1. Dynamic mechanical analysis
Dynamic mechanical analysis (DMA) is a technique used to study and characterize materials. It is most useful for studying the viscoelastic behavior of polymers. A sinusoidal stress is applied and the strain in the material is measured, allowing one to determine the modulus.
The temperature of the sample or the frequency of the stress are often varied, leading to variations in the modulus.
This approach can be used to locate the glass transition temperature of the material.

2. A typical DMA tester with grips to hold sample and environmental chamber to provide different temperature conditions. A sample is mounted on the grips and the environmental chamber can slide over to enclose the sample.

3. Material Functions Derived from Oscillatory Tests
In a typical sinusoidal oscillation experiment, the applied stress and resulting strain wave forms can be described as follows:
*The phase lag and amplitude ratio (σ0 / ϒ0 ) will generally vary with frequency, but are considered material properties under linear viscoelastic conditions.
*For an ideal solid, δ = 0°, the response is purely elastic, whereas
*For a Newtonian fluid yielding a purely viscous response, δ = 90°
Where; σ0 is the stress amplitude
ϒ0 is the strain amplitude
δ is the phase lag (loss angle)
Figure. Sinusoidal wave forms for stress and strain functions.

4. DMA measures stiffness and damping (sönümleme), these are reported as modulus and tan delta. Because sinusoidal stress is applied, modulus can be expresesed as;
in-phase component, the storage modulus (E‘) and
out of phase component, the loss modulus (E")
Storage modulus (E‘) is a measure of elastic response of a material. It measures the stored energy.
Loss modulus (E") is a measure of viscous response of a material. It measures the energy dissipated as heat.

5. Tan delta is the ratio of loss to the storage and is called damping
Tan delta is the ratio of loss to the storage and is called damping. It is a measure of the energy dissipation of a material. It tells us how good a material will be at absorbing energy. Basically tan delta can be used to characterize the modulus of the material. Delta should range between 0° and 90° and as delta approaches 0° it also approaches a purely elastic behaviour. As delta approached 90° the material approaches a purely viscous behaviour. The tan of delta is defined below: tan(delta) = E"/E' E" = loss modulus E' = storage modulus

6. Assume that you apply a load to a polymer, some part of the applied load is dissipated by the energy dissipation mechanisms ( such as segmental motions) in the bulk of polymer , and other part of the load is stored in the material and will be release upon removal of the load (such as the elastic response of a spring!).
Increasing Tan delta indicates that your material has more energy dissipation potential so the greater the Tan delta, the more dissipative your material is.
Decreasing Tan delta means that your material acts more elastic now and by applying a load, it has more potential to store the load rather than dissipating it!
For example, in case of nano-composites ( and filled polymers), increasing the nano-particle content diminishes the value of Tan delta as nano-particles impose restrictions against molecular motion of polymer chains (due to the adsorption of polymer chain on the surface of the particles) resulting in more elastic response of the material.

8. For example, the DMA curve of polycaprolactone measured at a meachnical vibration frequency of 1 Hz is shown below:
The drop in storage modulus (E') and peak in damping factor (tan delta) between -60 and -30°C is due to the glass transition (Tg) of the amorphous polymer in this semi-crystalline material. Above 50°C the sample begins to melt and flow, thus loosing all mechanical integrity. Below the Tg small peaks are evident in the tan delta curve at -80 and -130°C. These are the beta and gamma transtions in this polymer (the glass transition is known also as the alpha transition) and are caused by local motion of the polymer chains as opposed to large scale co-operative motion that accompanies the Tg. These small transitions are very difficult to observe by DSC but are often very important in determining the impact resistance of the polymer.

9. Lower crosslinked thermoset has a lower Tg and the storage moduli begins to decrease at much lower temperature. Also in the transition region, the loss modulus peak occurs at a lower temperature for the lightly crosslinked thermoset.
The major difference may be observed in the dynamic moduli in the rubbery plateau region.  The highly crosslinked thermoset has larger storage and loss moduli indicating the tighter network structure and higher stiffness.

10. Resilience Testing
Resilience of a rubber compound is a measurement of how elastic it is when exposed to various stresses. Measurement of a material’s resilience can assist engineers and scientists with choosing the right material for a given application.
Resilience is the ratio of energy released in deformation recovery to the energy that caused the deformation.  One test method is the Bayshore Resilience method. It calls for the dropping of a weighted ball from a specified height onto a given material sample. The rebound height of the ball is then measured and used to determine how resilient the material is to the stress.  The result is an indicator of hysteretic energy loss.  The percent rebound measured in the test is inversely proportional to hysteretic loss.
Another common method is Dynamic Mechanical Analysis (DMA) where stresses are applied to a given material and the strain in the sample is measured. 

11. Dynamic Mechanical Analysis: A Practical Introduction, Second Edition Yazar: Kevin P. Menard