Single Degree of Freedom of Vibration - Undamped and Damped


 

tex2html_wrap_inline107 Statement of the problem

Free vibration is the most fundamental and simplest problem. Here we look at a simple mass-spring system to simulate such motion. As you may expect that displacement of the mass is so called ``harmonic motion'' which can be represented by trigonometry functions sin or cos.

When an viscous damper is added to a free vibration system, it results a decaying oscillation and the system would eventually come to rest. The viscous damper is a dissipation mechanism which is caused by the viscous fluid inside the dashpot. For most dashpots, the rate of extension is proportional to the applied force through a damping constant c. Here we compare the two systems.
 

tex2html_wrap_inline107 Exercises

Under-damping
  1. By moving the Slider or input a value in the box, set the damping ratio zeta=0.1, Run the program until the system almost stop vibrating then Stop it.
  2.  Go to File and Export the Meter Data to a file. Using the Excel to plot the displacement and velocity v.s.. time, measure the time when system almost stop its vibration.
Critical damping
  1. By moving the Slider or input a value in the box, set the damping ratioc=1.0, Run the program until the system stops vibrating then Stop it. Now what is the difference between this case and the case of under-damping?

  2.  Go to File and Export the Meter Data to a file. Using the Excel to plot the displacement and velocity v.s. time, measure the time when system almost stop its vibration.

tex2html_wrap_inline121 Think Twice

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