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Thermoset Characterization Part 14: Introduction to Dynamic Mechanical Analysis (DMA)

July 14, 2014 By Jeffrey Gotro 1 Comment

Three point bend geometryAs we wrap up the characterization of thermosets series, the final topic for the next several posts will be Dynamic Mechanical Analysis (DMA).  I left this for the end of the Thermoset Characterization series since this will be a good lead-in to our next blog post series on Rheology of Thermosets.  So let’s dive into DMA.

The technique is called dynamic mechanical analysis since the sample being probed is subjected to a time-varying deformation and the sample response is measured.  In the DMA experiment, a sinusoidal time-varying strain (controlled deformation) is applied to the sample:

sinusoidal strain

1a sinusoidal strain equation

Where g  is the applied strain, go is the strain amplitude and w is the frequency.

 

The DMA instrument measures the resultant stress:

2 resultant stress

 

2A resulting stress

Where s  is the resultant stress, so is the stress amplitude and d is the phase angle.

For most polymers due to the viscoelastic nature (both viscous component and an elastic component) there is a phase lag due to the contribution of the viscous component:

3 phase lag

The phase angle is important since it is used to calculate the dynamic moduli.

For small strain amplitudes and time independent polymers (linear viscoelastic regime) the resulting stress can be written in terms of the dynamic storage modulus (E’) and the dynamic loss modulus (E”):

3 complete stress equation

The dynamic storage modulus (E’) and the dynamic loss modulus (E”) can be calculated using the following equations:

dynamic moduli equations

A typical DMA experiment is to measure E’ and E” as a function of temperature using a precise temperature-controlled oven with a linear heating ramp to the desired end temperature.  Typical heating rates are in the range of 2-5oC/minute.  DMA is useful for measuring the modulus both below and above the glass transition temperature (Tg) as well as measuring Tg and the breadth of the glass transition.  Shown below is a typical DMA curve.

typical DMA plot

Where tan d is the ratio of the loss and storage moduli:

tan delta equation

In the next post we will discuss the various experimental geometries and in a subsequent post, applications of DMA to solve various types of problems will be discussed.

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« Thermoset Characterization Part 13: Applications of TGA to Thermosets
Thermoset Characterization Part 15: Experimental Aspects of Dynamic Mechanical Analysis (DMA) »

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Polymer Innovation Blog

I’m Dr. Jeff Gotro and welcome to the Polymer Innovation Blog. Over the last 40 years I have been involved in polymer research, along with product and process development. I acquired invaluable experience working for IBM, AlliedSignal, Honeywell, Ablestik Labs (now Henkel) and in multiple consulting projects. In this blog, I (along with some guest contributors) will share our experiences, tips, and “tricks of the trade” to get more out of your innovation efforts and discuss new trends and technical advances in the polymer industry.
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