Elastic Pendulum with Newton's equations of motion

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Homework Help Overview

The discussion centers around a pendulum system involving a mass on an elastic rod that swings in the xy-plane. The forces acting on the pendulum include an elastic central force directed towards the origin and gravitational force, with gravity defined as acting in the positive y-direction. The equations of motion are provided, and the participants are tasked with deriving the equation of motion in the y-direction, computing equilibrium length, and demonstrating oscillatory motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the setup of the equations of motion, particularly the signs and directions of forces involved. There is confusion regarding the treatment of gravitational force and elastic force in the context of the equations. Questions arise about how to derive the second equation of motion and the implications of potential energy on force direction.

Discussion Status

The discussion is ongoing, with participants seeking clarification on the correct formulation of forces in the equations of motion. Some participants have offered insights into the relationship between gravitational force and elastic force, while others are questioning the assumptions made in the problem setup. There is no explicit consensus yet on the correct approach to the equations.

Contextual Notes

Participants note the importance of understanding the relationship between potential energy and force, as well as the implications of the chosen coordinate system on the equations of motion. There is a recognition of the need to clarify the definitions and signs of forces involved in the problem.

ojb89
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Homework Statement


A pendulum with a mass m hanging on a elastic bug rigid massless rod which may swing in the xy-plane. The pivot point is the origin of the coordinate system. The force acting on the pendulum is the sum of force of an elastic central force directed towards the origin, and gravity, which by choice of the orientation of the coordinate system, points in the positive y-direction. Friction of any kind (air, in pivot point) can be disregarded.

Newtons's equation of motion:
equation 1: mx''=-\frac{\partial V}{\partial x}
equation 2: my''=-\frac{\partial V}{\partial y}-mg

Gravity: g=9.81 m/s^2
Potential energy of the rod: V(r)=0.5*k*(r-L)^2, where r=\sqrt{x^2+y^2}
Length: L=1 m (length of rod in absence of external force)
We see from these equations that the solution does not depend separately on k and m, but only the combination w^2=\frac{k}{m}.

Homework Equations


a)[/B] Here we shall on look at the pendulum moving in vertical direction (x(t)=0). I need to derive the equation of motion in y-direction (in other words I need to show of to get equation 2).
But I'm having problem figure out how I can get it like equation 2. More in attempt of solution.

b) Compute the equilibrium of length L_r for this case.

c) Show that the solution of the equation of motion is an oscillation, up and down about the equilibrium with angular frequency w

The Attempt at a Solution


a)[/B] So the pendulum will act like a elastic spring with a mass. The two forces acting on the pendulum in each direction. The gravity force which we can write F_g=mg. And the force because of the potential energy which we can write F_u=-\frac{\partial V}{\partial y}.
I know we can use Newton's second law: \sum F=ma. And y''=a. But I'm having trouble with the how to set it up. From the problem description I read that F_g is positive and F_u is negative. This gives the the sum of forces F_g-F_u=my''. Inserting gives us: mg-(-\frac{\partial V}{\partial y})=my''. So I get both forces positive, but it should be negative. What am I missing?

b) I know I can find the equilibrium of length by setting my'' to 0. So I get 0=-\frac{\partial V}{\partial y}-mg. So after I derive -\frac{\partial V}{\partial y}, should I solve 0=-\frac{\partial V}{\partial y}-mg with respect to y and insert L=1 or with the respect to L? Which would give me a solution with something of y.

c) I guess I need to solve this as a second order differential equation. With the equation being: itex]y''+0*y'+\frac{\partial V}{\partial y}=0[/itex].
Is this correct? Not sure how to proceed to show the solution.

Sorry for a long post. I really hope I have showed you that I have tried, but I really need help. And not sure if posted in the right sub-forum.
 
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ojb89 said:
1. Homework Statement
ojb89 said:
A pendulum with a mass m hanging on a elastic bug rigid massless rod which may swing in the xy-plane. The pivot point is the origin of the coordinate system. The force acting on the pendulum is the sum of force of an elastic central force directed towards the origin, and gravity, which by choice of the orientation of the coordinate system, points in the positive y-direction. Friction of any kind (air, in pivot point) can be disregarded.

Newtons's equation of motion:
equation 1: mx''=-\frac{\partial V}{\partial x}
equation 2: my''=-\frac{\partial V}{\partial y}-mg

With y pointing downward, the force of gravity is mg in equation 2. my''=-\frac{\partial V}{\partial y}+mg
ojb89 said:
Gravity: g=9.81 m/s^2
Potential energy of the rod: V(r)=0.5*k*(r-L)^2, where r=\sqrt{x^2+y^2}
Length: L=1 m (length of rod in absence of external force)
We see from these equations that the solution does not depend separately on k and m, but only the combination w^2=\frac{k}{m}.

Homework Equations


a)[/B] Here we shall on look at the pendulum moving in vertical direction (x(t)=0). I need to derive the equation of motion in y-direction (in other words I need to show of to get equation 2).
But I'm having problem figure out how I can get it like equation 2. More in attempt of solution.

b) Compute the equilibrium of length L_r for this case.

c) Show that the solution of the equation of motion is an oscillation, up and down about the equilibrium with angular frequency w

The Attempt at a Solution


a)[/B] So the pendulum will act like a elastic spring with a mass. The two forces acting on the pendulum in each direction. The gravity force which we can write F_g=mg. And the force because of the potential energy which we can write F_u=-\frac{\partial V}{\partial y}.
I know we can use Newton's second law: \sum F=ma. And y''=a. But I'm having trouble with the how to set it up. From the problem description I read that F_g is positive and F_u is negative.
It is not negative, but opposite to the change of the length. Fu=-k(y-L)
ojb89 said:
This gives the the sum of forces F_g-F_u=my''.
NO, it should be F_g+F_u=my''
 
ehild said:
With y pointing downward, the force of gravity is mg in equation 2. my''=-\frac{\partial V}{\partial y}+mg

It is not negative, but opposite to the change of the length. Fu=-k(y-L)

NO, it should be F_g+F_u=my''

So the formula for equation in motion for y-direction (my''=-\frac{\partial V}{\partial y}-mg) that was written in the problem description is wrong based on the choice of the direction of y?
It should be my''=-\frac{\partial V}{\partial y}+mg ?
I just need to get this confirmed.

So F_u goes in the same direction as F_g since both are positive? Sorry for asking stupid question. But I'm not familiar with potential energy and the force created by it. All I know is that the force created by potential energy is -\frac{\partial V}{\partial y}.
 
ojb89 said:
So the formula for equation in motion for y-direction (my''=-\frac{\partial V}{\partial y}-mg) that was written in the problem description is wrong based on the choice of the direction of y?"
Yes.
my" = mg +Fu, the sum of gravity and the elastic force of the spring.
ojb89 said:
So F_u goes in the same direction as F_g since both are positive? Sorry for asking stupid question. But I'm not familiar with potential energy and the force created by it. All I know is that the force created by potential energy is -\frac{\partial V}{\partial y}.

No, the elastic force is -dV/dy. And how is the elastic potential V related to y?
If you have difficulties with the potential, remember Hook's Law. The spring force is opposite to the change of length of the spring. If the mass stretches the spring, the length of the spring increases, y-L is positive, so the force is negative. In general, the force a spring exerts on a body attached to it is F=-k(y-L). That force is negative, if y>L and positive, if x<L.

upload_2016-11-1_15-0-26.png
 

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