SHM except for the constant acceleration term, mgsinβ.
But we note that this makes F, and hence the acceleration, 0 when x = tan(β)/b. So that must be the equilibrium point.
If we measure the distance from x = tan(β)/b instead, i.e. distance = u = x - tan(β)/b, we get F = -b*u*mgcos(β)
Since u is just a constant different from x, the acceleration of x is the same as the acceleration of u, so this is now recognisably SHM, and you can use your standard knowledge about SHM in relation to frequency, amplitude... The only thing to remember is that u is not measuring distance from the top.
 
  • #44
Ok, so now i can say that k=-b*mgcos(β) so that period T=2π√(m/k), T=2π√(m/-bmgcos(β)) , T=2π√1/(-bgcos(β)) , and the frequency is 1/T.

But how do i get from this equations to those which help me find the actual distance and time that i need?
 
  • #45
squareroot said:
Ok, so now i can say that k=-b*mgcos(β) so that period T=2π√(m/k), T=2π√(m/-bmgcos(β)) , T=2π√1/(-bgcos(β)) , and the frequency is 1/T.

But how do i get from this equations to those which help me find the actual distance and time that i need?
The object starts at rest and we want the time until it is at rest again. Whether we measure distance as x or u does not affect the speed, so it's the time between successive points of zero speed in the SHM equation. How does that relate to the period of oscillation?
Similarly, amplitude is half the difference between extremes of position, and for that it won't matter whether we use x or u, so it's the amplitude you see in the SHM equation.
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
Replies
46
Views
4K
Replies
3
Views
3K
  • · Replies 2 ·
Replies
2
Views
1K
  • · Replies 33 ·
2
Replies
33
Views
4K
  • · Replies 23 ·
Replies
23
Views
3K
Replies
7
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 11 ·
Replies
11
Views
4K
Replies
2
Views
2K