リケラボ論文検索は、全国の大学リポジトリにある学位論文・教授論文を一括検索できる論文検索サービスです。

リケラボ 全国の大学リポジトリにある学位論文・教授論文を一括検索するならリケラボ論文検索大学・研究所にある論文を検索できる

リケラボ 全国の大学リポジトリにある学位論文・教授論文を一括検索するならリケラボ論文検索大学・研究所にある論文を検索できる

大学・研究所にある論文を検索できる 「Material Evaluation of Cellulosic Materials by Terahertz Time-domain Spectroscopy」の論文概要。リケラボ論文検索は、全国の大学リポジトリにある学位論文・教授論文を一括検索できる論文検索サービスです。

コピーが完了しました

URLをコピーしました

論文の公開元へ論文の公開元へ
書き出し

Material Evaluation of Cellulosic Materials by Terahertz Time-domain Spectroscopy

王, 晗 名古屋大学

2022.11.11

概要

With the wild use of fossil resources since the second industrial revolution, global environmental problems such as global warming and climate anomalies have now become significant challenges for human survival. Cellulose, as an important recyclable and abundant resource, the effective using and development of cellulose materials such as wood and bamboo is an essential countermeasure against global warming and other environmental issues, thus, the non-destructive evaluation of material properties is necessary. Terahertz (THz) radiation lies in far-IR radiation between microwaves and IR of the electromagnetic spectrum with a frequency range of 0.1 –10 THz, corresponding to wavelengths of 3 –0.03 mm, and terahertz time-domain spectroscopy (THz-TDS) has been developed for commercial. THz radiation is non-ionizing, safe for human bodies, and many non-conductive dry materials (wood, ceramic, paper, etc.) are transparent at THz frequency. This transparency allows for transmission imaging of many materials with sub-millimeter spatial resolution. Besides, with one measurement, the refractive index and absorption coefficient can be obtained simultaneously by calculation. Furthermore, THz radiation is responsive to optical phonons in crystalline lattices. This means that THz is very suitable to investigate cellulose crystalline and cellulose-based materials. Therefore, in this study, THz-TDS was used to investigate various porosities of cellulosic materials.

 First of all, moisture content (MC) and density influence the mechanical and physicochemical properties of wood, therefore, an accurate prediction of these properties is necessary. In the previous study, the prediction was approached by the effective medium theory (EMT) model combined with the Double Debye model to express the dielectric function of water in the cell wall of wood. However, using the Double Debye model to explain the behavior of water in the cell walls, particularly at a relatively low MC under fiber saturation point (FSP) is inaccurate, because the Double Debye model is applied to the bulk water, and when the MC is relatively low, the behavior of water in the cell wall is closer to the bound water, thus, using the Double Debye model led to a systematic underestimation of MC. In this study, by building an MC-dependent dielectric function of water in the THz region, the accuracy of the prediction model of density and MC of wood was significantly improved compared with the previous model, and the problem of systematic underestimation of MC was solved.

 Undertaking the above research, the other important properties of wood, including density, MOE, cellulose crystallinity, and microfibril angle (MFA) was attempted to predict by THz-TDS with a simpler multiple linear regression (MLR) model (compare with the EMT model using dielectric function). The density and MOE can be predicted well. However, the prediction accuracy of MFA and cellulose crystallinity was limited. This result indicated the possibility of using THz-TDS to predict the physical properties of cellulosic materials simultaneously. Thus, in order to improve the prediction accuracy of MFA and cellulose crystallinity, the following study is focused on the optical properties in the THz region of various cellulose crystallines.

 It has reported of the absorption coefficient spectra of some polysaccharide crystals, including fructose, glucose, and sucrose. However, the virous crystalline of cellulose has not been studied in detail in the THz region. In this study, native cellulose Iα and Iβ allomorphs were investigated by THz-TDS and X-ray diffraction (XRD). In the XRD patterns, the difference between these allomorphs was difficult to identify since there are only slight changes in peak positions that can be observed. On the other hand, cellulose I α and Iβ showed a characteristic absorption at 2.38 THz and 2.11 THz, respectively. Furthermore, different from the relative content cannot be calculated directly in the XRD patterns, the intensity of the absorption peaks in the THz region was directly correlated with the relative content of the component, which makes the evaluation of the cellulose allomorphs in the THz region is easier and simpler.

 After this, the amount of cellulose in various materials which is also an important parameter that influences the properties of the cellulosic materials was determined by THz-TDS and XRD with wood, microcrystalline (MCC) cellulose, and pseudo -wood (MCC mixed with lignin). The standard for evaluating the cellulose crystallinity has been used as the cellulose crystallinity index (CrI, related to th e relative content of cellulose in materials), which is just a relative parameter calculated from XRD patterns and the calculation was dependent on the experience of the analyst, where the available profile for the peak deconvolution is not unique. On the other hand, cellulose I regardless of I α or Iβ all showed absorption peaks around 3.04 THz, the integrated intensity of the absorption peaks at 3.04 THz was directly correlated with the amount of cellulose I, which showed a more reasonable result of the cellulose crystallinity compared with CrI. This means that the integrated intensity of the THz absorption peaks has the potential to instead of the CrI which is a relative parameter calculated from XRD becoming a new standard for evaluating the amount of cellulose crystalline in materials.

