Dynamic modulus (sometimes complex modulus ) is the ratio of stress to strain under vibratory conditions (calculated from data obtained from either free or forced vibration tests, in shear, compression, or elongation). It is a property of materials.
[pdf] A high storage modulus indicates that a material behaves more like an elastic solid, while a low storage modulus suggests more liquid-like behavior. The ratio of storage modulus to loss modulus can provide insight into the damping characteristics of a material.
[pdf] For a good PSA with high cohesive strength, the storage modulus (G') at room temperature has a value of 5x10 4 to 2x10 5 Pa. 2 The approximate strain rates encountered in typical operations associated with the manufacture and end use of a common pressure-sensitive tape adhesive can be calculated.
[pdf] One important application of DMA is measurement of the of polymers. Amorphous polymers have different glass transition temperatures, above which the material will have properties instead of glassy behavior and the stiffness of the material will drop dramatically along with a reduction in its viscosity. At the glass transition, the storage modulus decreases dramatically and the loss modulus reaches a maximum. Temperature-sweeping DMA is often used to characterize the g. As temperature increases, the storage modulus typically decreases, while the loss modulus and damping factor increase. This is because higher temperatures provide more energy for molecular motion, leading to increased viscous behavior.
[pdf] is studied using where an oscillatory force (stress) is applied to a material and the resulting displacement (strain) is measured. • In purely materials the stress and strain occur in , so that the response of one occurs simultaneously with the other.• In purely materials, there is a between stress and strain, where strain lags stress by a 90 degree ( ) phase lag.
[pdf] We can use dynamic mechanical analysis to measure the modulus of the material. Instead of continuously moving all the way through the linear elastic region, beyond which Hooke's law breaks down, we carefully keep the sample in the Hookean region for the entire experiment.
[pdf] 
