2nd Order Linear - Modeling Spring Oscillation

In summary: I was wrong.In summary, the conversation discusses Newton's second law of motion and Hooke's Law in relation to a mass attached to a spring at equilibrium. It also addresses how to get the equation mx''+kx=0 and clarifies the roles of "s" and "x" as the distance displaced by the mass and the natural length of the spring, respectively. It also explains the concept of forces at equilibrium and how they change when the mass is pulled past the equilibrium point. The conversation ends with a clarification of the equation mx''+kx=0 and an apology for not being able to explain it well.
  • #1
jlawson
5
0
To my knowledge I assume:

Newton's second law of motion :

F = ma = mx''

Hooke's Law

F = ks where s is the distance displaced by the mass.

When a mass is attached to the spring, the new spring force is:

F = k(s+x)

While the downward force is still:

mg

If the two forces are equal and opposite, then:

mg = k(s+x) after simplifying

kx=0

***********************

My question is: From kx=0, how do I get:

F=kx

I know how this leads to the final equation mx''-kx=0

But do we just assume that kx is a force and set it equal to F. I just don't understand the reasoning.
 
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  • #2
jlawson said:
To my knowledge I assume:

Newton's second law of motion :

F = ma = mx''

Hooke's Law

F = ks where s is the distance displaced by the mass.

When a mass is attached to the spring, the new spring force is:

F = k(s+x)
What do "s" and "x" mean here? In the first two equations, they are essentially the same. Do you mean that s is the "natural length" of the spring?

While the downward force is still:

mg

If the two forces are equal and opposite, then:

mg = k(s+x) after simplifying

kx=0
What? mg= ks+ kx so kx= mg- ks. How did that become 0? At the equilibrium position, if s is the length of the spring when hanging with mass m attached (NOT quite the same as the "natural length"), then that will be correct and the conclusion would be that x= 0- that we are at the equilibrium position.

***********************

My question is: From kx=0, how do I get:

F=kx
You don't. F= k(s+ x)- mg.

I know how this leads to the final equation mx''-kx=0

But do we just assume that kx is a force and set it equal to F. I just don't understand the reasoning.
Perhaps because that is NOT the correct result. There is a gravitational force of -mg, which is always negatve and so always downward, and a spring force of -k(s+x), which is negative if x< -s, if x is above the "natural length", and so downward, but positive if x> -s, s is below the "natural length", and so upward.
"mass times acceleration equals force" gives mx''= -k(s+x)- mg which is the same as mx''+ kx= -ks- mg.

Now, with that given, the standard method of solving such an equation is to find the general solution to the "associated homogeneous equation", x''+ kx= 0, and add to that any specific solution to the entire equation. That may be where "x''+ kx= 0" is coming from.
 
  • #3
What do "s" and "x" mean here? In the first two equations, they are essentially the same. Do you mean that s is the "natural length" of the spring?

Start with any spring attached to the ceiling of room. Attach a mass to this spring. The spring will stretch downward due to the mass attached to it. Eventually the mass, attached to the spring, will reach an equilibrium point. At this point, there are two forces acting on the mass: The force of gravity puling the mas down, and the force of the spring puling the mass up.

For this problem, we assume that the downward direction is positive, while the upward direction is negative.

Downward force: F=mg

Upward force: Using Hooke's Law: the spring itself exerts a restoring force, F, opposite to the direction of the elongation, s. S is the distance the spring stretched (the length of the spring after attaching the mass - the length of the spring before attaching the mass).

*See figures 1 and 2 of my attachment.

Simply stated: F=ks, where k is a constant of proportionality.

At equilibrium, the two opposing forces are equal.

mg=ks --> mg-ks=0

Then, we use our hands to pull the mass down, past it's equilibrium point.

The two forces acting on the object are now:

Downward: F=mg

Upward: F=k(s+x) = ks+kx

If the two forces are equal:

mg = ks + kx
mg - ks - kx = 0 In this system, we know that mg-ks=0, so
0 - kx = 0
 

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  • #4
If the two forces are equal:

mg = ks + kx
mg - ks - kx = 0 In this system, we know that mg-ks=0, so
0 - kx = 0

Oops, That's wrong but I figured it out.

The total force acting on the mass, when it's stretched down past equilibrium, is:

F = mg - k(s+x)

The upward force "-k(s+x)" is negative and the downward force "mg" is positive because we assumed upward direction was negative and downward direction was positive. Simplifying:

F = mg - ks - kx Again, in this system we know that mg-ks=0, so
F= -kx The total force acting on the mass at a distance x from the
equilibrium.

Once we let go of the mass, the spring will bounce up and down, or oscillate. Force in motion is characterized by F=ma

ma = -kx Acceleration can be expressed as the 2nd derivative of x with respect
to time
mx'' = -kx

mx'' + kx = 0

Thanks for trying to help. I'm sorry I'm not good at explaining this stuff. I had assumed that this problem was a standard 2nd order linear differential equation application and that most people would know what I was trying to say.
 
  • #5


As a scientist, it is important to understand the reasoning behind mathematical equations and not just accept them blindly. In this case, the equation kx=0 comes from the equilibrium condition, where the forces acting on the mass are balanced and the mass is not accelerating. From Newton's second law, we know that the net force on an object is equal to its mass multiplied by its acceleration. In this case, the net force is equal to the spring force (F=ks) minus the gravitational force (mg). When these forces are balanced, the mass is not accelerating and we can set the net force equal to zero. This gives us the equation ks-mg=0. From Hooke's Law, we know that the spring force is also equal to kx, so we can substitute kx for F in our equation. This gives us kx-mg=0, which can be rearranged to give us kx=mg. Since the mass is not accelerating and the net force is zero, we can set kx equal to zero. This leads to the final equation mx''-kx=0, which is the equation for a second order linear system modeling spring oscillation. In summary, we do not simply assume that kx is a force and set it equal to F, but rather we use the principles of equilibrium and Hooke's Law to derive the equation.
 

Related to 2nd Order Linear - Modeling Spring Oscillation

What is a 2nd Order Linear Model?

A 2nd Order Linear Model is a mathematical representation of a physical system or phenomenon that can be described using a second-order differential equation. This type of model is commonly used to study the motion of objects that are subjected to forces, such as a spring oscillation.

What is Spring Oscillation?

Spring Oscillation is a type of motion in which a spring attached to an object is compressed or stretched, causing the object to oscillate back and forth around a resting position. This type of motion is described by a second-order linear differential equation and is commonly observed in various systems such as mechanical springs, electrical circuits, and pendulums.

How is Spring Oscillation modeled using a 2nd Order Linear equation?

A spring oscillation can be modeled using the equation: mx'' + bx' + kx = 0, where m is the mass of the object attached to the spring, b is the damping coefficient, and k is the spring constant. This equation is derived from Newton's Second Law of Motion and takes into account the forces acting on the system, including the restoring force of the spring and any external forces.

What are the key parameters in a 2nd Order Linear Model for Spring Oscillation?

The key parameters in a 2nd Order Linear Model for Spring Oscillation are the mass of the object attached to the spring, the damping coefficient, and the spring constant. These parameters affect the behavior of the system and can be adjusted to study different scenarios, such as the effect of different masses or damping on the oscillation frequency.

How is the motion of a spring described using a 2nd Order Linear Model?

The motion of a spring can be described using a 2nd Order Linear Model by solving the differential equation to obtain a function that represents the position of the object over time. This function can be graphed to visualize the oscillation of the object, and various properties, such as amplitude, frequency, and period, can be calculated to further analyze the motion of the spring.

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