alexa The Influence of Ceramic Far-Infrared Ray (cFIR) Irradiation on Water Hydrogen Bonding and its Related Chemo-physical Properties | Open Access Journals
ISSN: 2157-7587
Hydrology: Current Research
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The Influence of Ceramic Far-Infrared Ray (cFIR) Irradiation on Water Hydrogen Bonding and its Related Chemo-physical Properties

Leung TK1,2,3*, Lin SL4, Yang TS5, Yang JC5 and Lin YS6
1Department of Physics, Fu Jen Catholic University, Hsinchuang, Taiwan
2Department of Diagnostic Radiology, Taipei Municipal Wanfang Hospital & Department of Radiology, School of Medicine, College of Medicine, Taipei Medical University, Taiwan
3Diagnostic Radiology department, Taipei Hospital, Ministry of Health and Welfare, Taiwan
4Department of Surgery, Taipei Hospital, Ministry of health and Welfare, No. 117, Su Yuan Road, Hsinzhuang, New Taipei City 242-13, Taiwan
5School of Dental Technology, Taipei Medical University, Taipei 110, Taiwan
6Department of Applied Cosmetology and Graduate Institute of Cosmetic Science, Hungkuang University, Taichung, Taiwan
Corresponding Author : Leung TK
Department of Physics, Fu Jen Catholic University
No.510, Zhongzheng Rd., Xinzhuang Dist
New Taipei City 24205, Taiwan (R.O.C)
Tel: (886) 2-89255261
E-mail: [email protected]
Received February 27, 2014; Accepted July 25, 2014; Published August 05, 2014
Citation: Leung TK, Lin SL, Yang TS, Yang JC, Lin YS (2014) The Influence of Ceramic Far-Infrared Ray (cFIR) Irradiation on Water Hydrogen Bonding and its Related Chemo-physical Properties. Hydrol Current Res 5:174. doi: 10.4172/2157-7587.1000174
Copyright: © 2014 Leung TK, et al. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
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The property of water is highly related to the earth's environment and climate change. The fundamental
dynamical process of water is include formation and breaking of hydrogen bonds. This dynamic process, so far, is still poorly understood. We investigated weakening of the hydrogen bonds of water after ceramic Far-Infrared Ray (cFIR) irradiation and the resulting effects on physical and chemical properties of water. In this study, the Fourier transform infrared spectroscopy (FT-IR) was used to explore hydrogen bonding change of cFIR-irradiated water; in addition, capillary viscometers, Gas Chromatographs (GC), Differential Scanning Calorimetry (DSC), contact angles, Franz cells,  High-Performance Liquid Chromatography (HPLC), and capillary electrophoresis analysis were used to evaluate its physical characteristics, such as viscosity, volatility, temperatures of water crystallization, surface tension, diffusion, hydrogen peroxide dissociation, solubility of solid particles, and changes in pH of acetic acid. The cFIR treated water decreased in viscosity and surface tension (contact angles), but increased in the solubility of solid particles, hydrogen peroxide dissociation, temperatures of water crystallization, and acidity of acetic acid. The weakening of water hydrogen bonds caused by cFIR  irradiation is correspondent with our previous medicalbiological
studies on cFIR.

Contact angle; Ceramic far infrared ray (cFIR); Irradiation water; Fourier transform infrared spectroscopy (FT-IR); Hydrogen bonds; Solubility; Volatility
Water possesses important properties required for life-giving processes. These properties are effectuated by a hydrogen-bonded environment particularly evident in liquid water. Each liquid water molecule is involved in approximately four hydrogen bonds with strengths considerably less than covalent bonds but considerably greater than natural thermal energy. These hydrogen bonds are roughly tetrahedrally arranged, such that when strongly formed local clustering expands, the density decreases. It is different from actual chemical bonds such as ionic and covalent bonds. Hydrogen bonding is at onetenth of the strength of normal covalent bonds within a molecule. Hydrogen bonding in water, combined with its tendency to form open tetrahedral networks at low temperatures, and possess its characteristic properties [1-9].
