Coupled Vertical Spring-Mass Systems

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SUMMARY

The discussion focuses on the dynamics of coupled vertical spring-mass systems, specifically analyzing the equations of motion for two masses, \(m_1\) and \(m_2\), under the influence of gravitational and spring forces. The equations provided include a second-order ordinary differential equation (ODE) for each mass, with the potential to simplify the system into a single fourth-order ODE. Key equations include the static equilibrium conditions and the dynamic equations of motion, which are derived from displacing the masses from their equilibrium positions.

PREREQUISITES
  • Understanding of Newton's second law of motion
  • Familiarity with ordinary differential equations (ODEs)
  • Knowledge of static equilibrium in mechanical systems
  • Basic concepts of spring mechanics, including Hooke's law
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  • Study the derivation and solution methods for second-order ordinary differential equations
  • Learn about coupled oscillations in mechanical systems
  • Explore numerical methods for solving ODEs, such as the Runge-Kutta method
  • Investigate the stability analysis of dynamic systems
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Students and professionals in mechanical engineering, physicists, and anyone interested in the analysis of dynamic systems involving springs and masses.

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Homework Statement
A vertical spring mass system is attached in series with another vertical spring mass system. Masses of both objects are different and so are the spring constants of both springs. y1 and y2 are the coordinates measured from the rest position of mass 1 and mass 2 respectively.

I have identified the forces on both masses using free body diagram, but I do not know how to proceed next.
My final goal is to set up matrix equation and then solve for normal frequencies.
Relevant Equations
Mq'' = Kq
How should I proceed?
112.jpeg
 
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I'm getting ##\downarrow^+##:

$$m_1 \ddot y_1 = m_1 g - k_1( y_1 - l_1) + k_2 \Big[ (l_2 + y_2) - (l_1 + y_1) \Big]$$

$$m_2 \ddot y_2 = m_2 g - k_2 \Big[ (l_2 + y_2) - (l_1 + y_1) \Big]$$
 
As for solving the system, another option is to solve a single fourth order ODE by either solving ##y_1## in terms of ##y_2## and computing ##\ddot y_1## or visa-versa.
 
Actually, I blundered too.

1670942861162.png


Let ##l_1## and ##l_2## be the unloaded free lengths of the springs. The equation for static equilibrium ( LHS of the diagram)

$$ m_1 g - k_1( y_1 - l_1) + k_2( y_2 - l_2) = 0 \tag{1} $$

$$ m_2 g - k_2( y_2 - l_2 ) = 0 \tag{2}$$

Now, displace ##m_1, m_2## from equilibrium by some distance ## \Delta y_1, \Delta y_2## respectively. What follows is that:

$$ m_1 \ddot{\Delta y_1} = m_1 g - k_1( y_1 + \Delta y_1 - l_1 )+ k_2( y_2 + \Delta y_2 - \Delta y_1 - l_2) \tag{3}$$

Now, expand (3) as follows:

$$ m_1 \ddot{\Delta y_1} = \cancel{ \boxed{m_1 g - k_1( y_1 - l_1) + k_2( y_ 2 - l_2)}}^0 -k_1 \Delta y_1 + k_2( \Delta y_2 - \Delta y_1)$$

Notice the boxed terms are identically 0 by (1). It follows that:

$$ m_1 \ddot{\Delta y_1} = -k_1 \Delta y_1 + k_2( \Delta y_2 - \Delta y_1) \tag{4}$$

I'll let you determine the result for ##m_2##.
 
Last edited:

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