Engineering Dynamics: Connected Systems

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SUMMARY

The discussion focuses on analyzing a dynamic system involving a uniform bar ABCD, supported by springs and connected to another beam EFG. The key components include a mass of 4.25kg at ABCD, springs with stiffness values of 12kN/m and 2kN/m, a torsional spring of 100Nm/rad at pivot B, and a damper with a coefficient of 6kNs/m. Participants suggest calculating the equivalent mass-spring-damping system at point A and determining the natural frequency, emphasizing the importance of developing a displacement relationship among all points in the system.

PREREQUISITES
  • Understanding of mass-spring-damping systems
  • Knowledge of torsional spring constants
  • Familiarity with dynamic system analysis
  • Ability to develop displacement relationships in mechanical systems
NEXT STEPS
  • Research methods for converting torsional spring constants to linear equivalents
  • Learn about calculating natural frequencies in multi-body systems
  • Study the principles of dynamic equilibrium in mechanical systems
  • Explore advanced topics in mechanical vibrations and damping techniques
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Mechanical engineers, students studying dynamics, and professionals involved in system dynamics analysis will benefit from this discussion.

VonDanglewanger
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Homework Statement


A uniform bar ABCD having a mass of 4.25kg is pivoted at B shown in Figure below. The bar ABCD is
supported at A and D by springs having stiffness’s of 12kN/m and 2kN/m respectively. A torsional spring
of stiffness 100Nm/rad is also present at the pivot B and a damper is located at C having a coefficient of
damping of 6kNs/m. A discrete mass of 6.75kg is at D. Beam ABCD is connected to another beam EFG by
Link DG. The Link has negligible mass. Beam EFG is also uniform and has a mass of 7.1kg/m and is pivoted
at E and carries a mass of 8kg and a spring of stiffness 10kN/m at F. Determine:

(a) the equivalent mass-spring-damping system at A;
(b) the natural frequency of the system.

upload_2014-10-20_11-28-13.png


My thoughts at a solution involve moving the mass and spring from F to D to find the equivalent mass-spring system at D. I would then calculate the equivalent mass of lever EFG, which I believe would be transmitted through lever DG to point D. Adding the equivalent mass of lever EFG to the mass at D would give me a new value for the equivalent mass at D which means I could treat the whole thing as a linear system and work back from D referring everything to point A as instructed.

Question: Does this appear to be a logical solution? What do I do about the torsional spring at pivot B, can I somehow convert it into a linear spring constant?
 
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The way you state it doesn't sound correct.

For example, I am not entirely sure what you mean by "moving the mass and spring from F to D". If you literally mean this then I don't think this will give you the correct answer.

The correct approach I think would be to develop a displacement relationship between all the points.

BTW, there appear to be some typos in the written description since it doesn't match the diagram 100%.
 

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