 At last, the crystalline lattice structure and the crystallinity changing of cellulose I after chemical treatment. Tracing the transformation of the crystalline structure is essential for a better understanding of the processes of industry and biosynthesis where cellulose is involved, such as viscose rayon manufacturing. In this study, the transformation of the crystalline lattice of cellulose I to cellulose II was traced by using THz -TDS and XRD. Cellulose I and cellulose II was shown a different characteristic absorption profile in the THz region, and the relative content can be expressed by the coefficient calculated from fitting the absorption coefficient spectra in the THz region. And the crystallinity changing of cellulose II after ball-milling was evaluated by the integrated intensity of the characteristic absorption peaks of cellulose II.

 In summary, THz-TDS was used for investigating various cellulosic materials. The THz signal can be measured at room temperature and does not require sample pretreatment, the measurement and analysis processes are rapid and simple compared with the XRD patterns. As the results obtained, we believe THz-TDS not only can be used to predict the properties of cellulosic materials but also has the potential to become a useful tool in the research and understanding of cellulose crystallography. Especially when analyzing the cellulose crystallinity, the results are better than XRD, which demonstrates the great potential of THz-TDS in the research of cellulosic materials.

この論文で使われている画像

参考文献

Atalla RH, VanderHart DL (1984) Native cellulose: A composite of two distinct crystalline forms. Science (80- ) 223:283–285.

Barnett JR, Bonham VA (2004) Cellulose microfibril angle in the cell wall of wood fibres. Biol Rev Camb Philos Soc 79:461–472.

Baxter JB, Guglietta GW (2011) Terahertz spectroscopy. Anal Chem 83:4342–4368.

Belton PS, Tanner SF, Cartier N, Chanzy H (1989) High-Resolution Solid-State 13C Nuclear Magnetic Resonance Spectroscopy of Tunicin, an Animal Cellulose. Macromolecules 22:1615–1617.

Bhuiyan MTR, Hirai N, Sobue N (2000) Changes of crystallinity in wood cellulose by heat treatment under dried and moist conditions. J Wood Sci 46:431–436.

Born B, Weingärtner H, Bründermann E, Havenith M (2009) Solvation dynamics of model peptides probed by terahertz spectroscopy. observation of the onset of collective network motions. J Am Chem Soc 131:3752–3755.

Bragg WH, Bragg WL (1913) The reflection of X-rays by crystals. Proc R Soc London Ser A, Contain Pap a Math Phys Character 88:428–438

de Keijser T, Mittemeijer EJ, Rozendaal HCF (1983) The determination of crystallite-size and lattice- strain parameters in conjunction with the profile-refinement method for the determination of crystal structures. J Appl Crystallogr 16:309–316.

del Cerro DR, Koso T V., Kakko T, et al (2020) Crystallinity reduction and enhancement in the chemical reactivity of cellulose by non-dissolving pre-treatment with tetrabutylphosphonium acetate. Cellulose 27:5545–5562.

Duvillaret L, Garet F, Coutaz JL (1996) A reliable method for extraction of material parameters in terahertz time-domain spectroscopy. IEEE J Sel Top Quantum Electron 2:739–745.

Ebbinghaus S, Seung JK, Heyden M, et al (2007) An extended dynamical hydration shell around proteins. Proc Natl Acad Sci U S A 104:20749–20752.

Federici JF, Schulkin B, Huang F, et al (2005) THz imaging and sensing for security applications - Explosives, weapons and drugs. Semicond Sci Technol 20:.

Ferguson B, Zhang XC (2002) Materials for terahertz science and technology. Nat Mater 1:26–33. Fischer BM, Walther M, Jepsen PU (2002) Far-infrared vibrational modes of DNA components studied by terahertz time-domain spectroscopy. Phys Med Biol 47:3807–3814.

Fujimoto T, Yamamoto H, Tsuchikawa S (2007) Estimation of wood stiffness and strength properties of hybrid larch by near-infrared spectroscopy. Appl Spectrosc 61:882–888.

Hashin Z (1983) Analysis of Composite Materials—A Survey. J Appl Mech 50:481.

Horii F, Hirai A, Kitamaru R (1987) CP/MAS13C NMR Spectra of the Crystalline Components of Native Celluloses. Macromolecules 20:2117–2120.

