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The fabric is modelled as a network of nodal masses connected by one-dimensional viscoelastic elements.
The biomechanical model consists of several lumped masses connected by linear spring and dampers.
The system consists of two lumped masses connected by a coupling spring.
A chain of point masses connected by linear springs and sometimes dashpots is considered.
In this context, a diatomic molecule may be modeled as two masses connected by an ideal spring.
The model of the system is formed by two masses connected by a nonlinear spring and a viscous damping.
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It is modeled as three equal end-masses connected by a uniform-mass straight tether.
The mass damper consists of a viscous damper and a mass connected by springs and a rigid bar.
The harvester is made of a sprung mass (body mass) and an unsprung mass (wheel mass) connected by a piezoelectric bar transducer which is equivalently modeled as a suspension spring and a damper in a mathematics model.
A simple two-degree-of-freedom system consisting of an absorbing mass connected by springs to a drive mass is introduced and used to interpret the vibration behavior of the sandwich structure with resonators.
This mass develops distally into a thick band lining the bundle concavity (Figs. 5e, 6a, b), and may further differentiate into two lateral masses connected only by a rather thin strip (Fig. 5f, g).
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