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43754-AC7
Electromagnetic Properties of Block Copolymer/Inorganic Oxide Nanocomposite Materials

K. A. Mauritz, University of Southern Mississippi

Electromagnetic Properties of Chemically-Layered Materials

Research Objectives

The goal was to create materials with interesting dielectric properties to tailor absorption of electromagnetic (EM) radiation in frequency-selective fashion.  Chemical contrast between dissimilar components can generate charge polarization relaxation at interfaces more intense than relaxations due to molecular dipole re-orientation.[1]  

Broadband dielectric spectroscopy (BDS)

BDS can interrogate molecular motions over a wide frequency (f) range.[2]  Complex dielectric permittivity e* is given as follows.

e*(f) = e'(f) -  ie”(f)

e' and e are real and imaginary permittivities. e' reflects material polarizability.  eis proportional to molecular energy dissipated per cycle.

A broadband dielectric spectrometer was used over the range 0.1Hz - 3MHz at temperatures (T) from -130 to 200˚ C.

Chemically-layered Materials

Nafion precursor films were modified on one/both sides by reactions of alkyldiamines with SO2F groups. 1200 equivalent weight samples ~100 mm thick were reacted  with ethylene diamine (1,2 EDA), 1,2 propylene diamine (1,2 PDA), 1,3 propylene diamine (1,3 PDA) and 1,4 butylene diamine (1,4 BDA). The goal was to create chemically-layered films having SO2F groups on one side and sulfonamide groups on the other side, or sulfonamide groups on both sides with SO2F groups in the middle.

Conversion to the sulfonamide form proceeds according to the reaction on the left at room temperature.

Due to index of refraction contrast between modified and unmodified regions, optical microscopy can be used to observe reaction depth. 

After initial reaction, films were heated so both amine groups react with SO2F groups forming cross links.2,3 Optical micrographs of a film asymmetrically (one side) reacted with 1,4 BDA to a depth of 25mm, and a film symmetrically (both sides) reacted with EDA to a depth of 10mm both sides are in Fig.1.  These are clearly layered materials.  

FTIR/ATR spectra for unmodified control and 1,2 EDA and 1,4 BDA films symmetrically reacted for 30 min with no curing were obtained.  Both sides have the same spectra in each case.   

Figure 2 plots e vs. f and T for an unreacted film.  There are five features in order from high to low T assigned to membrane½electrode interfacial polarization, dc onductivity, a (glass transition), b and g  relaxations noted earlier.[3]  dc conductivity arises from impurity charges.  The spectral signature for this conductivity is a linear segment with slope ~1.00 on log10e - log10 f plots. 

dc
 
Figure 3 shows an e” – f –T surface for a film reacted symmetrically with 1,4 BDA to a from both surfaces without prior heat treatment.  ‘Onset of curing' refers to reactions driven by heating in sample cell. This and all modifications have additional relaxations (A1R, A2R) at temperatures higher than the control a temperature. 

All three modified films show Tg of the unmodified region and two for amine modified regions. 

(b)
 
e” – f –T surfaces for films cured 12h before BDS measurements are in Figure 4: EDA symmetrically reacted; b) 1,4 BDA symmetrically reacted.  Dashed black curves are crests of relaxation peaks over the T range and are sensitive to diamine type. A1R relaxation times are lower than those for A2R. Increased number of relaxations indicates more modes of energy absorption. The sharp change in e* at the interface has potential to cause electromagnetic wave reflection as well as inter-layer transmission .

(a)                                                                                                                                         (b)

(a)
 
 

A1R
 
A2R
 
Fig. 5.  Dynamic mechanical tan d for indicated cure times for symmetrically reacted 1,3 PDA films.
 

Dynamic mechanical analyses were performed. Generally, for all amines, A1R shifts to DMA spectra shifts to lower temperature.  Tan d vs. T at 1 Hz for indicated cure higher T with increasing cure time similar to that of BDS peaks, although A2R in times for 1,3 PDA films symmetrically reacted is in Fig. 5.  Tg of the unreacted region shifts to higher temperature, A1R relaxation diminishes in intensity and shifts to higher T and 2R

shifts to lower temperatures while the peak narrows with increased cure time.

A1R
 
a
 
Conclusions

A sulfonyl fluoride perfluoropolymer was reacted symmetrically and un-symmetrically with alkyldiamine molecules to create chemically-layered materials. Optical microscopy confirmed sharp boundaries between distinct layers and FTIR spectroscopy provided evidence of formation of sulfonamide links. BDS indicated appearance of new relaxations attributed to cross-linked layers; these relaxations were also seen in dynamic mechanical analyses.    

References


[1] Wagner, K.W. Arch. Elektrotech. 1914, 2,371.  (b) Sillars, R.W. J. Inst. Elec. Engrs. (London) 1937, 80, 378.  (c) Van Beek, L. K. H. Prog. Dielectr. 1967, 7, 69.
[2]  Kremer, F.; Schönhals, A.  Broadband Dielectric Spectroscopy  Springer: Berlin  2003.
[3]  Hodge, I. M.; Eisenberg, A. Macromolecules 1978, 11, 289-293.

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