The cluster formations where all water molecules are linked by three or four strong hydrogen bonds. The characteristics of hydrogen bonding that are responsible for the special properties of water allow it to act in diverse ways under different conditions, such as the clustering of water molecules [10-12]. For example, Stronger hydrogen bonds decrease viscosity because they decrease the liquid's interactions between molecules (Table 1) [1,3-9,13,14].
By decreasing the size of water clusters, the physical properties of water, including permeability and diffusibility, may be improved [1,2,15]. Many other properties and characteristics of hydrogen bonding relating to the weakening effect of hydrogen bonds of water may also exist (Table 1).
Many methods have been used to reduce the size of water clusters, such as magnetic fields, electric fields, heat, and far-infrared ray (FIR) irradiation [13,14]. Previous studies demonstrated that FIR with wavelengths of 4–16 μm appears to non-specifically induce an increase in the temperature of body tissues and elevate the motility of body fluids because of decreases in the size of water clusters in living organisms [1,2,15]. Researchers have deduced, but lack of strong evidence, that FIR could break the intermolecular hydrogen bonds by exciting stretching or bending vibrations in water clusters, and reducing the size of water clusters [10-12]. Ceramic material irradiate far infrar ray under room temperatures (cFIR) was developed and applied in our laboratory, which was proven to have various biological and medical effects [16-25]. However, its fundamental physical-biological mechanism has not been fully explored. Various tests were performed to investigate its effects on the hydrogen bonding of liquid water.
Materials and Methods
cFIR ceramic powder
The FIR-emitting ceramic powder is micro-sized particles composed of numerous elemental ingredients, including calcium (Ca), zirconium (Zr), sulfur (S), silicon (Si), aluminum (Al), magnesium (Mg), iron (Fe), oxygen (O), and carbon (C), which were developed by the biomaterials laboratory of Taipei Medical University, Taiwan [16- 25]. A Scanning Electron Microscopy (SEM) image on the cFIR powder was demonstrated in this study (Figures 1a and 1b), and emitted a high infrared ray with the emissivity at 4 to 16 μm; the ratio of radiation energy irradiated from the sample to an ideal black body as described by the Planck’s Law was determined by a CI SR5000 infrared spectroradiometer (CI, Ltd., Migdal HaEmek, Israel).
Fourier transforms infrared spectroscopy (FT-IR) measurement
The non-cFIR double distilled water (DDW) and cFIR-irradiated DDW treated for 1 h was prepared for the infrared measurement. The liquid specimen was sealed between a pair of CaF2 windows (Beckman FH-01) with a thin Teflon spacer approximately 150 ?m in thickness. Infrared spectrum was recorded at 25°C using a Nicolet Magna 550 spectrometer equipped with a dTGS detector. Each spectrum was recorded at a resolution of 2 cm-1, 32 scans was carried out and merged for each sample. The data were then calculated from absorption spectrum in the FIR region (3400 cm-1).
Fluid viscosity test by an optically trapped Brownian particle
Recently, we have presented an image-based approach for a nonintrusive fluid viscosity measurement in micro domains [26,27]; details of this system has been described previously [27]. We applied optical tweezers to control the position of optically trapped bead in confined region and use fluctuation of the trapped bead as a micro domain sensor to probe the local viscosity. Here, the two-dimensional mean square displacement (2-D MSD) was applied to capture the characteristics of the motion of a Brownian particle trapped by optical tweezers, where MSD is proportional to diffusion coefficient (D) in diffusive Brownian motion regime, namely, MSD=4DΔt [28] and diffusion coefficient is proportional to (T/?), where Δt, T and ? are time lag, temperature and temperature-dependent fluid viscosity, respectively. This approached were further applied to evaluate the possible effect of cFIR on fluid viscosity. In this study, the optical tweezers system was applied to trap polystyrene bead (1.87 μm, Bangs Laboratories, Fishers, IN), where sequential images of the trapped bead were acquired by the EMCCD camera (LucaEM DL6581, Andor) and were used to track the fluctuation of an optically trapped bead in a fluid with or without the effect of cFIR (Figure 2).
