Spring Mass Dashpot System
Spring mass dashpot system. If a spring-mass-dashpot system is subjected to excitation by a constant harmonic force then at resonance its amplitude of vibration will be IES-1999 a infinity b inversely proportional to damping c directly proportional to damping d decreasing exponentially with time 23. Now we consider a mass on a spring in which there is friction. We will consider three types of forcing applied to the spring-mass system as shown below.
A mass spring dashpot subsystem in a falling container of mass m 1 is shown. There is only one position in this system defined by the variable x that is positive to the right. Ii Draw the arrows vectors to represent the direction of Forces being applied to each component.
Another common misconception is that the model shown in Figure 12 is re-lated to only a particular physical system which consists of a lumped mass attached to a tension-compression spring with a dashpot acting in paral-lel. Spring elastic element Damper frictional element Mass inertia element Translational and rotational versions These are passive non-energy producing devices Driving Inputs force. The coefficients represent parameters of the system -- for example mass damping constant spring constant.
The spring exerts a force given by ky x where k is the spring constant and the dashpot exerts a force given by bx0 against the motion of the mass with damping coefficient b. The system is subject to constraints not shown that confine its motion to the vertical direction only. The spring friction between the mass and the guides if any that constrain its motion to one dimension or a mechanical device dashpot that imparts a resistive force to the mass.
The basic vibration model of a simple oscillatory system consists of a mass a massless spring and a damper. A structure is modelled as the spring-mass-dashpot system shown below. Suppose that the mass in a mass-spring-dashpot system with m 10 c 7 and k 1 is set in motion with x0 0 and x0 5.
A Determine the natural frequency of the undamped system in both rads and Hz and its natural period. In any case we assume that the resistive force is proportional to the speed dudtof the mass. For such a system is its natural frequency of vibration.
B Given the damping coefficient c calculate the damping ratio. I Break down the system into each component.
There are two forces acting on the mass.
It is subject to a force f t forcing the motion as in Figure 142. Now we consider a mass on a spring in which there is friction. A mass spring dashpot subsystem in a falling container of mass m 1 is shown. The spring exerts a force given by ky x where k is the spring constant and the dashpot exerts a force given by bx0 against the motion of the mass with damping coefficient b. The system can then be considered to. The basic vibration model of a simple oscillatory system consists of a mass a massless spring and a damper. B Given the damping coefficient c calculate the damping ratio. A Find the position function xt and show that its graph looks as indicated in the figure. So the di erential equation for the mass spring is now m d2x dt2 kx dx zdt friction force.
A mass spring dashpot subsystem in a falling container of mass m 1 is shown. The mass could represent a car with the spring and dashpot representing the cars bumper. The frequency-dependent spring and dashpot properties are generated by a FORTRAN program using the basic model constants for the mass m and for the spring In addition the parameters b138366 23508 в 10 2 and 65001 в 10 2 are used. B Find how far the mass moves to the right before starting back toward the origin. This discussion on If a spring-mass-dashpot system is subjected to excitation by a constant harmonic force then at resonance its amplitude of vibration will be aInfinitybInversely proportional to damp in cDirectly proportional to dampingdDecreasing exponentially with timeCorrect answer is option A. Spring elastic element Damper frictional element Mass inertia element Translational and rotational versions These are passive non-energy producing devices Driving Inputs force. 6 In this example it is natural to regard y rather than the right.
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