Passive Infrared Spectroscopy with a Planar Array to Detect Trace Quantities of Gas Phase Chemical Warfare Agents and Other Toxic Materials

 

 

 

 

 

 

 

In order to provide a high surface area membrane to concentrate gas phase molecules for examination with the IR spectrograph,electrospinning of fibers of various commodity materials was undertaken. These included poly(styrene) (PS) and a polyamide (Nylon 6). Both the fiber size and, in the case of PS, the density of nanopores on the fiber surface could be varied so as to optimize the surface to volume ratio. Shown in Fig. 1 is a field emission scanning electron microscope (FE-SEM) picture of an electrospun fiber membrane of Nylon 6. The fiber diameters range between 2-3 microns and the fibers themselves are quite uniform. On the right of Fig. 1 is the FT-IR and PA-IR spectra of the Nylon 6 fibrous membrane. Although the intensities of the bands below 1500 cm-1 compare favorably between the two techniques, the FTIR bands in the amide I (1655 cm-1) and amide II (1545 cm-1) region appear more intense than their PA-IR counterparts. This is because the FT-IR spectrum was recorded through a thicker part of the membrane and Beer's law is no longer valid at absorbance values > 1.5 a.u. The main "take away" point is that the PA-IR spectrum was recorded in seconds compared to tens of minutes for the FT-IR spectrum1,2.

 

 

 

FE-SEM of Nylon 6 Fibers

IR of Electrospun Nylon 6

Fig. 1. FE-SEM of electrospun fiber membrane of Nylon 6 (left) and a comparison of its FT-IR and PA-IR spectra (right).

 

 

 

 

 

 

 

The speed advantage of the PA-IR technique is also demonstrated in the left side of Fig. 2 where the spectra of dimethylphosphonate, (HP(CH3)2(O)) (DMP), obtained in a 10 cm. gas cell as a function of pumping time is shown. Each spectra is recorded in 8.7 millisec except the two weakest, which were recorded in 87 milliseconds. The strong υa(P-O-C) band at 985 cm-1 is clearly observed even at the lowest concentrations.

 

 

 

When DMP (a Sarin surrogate) is adsorbed onto the Nylon 6 membrane, the resulting spectra (blue - shown on right of Fig.2) can be seen to contain additional bands due the presence of the DMP adsorbent. Subtracting the Nylon 6 spectrum produces a spectrum of adsorbed DMP that closely resembles that of the gas phase except for a shift of many of the bands to lower frequency due to the interaction of DMP molecules with non- hydrogen bonded C=O and N-H bonds on the surface of the Nylon 6 fibers. Hence combining the speed of the PA-IR technique and the amplification of a high surface area electrospun membrane can provide a rapid method for the detection of chemical warfare agents (CWAs).

 

 

 

 

 

 

Fig. 2. Gas phase spectra (left) of DMP obtained in a 10 cm. gas cell as a function of pumping time. Each spectra is recorded in 8.7 millisec except the two weakest, which were recorded in 87 millisec. Right-spectra of Nylon 6 membrane, DMP adsorbed on membrane and difference (bottom) spectrum.

 

 

 

Hence this demonstrates that the high surface area electrospun membrane concept is a valid and valuable strategy for amplifying the presence of gaseous and liquid molecules by concentrating them on the fiber surface.

 

 

 

 

 

 

 

 

 

 

 

References

 

 

 

1)"Design and Performance of a Planar Array Infrared Spectrograph that Operates in the
3400 to 2000 cm-1 Region", Elmore, D. L.; Tsao, M. W.; Frisk, S.; Chase, D. B.; J.F., Rabolt. Applied Spectroscopy 2002, 56, 145.

 

 

 

2) "Performance and Application of a New Planar Array Infrared Spectrograph Operating in the Mid-Infrared (2000-975 cm1) Fingerprint Region", C. Pellerin, C. Snively, D. B. Chase, and J. F. Rabolt Applied Spectroscopy 2004, 58, 639-646.