Help Understanding A Paper - Brachistochrone With Friction

In summary, the paper "Help Understanding A Paper - Brachistochrone With Friction" explores the classic problem of the brachistochrone curve, which determines the fastest path between two points under the influence of gravity. It extends the analysis by incorporating frictional forces that affect the motion of a particle along the curve. The study examines the mathematical formulation of the problem, the impact of friction on the optimal path, and the resulting equations of motion. It aims to provide a deeper understanding of how friction alters the behavior of the system compared to the ideal scenario without friction.
  • #1
eddiezhang
26
6
Homework Statement
I am currently reading this paper (https://www.researchgate.net/publication/373607009_Exact_Solution_of_the_Problem_of_Brachistochrone_with_Allowance_for_the_Coulomb_Friction_Forces), where the author models the brachistochrone (least time of descent) curve for a circular ball while considering coulomb friction.

I'm confused by the penultimate step (the working behind equation 18).
Relevant Equations
.5mv^2 + mgy = mgH
Others contained in file / attached in attempt
Conservation of energy is invoked, which I understand, but the author omits most of the steps. He arrives at (18):


1727248857569.png




I've tried to substitute (13) and (17) into the LHS of the energy conservation equation, but the result is quite messy and my gut feeling is that it doesn't simplify in a nice way to achieve equation (18). For example:



Working.png



My Maths teacher has looked at this and is also confused as to how the author arrives at (18).

I realise that having to slog your way through this paper is not a trivial task, so any help or insight into how the author arrives at (18) is deeply appreciated. My gut feeling is that there is a simple physics principle applicable that I've missed from which (18) follows.

Relevant symbols used in the paper (for your convenience):
- μ is the coefficient of friction
- α is the angle formed between the unit tangent vector of the point on the curve being investigated; φ I believe is the same, but specifically as a function of time. The notation used is a little confusing.
- C1 is introduced as a constant of integration in (13)
- H is the starting height of of the ball above (0,0), i.e. the maximum y-value the ball possesses


Many thanks
 

Attachments

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  • #2
Forgot to mention: the author is Russian and I don't know how I might contact him (if necessary... or even welcome). Would anyone know how to and should I try?

Thanks.
 
  • #3
Continued grinding away on it; I think I get it now.
 

FAQ: Help Understanding A Paper - Brachistochrone With Friction

What is the Brachistochrone problem?

The Brachistochrone problem is a classic problem in the calculus of variations that seeks to determine the shape of a curve down which a particle will fall from one point to another in the least time, under the influence of gravity. The solution to this problem reveals that the optimal path is a cycloid, which is the trajectory traced by a point on the circumference of a circular wheel as it rolls along a straight line.

How does friction affect the Brachistochrone curve?

Friction introduces additional forces that oppose the motion of the particle along the path. This means that the optimal curve will not only depend on the gravitational force but also on the coefficient of friction between the surface and the particle. As a result, the presence of friction alters the shape of the curve, making it less efficient than the ideal Brachistochrone without friction.

What mathematical tools are used to solve the Brachistochrone problem with friction?

To solve the Brachistochrone problem with friction, one typically employs calculus of variations, differential equations, and numerical methods. The Lagrangian or Hamiltonian mechanics can also be applied to derive the equations of motion, taking into account both gravitational and frictional forces. Additionally, optimization techniques may be used to find the path that minimizes travel time under the influence of these forces.

Can the Brachistochrone problem with friction be solved analytically?

In many cases, the Brachistochrone problem with friction does not have a straightforward analytical solution due to the complexity introduced by the frictional forces. While it may be possible to derive approximate solutions or specific cases analytically, numerical methods are often employed to simulate and analyze the system for various conditions of friction and geometry.

What are the practical applications of understanding the Brachistochrone problem with friction?

Understanding the Brachistochrone problem with friction has practical applications in various fields such as engineering, physics, and robotics. It can inform the design of roller coasters, transportation systems, and mechanical systems where the motion of objects is influenced by friction. Additionally, insights from this problem can enhance our understanding of dynamics and optimization in real-world scenarios involving frictional forces.

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