2nd order ODE: modeling a spring

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Homework Help Overview

The discussion revolves around setting up a second-order ordinary differential equation (ODE) to model a spring-mass system. The spring has a constant of 6 N/m, and the mass attached is 3 kg, with a damping constant of 1 N s/m. The original poster is tasked with formulating the equation in terms of displacement, velocity, and acceleration.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to apply the standard form of the differential equation for a damped harmonic oscillator but expresses uncertainty about the forces involved, particularly regarding the mass and the concept of inertia. Participants question the necessity of including an "inertia" term and suggest focusing on real forces acting on the system. There is also discussion about identifying external forces and their implications for the equation.

Discussion Status

Participants are actively engaging with the original poster's approach, providing clarifications about the mass and the forces at play. Some suggest that the right-hand side of the equation could be set to zero if no external force is acting on the system, while others emphasize the importance of correctly identifying all forces involved. The conversation reflects a mix of interpretations and clarifications without reaching a definitive conclusion.

Contextual Notes

The original poster's setup assumes positive displacement indicates movement away from the wall, and there is an emphasis on ensuring that all forces are accounted for in the differential equation. The discussion highlights the importance of correctly interpreting the problem statement and the forces acting on the mass-spring system.

ReidMerrill
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Thread moved from the technical forums, so no Homework Template is shown
Suppose a spring with spring constant 6N/m is horizontal and has one end attached to the wall and the other end attached to a 3 kg mass. Suppose the friction/damping constant is 1 N s/m

Set up a differential equation that describes this system with x denoting displacement of the mass from equilibrium position and give your answer in terms of x,x', and x''. Assume that positive displacement means the mass is farther from the wall than equalibrium

I'm not sure what to do here. I'm guessing I'll need the equation

mx'' + bx' + kx = F Where mx'' = Fdamping + F spring + F inertia b is damping coefficient: 1 N m/s k is spring coefficient: 6 N/m

Where do I get m? Fdamping is 1 and Fspring is 6 right? Would I get Finertia from F=ma? Because a is not given.
 
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Hi,

You already have the acceleration a when you write ##\ddot x##.

If there is no spring, your equation of motion reads ##F = ma = m\ddot x##. In that case, what is F ?

Are there other (external) forces at work, except for the spring and the damping force ?
 
Why do you think you need a "Finertia" term? Newton's Second Law only involves the sum of real forces; no fictional forces are to be included. Draw the FBD and include in your force sum on the actual forces present.
 
BvU said:
Hi,

You already have the acceleration a when you write ##\ddot x##.

If there is no spring, your equation of motion reads ##F = ma = m\ddot x##. In that case, what is F ?

Are there other (external) forces at work, except for the spring and the damping force ?

I don't think so.
 
You asked "where do I get m?" but the problem statement said that one end of the spring was attached to a 3 kg mass. That is where you get m.
 
You missed the 'in that case, what is F?' :smile:. I was fishing for the answer: 'the externally applied force'
ReidMerrill said:
I don't think so.
So that means in your differential equation the right-hand side can be set to 0 and ##m\ddot x = ## the two forces in the story (##\beta\dot x## and ##kx##) , each with the proper sign
 
BvU said:
You missed the 'in that case, what is F?' :smile:. I was fishing for the answer: 'the externally applied force'
So that means in your differential equation the right-hand side can be set to 0 and ##m\ddot x = ## the two forces in the story (##\beta\dot x## and ##kx##) , each with the proper sign
So the equation would be 3x'' + 1x' + 6x =0 ?
 
Only if you willingly omit the dimensions -- generally not a wise thing to do :smile:. Any doubt remaining ?
 

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