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The dipolar relaxation, analysed by the peak of the maximum loss factor, was correlated with the vitrification determined by TMDSC.
The compound spring is shown to have a maximum loss factor which quickly reaches an asymptotic value as the tank/cylinder volume ratio increases.
In the optimal lay-up design problem, a layerwise optimization (LO) method is applied to the plates comprised of two different orthotropic materials, and the optimal fiber orientation angles are determined to obtain the maximum loss factor in the fundamental mode.
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The optimal damping set could be found in a structure, in its fundamental vibration mode, such that the maximum modal loss factor of the system is achieved.
The P VDF-TrFE-CTFE) thin film with 2.75 wt% oxidized CB shows 1.6 fold increased dielectric constant and maximum P VDF-TrFE-CTFEth low loss factor comP VDF-TrFE-CTFEre thinolymer.
The analysis of the damping spectra, i.e. the model describing the relation of loss factor to maximum macroscopic specimen strain εyy was drafted.
For the case of an extremely stiff outer cover, however, the maximum magnitude of the bending loss factor obtained could be of the order of 0·2.
It is concluded that the maximum magnitude of the axial loss factor, as well as the bending loss factor, for the case of a soft outer cover could be of the order of 10-2, bevense even in the bending deformation mode, the bending-induced axial deformation acts as the main source of damping when a comparatively soft outer cover is chosen.
By using this approach to the cantilever beam problem one theoretically derives the relationship between the loss factor and the maximum stress amplitude in each mode of vibration.
It is found that the relationship between the loss factor and the maximum stress amplitude is very similar for each mode of vibration when the modes vibrate with equal stress amplitude.
A maximum in dissipated energy and in the loss factor is observed around 0·1 Hz.
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