Viscosity test by a capillary viscometer
The effects of the cFIR irradiation on the intra-molecular hydrogen bonding of water were indirectly assayed by a capillary viscometer. Figure 3 show the specimen received the cFIR treatment, setup by 20 ml aliquot DD water for 1 min at ambient temperature. The kinematic viscosity (v) was measured by a calibrated Cannon-Ubbelohde capillary viscometer (Schott, 532 03/ 0C, Germany) with a control unit (Lauda, PVS1-X02004, Germany). The viscometers were placed inside the thermostat with a water bath (Lauda, E200, Germany) at 25°C. Data were correlated using the statistical analysis system (Lauda DR. R. WOBSER GMBH & CO.) package. Kinematic viscometry is defined as the quotients of the dynamic viscosity by the density and has the unit mm2/s (or centistokes, cst). Kinematic viscosities ν, expressed in centistokes, were calculated from the measured flow time θ and instrument constant c by using the following equation: ν= cθ. The values for c are provided by the viscometer manufacturer. The viscometer constants were calibrated for effects of temperature.
GC-SPME analysis of the sorghum wine after direct cFIR irradiation: Samples of 58% sorghum wine were mixed with the cFIR ceramic powder (20 g) and irradiated for 20 min in a sealed glass vessel. Control samples were prepared following the same procedures as the experimental group, and placed in an isolated system for 20 min without irradiation. Sample volatility was tested using the Gas Chromatograph (GC) analyses of the solid-phase micro-extraction (SPME) fractions, using a Varian STAR 3400Cx series The mobile phase ratio was acetonitrile- water (0.1% TFA) 80:20, and the flow rate was 1 ml/min. Indomethacin was detected at a wave length of 320 nm [15].
II GC, equipped with a 30 m×0.5 mm I.D. and 0.25μm film thickness DB Waxter fused with a silica capillary column, connected to a Varian Saturn III mass selective detector using split less injectors. The initial oven temperature was set to 50°C (3 min), and then increased to 200°C, and was maintained at a constant temperature for 5 min. The injector temperature was 240°C, and the transfer line was maintained at 220°C, using nitrogen N60 carrier gas, with a column-head pressure of 13 psi (1 psi=6894.76 Pa).
GC-SPME analysis of the sorghum wine after indirect cFIR irradiation: The 20 g power of cFIR ceramic, enclosed in plastic bags, was used to irradiate various water samples (10 ml in a glass dish) for 20 min. Samples of 58% sorghum liquor (2 ml each) were irradiated by the cFIR-irradiated water samples (indirect contact separated by collection tubes) for 1 min in a closed system. The control samples were also prepared using the same procedure as the experimental groups but using usual water samples. GC analyses of the SPME experiments were also conducted using a Varian STAR 3400Cx series II GC. The following procedures and conditions were identical to those described in the previous section.
Diffusion test model by passing drug (Indomethacin) through the artificial membrane
Franz cell apparatus: Cellulose acetate membranes with a molecular weight (MW) cutoff of 10,000 (Spectrum, Laguna Hills, CA) were trimmed into circular discs (diameter approximately 10 mm) sufficient to cover the effective diffusion area of the receptor, and then soaked in a phosphate buffer (pH 7.4) for at least 12 h. Cellulose acetate membranes, which contained glycerin, were rinsed once with the receptor fluid before placing them onto the receptor. Membranes were hydrated and sandwiched between two microscope glass slides and submerged in receptor fluid in a Petri dish to prevent creases or folds when wetted. Air bubbles are trapped within the interface of membrane and receptor. The donor compartment was then covered and closed up tightly by a pinch clamp. During the operation of the Franz cell, we collected 500 μl from the receptor buffer through a sample port by using a pipette [15]. Drug content was assessed by HPLC methods. HPLC analysis was performed using a Waters 2487 HPLC UV-Visible Detector (Milford, MA, USA) with an auto sampler equipped with a quaternary pump and a variable-wavelength detector. All samples were analyzed using a reverse phase C18 column (Microsorb-MV C18 15 cm, 5 μm). The mobile phase ratio was acetonitrile-water (0.1% TFA) 80:20, and the flow rate was 1 ml/min. Indomethacin was detected at a wave length of 320 nm.