Horikawa Y (2017) Assessment of cellulose structural variety from different origins using near infrared spectroscopy. Cellulose 24:5313–5325.

Imai T, Sugiyama J (1998) Nanodomains of Iα and Iβ cellulose in algal microfibrils. Macromolecules 31:6275–6279.

Imai T, Sugiyama J, Itoh T, Horii F (1999) Almost pure I(α) cellulose in the cell wall of Glaucocystis. J Struct Biol 127:248–257.

Inagaki T, Ahmed B, Hartley ID, et al (2014a) Simultaneous prediction of density and moisture content of wood by terahertz time domain spectroscopy. J Infrared, Millimeter, Terahertz Waves 35:949–961. Inagaki T, Hartley ID, Tsuchikawa S, Reid M (2014b) Prediction of oven-dry density of wood by time- domain terahertz spectroscopy. Holzforschung 68:61–68.

Inagaki T, Mitsui K, Tsuchikawa S (2009) Near-Infrared Spectroscopic Investigation of the Hydrothermal Degradation Mechanism of Wood as an Analogue of Archaeological Objects. Part I: Softwood. Appl Spectrosc 63:753–758.

Jepsen PU, Møller U, Merbold H (2007) Investigation of aqueous alcohol and sugar solutions with reflection terahertz time-domain spectroscopy. Opt Express 15:14717.

Kafle K, Greeson K, Lee C, Kim SH (2014) Cellulose polymorphs and physical properties of cotton fabrics processed with commercial textile mills for mercerization and liquid ammonia treatments. Text Res J 84:1692–1699.

Kawase K, Ogawa Y, Watanabe Y, Inoue H (2003) Non-destructive terahertz imaging of illicit drugs using spectral fingerprints. Opt Express 11:2549.

Keunecke D, Novosseletz K, Lanvermann C, et al (2012) Combination of X-ray and digital image correlation for the analysis of moisture-induced strain in wood: Opportunities and challenges. Eur J Wood Wood Prod 70:407–413.

Kirkpatrick S (1971) Classical Transport in Disordered Media: Scaling and Effective-Medium Theories. Phys Rev Lett 27:1722–1725

Koch M, Hunsche S, Schuacher P, et al (1998) THz-imaging: A new method for density mapping of wood. Wood Sci Technol 32:421–427.

Kolpak FJ, Blackwell J (1976) Determination of the Structure of Cellulose II. Macromolecules 9:273– 278.

Kore PS, Pawar PP (2014) Measurements of mass attenuation coefficient, effective atomic number and electron density of some amino acids. Radiat Phys Chem 98:86–91.

Langan P, Nishiyama Y, Chanzy H (1999) A revised structure and hydrogen-bonding system in cellulose II from a neutron fiber diffraction analysis. J Am Chem Soc 121:9940–9946.

Langan P, Nishiyama Y, Chanzy H (2001) X-ray structure of mercerized cellulose II at 1 Å resolution. Biomacromolecules 2:410–416.

Langkilde FW, Svantesson A (1995) Identification of celluloses with Fourier-Transform (FT) mid- infrared, FT-Raman and near-infrared spectrometry. J Pharm Biomed Anal 13:409–414.

Lindgren LO (1991) Medical CAT-scanning: X-ray absorption coefficients, CT-numbers and their relation to wood density. Wood Sci Technol 25:341–349.

Ma T, Inagaki T, Tsuchikawa S (2017) Calibration of SilviScan data of Cryptomeria japonica wood concerning density and microfibril angles with NIR hyperspectral imaging with high spatial resolution. Holzforschung 71:341–347.

Mantsch HH, Naumann D (2010) Terahertz spectroscopy: The renaissance of far infrared spectroscopy. J Mol Struct 964:1–4.

Mourou G, Stancampiano C V., Antonetti A, Orszag A (1981) Picosecond microwave pulses generated with a subpicosecond laser-driven semiconductor switch. Appl Phys Lett 39:295–296.

Mwaikambo LY, Ansell MP (2001) The determination of porosity and cellulose content of plant fibers by density methods. J Mater Sci Lett 20:2095–2096.

Nahata A, Weling AS, Heinz TF (1996) A wideband coherent terahertz spectroscopy system using optical rectification and electro-optic sampling. Appl Phys Lett 69:2321–2323.

Nakamura K, Wada M, Kuga S, Okano T (2004) Poisson’s Ratio of Cellulose Iα and cellulose II. J Polym Sci Part B Polym Phys 42:1206–1211.

Nishiyama Y (2009) Structure and properties of the cellulose microfibril. J Wood Sci 55:241–249. O’sullvian AC (1997) Cellulose: the structure slowly unravels. Cellulose 4:173–207

Oh SY, Dong IY, Shin Y, et al (2005) Crystalline structure analysis of cellulose treated with sodium hydroxide and carbon dioxide by means of X-ray diffraction and FTIR spectroscopy. Carbohydr Res 340:2376–2391.

