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The Use of PA-IR for
Dynamic Measurements: Dynamic Infrared Linear Dischroism (DIRLD) of
Polymeric Films
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When infrared measurements are coupled with dynamic
mechanical deformation, it results in a technique that can probe
polymeric structure and orientation during elastic deformation. Dynamic Infrared
Linear Dichroism (DIRLD) was originated by Marcott and Noda1 in the 1980s
and has been shown to have the potential to connect microscopic
structural properties such as orientation and conformation with
macroscopic properties such as toughness and elasticity. The basis of the
experiment is shown in Figure 1. A DMA device is inserted into the sample
chamber of an infrared absorption instrument; the sample is perturbed
with an oscillatory strain in the elastic domain, and infrared spectra
are recorded during the strain cycle. The actual changes induced by a
small amplitude strain (<0.3%) are quite small, so a very high
sensitivity measurement is needed. The original measurements were made
with single channel dispersive infrared instruments. This allowed one to
focus on a very small wavelength range and achieve the required
sensitivity. However, the measurement times were significant, often in
excess of an hour. In the 1990s the technique was extended to FT-IR with
a very complicated set of demodulation electronics2. Measurement times
were reduced to less than an hour, but sensitivity and spectral artifacts
were still a problem. Using PA-IR, this experiment can produce high
sensitivity DIRLD spectra in very short measurement times3. Figure 2
shows the PA-IR spectrum of isotactic polypropylene. Also shown are the
DIRLD in phase spectra obtained with a step-scan FT-IR and a PA-IR
instrument. The PA-IR spectrum has been inverted to allow a reasonable
comparison with the FT-IR results. The acquisition time for the FT-IR
experiment was 48 minutes. The acquisition time for the PA-IR experiment
was 48 seconds. The agreement between the two spectra is excellent.
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The
linearity of the measurement is shown in figure 3 where the applied
strain is increased from 0.02% to 0.14%. The peak amplitudes show the
high degree of linearity with applied strain.
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Figure 4 shows that useable DIRLD data can even be
obtained on the millisecond time scale.
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The high sensitivity and rapid temporal response of
the PA-IR measurement have been combined to make DIRLD measurements
simple, fast, and sensitive.
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References
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1) Marcott and Noda, In Handbook of Vibrational
Spectroscopy; Griffiths and Chalmers, Eds.; John Wiley & Sons Inc.:
Chichester, 2002; Vol. 4, pp 2576-2592
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2) "Step-Scan Fourier Transform Infrared Study on
the Effect of Dynamic Strain on Isotactic Polypropylene", B. O.
Budevska, C. J. Manning, P. R. Griffiths, R. T. Roginski, Applied
Spectroscopy, 1993, 47, 1843
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3) "A Faster Approach to Infrared Rheo-Optics
Using a Planar Array Infrared Spectrograph", C. Pellerin, C. M.
Snively, J. F. Rabolt and D. B. Chase, Applied. Spectroscopy., 2004, 58,
799.
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