2nd order ODE: modeling a spring

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SUMMARY

The discussion centers on modeling a spring-mass-damper system using a second-order ordinary differential equation (ODE). The spring constant is 6 N/m, the mass is 3 kg, and the damping constant is 1 N·s/m. The correct form of the differential equation is derived as 3x'' + 1x' + 6x = 0, where x denotes the displacement from the equilibrium position. The participants clarify that the mass (m) is given as 3 kg and emphasize the importance of including only real forces in the equation of motion.

PREREQUISITES
  • Understanding of Newton's Second Law of Motion
  • Familiarity with differential equations, specifically second-order ODEs
  • Knowledge of spring-mass-damper systems
  • Basic concepts of forces, including damping and spring forces
NEXT STEPS
  • Study the derivation of second-order differential equations in mechanical systems
  • Learn about the applications of damping in engineering, particularly in spring systems
  • Explore numerical methods for solving ordinary differential equations
  • Investigate the effects of varying spring constants and damping coefficients on system behavior
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Mechanical engineers, physics students, and anyone involved in modeling dynamic systems, particularly those focusing on spring-mass-damper systems.

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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