Oudiani A El, Chaabouni Y, Msahli S, Sakli F (2011) Crystal transition from cellulose i to cellulose II in NaOH treated Agave americana L. fibre. Carbohydr Polym 86:1221–1229.

Park S, Baker JO, Himmel ME, et al (2010) Cellulose crystallinity index: Measurement techniques and their impact on interpreting cellulase performance. Biotechnol Biofuels 3:1–10.

PETTERSEN RC (1984) The Chemical Composition of Wood. In: The Chemistry of Solid Wood. pp 57–126

Pickwell E, Wallace VP (2006) Biomedical applications of terahertz technology. J Phys D Appl Phys 39:.

Popescu MC, Popescu CM, Lisa G, Sakata Y (2011) Evaluation of morphological and chemical aspects of different wood species by spectroscopy and thermal methods. J Mol Struct 988:65–72.

Reid M, Fedosejevs R (2006) Terahertz birefringence and attenuation properties of wood and paper. Appl Opt 45:2766–2772

Ren A, Zahid A, Fan D, et al (2019) State-of-the-art in terahertz sensing for food and water security – A comprehensive review. Trends Food Sci Technol 85:241–251.

Rice A, Jin Y, Ma XF, et al (1994) Terahertz optical rectification from 〈110〉 zinc-blende crystals. Appl Phys Lett 64:1324–1326.

Schenzel K, Fischer S (2001) NIR FT Raman spectroscopy - A rapid analytical tool for detecting the transformation of cellulose polymorphs. Cellulose 8:49–57.

Shen YC, Upadhya PC, Beere HE, et al (2004) Generation and detection of ultrabroadband terahertz radiation using photoconductive emitters and receivers. Appl Phys Lett 85:164–166.

Sugino H, Sugimoto H, Miki T, Kanayama K (2007) Fine Structure Changes of Wood during Moisture Adsorption and Desorption Process Analyzed by X-ray Diffraction Measurement. Mokuzai Gakkaishi/Journal Japan Wood Res. Soc. 53:82–89

Sugiyama J, Vuong R, Chanzy H (1991) Electron Diffraction Study on the Two Crystalline Phases Occurring in Native Cellulose from an Algal Cell Wall. Macromolecules 24:4168–4175.

Takeuchi I, Tomoda K, Nakajima T, et al (2012) Estimation of crystallinity of trehalose dihydrate microspheres by usage of terahertz time-domain spectroscopy. J Pharm Sci 101:3465–3472.

Tanaka S, Shiraga K, Ogawa Y, et al (2014) Applicability of effective medium theory to wood density measurements using terahertz time-domain spectroscopy. J Wood Sci 60:111–116.

Todoruk TM, Hartley ID, Reid ME (2012) Origin of birefringence in wood at terahertz frequencies. IEEE Trans Terahertz Sci Technol 2:123–130.

Todoruk TM, Schneider J, Hartley ID, Reid M (2008) Birefringence of wood at terahertz frequencies - art. no. 70992Q. Photonics North 2008 7099:Q992-Q992\r36.

VanderHart DL, Atalla RH (1984) Studies of Microstructure in Native Celluloses Using Solid-State 13C NMR. Macromolecules 17:1465–1472.

Vieira FS, Pasquini C (2014) Determination of cellulose crystallinity by terahertz-time domain spectroscopy. Anal Chem 86:3780–3786.

Wada M, Okano T (2001) Localization of Iα and Iβ phases in algal cellulose revealed by acid treatments. Cellulose 8:183–188.

Wada M, Okano T, Sugiyama J (2001) Allomorphs of native crystalline cellulose I evaluated by two equatorial d-spacings. J Wood Sci 47:124–128.

Wada M, Okano T, Sugiyama J (1997) Synchrotron-radiated X-ray and neutron diffraction study of native cellulose. Cellulose 4:221–232.

Walther M, Plochocka P, Fischer B, et al (2002) Collective vibrational modes in biological molecules investigated by terahertz time-domain spectroscopy. Biopolym - Biospectroscopy Sect 67:310–313. Williams GP (2006) Filling the THz gap - High power sources and applications. Reports Prog Phys 69:301–326.

Yao W, Weng Y, Catchmark JM (2020) Improved cellulose X-ray diffraction analysis using Fourier series modeling. Cellulose 27:5563–5579.

Zeitler JA, Kogermann K, Rantanen J, et al (2007) Drug hydrate systems and dehydration processes studied by terahertz pulsed spectroscopy. Int J Pharm 334:78–84.

Zsigmondy R, Scherrer P (1912) Bestimmung der inneren Struktur und der Größe von Kolloidteilchen mittels Röntgenstrahlen. Kolloidchem Ein Lehrb 277:387 –409.

参考文献をもっと見る