Surface tension-measurement of water contact angles: We used a remote-computer-controlled goniometer system (Digidrop, GBX, France) to measure the contact angles. The cFIR-irradiated water and control water’s contact angle to the surface were measured at 25°C and 70% relative humidity. A minimum of three readings were made on each sample, and the values from a minimum of 30 samples were averaged.
Analysis of Hydrogen Peroxide (H2O2) dissociation - direct scavenging of H2O2: An H2O2 solution (Sigma, St. Louis, MD, USA) with 1M concentration was prepared, and equal amounts of 9 ml H2O2 solution was added to the test tubes. H2O2 solution was categorized into two groups: the control and cFIR. For the cFIR group, test tubes were incubated at room temperature and externally covered by plastic bags filled with 100 gm cFIR powder for 3 h of irradiation. The control group was treated similarly, with the exception of the cFIR treatment. After the incubation period, 7.5 mM phenol red (Sigma, St. Louis, MD, USA) and 5 mg/ml horseradish peroxidase (Sigma, St. Louis, MD, USA) were added to each test tube. The mixture was allowed to react for 10 min, and absorbance was observed at 550 nm by an enzyme-linked immune sorbent assay (ELISA) reader (Gemini XPS Molecular Devices, Sunnyvale, CA, USA), with lower absorbance values representing higher H2O2 scavenging ability.
Solubility-measured by capillary electrophoresis analysis: Water samples were prepared from ultra-pure water with 18.2 MΩ resistance (Satorius 337070, Germany). The water samples were preirradiated by FIR ceramic powder at room temperature for 20 h, and the control water samples were covered with aluminum foil and stored in a dark environment at room temperature. After 20 h, the water samples were aliquot into 25 ml in the 50 ml polypropylene centrifuge tubes. Aqueous extracts were prepared by infusing 0.1 grounded and homogenized dry green tea leaves into each of the 25 ml water samples at room temperature for 10 min. This was repeated five times for cFIR irradiation treatment for the statistic analysis. A thermal-controlled (25oC) capillary electrophoresis (CE) system (G1600A, Agilent) was used and controlled by 3D-CE ChemStation software (Agilent) to obtain quantitative measurements of various components in the green tea samples. An untreated fused-silica capillary tube (Beckman; total length 48.5 cm, effective length to detector 40 cm, I.D. 50 μm, O.D. 375 μm) was thoroughly flushed with 1.0N NaOH for 50 min and then deionized water for 30 min before use. Before injection, the initialized capillary was preconditioned by rinsing sequentially with 1.0N NaOH for 2 min, water for 1 min, and a running buffer for 2 min. The sample solution was injected at 30 mbar for 5 s, and then followed with an injection at 30 mbar for 1 s of the running buffer to minimize the sample loss. The electrophoretic separation process was monitored with a built-in photodiode array (PDA) detector at 200, 205, 220, 266, and 280 nm. After electrophoresis, the capillary was cleaned by flushing with deionized water for 2 min.
Because of the better separation efficiency, better separation speed, and less consumption of water samples and reagent, CE has been used to be the complement to ion chromatography [29]. In this study, CE was used to verify the categories and the quantity of each catechin. A mixture of 13 main standards (include GC, caffeine, EGCG, EGC and EC) in tea was analyzed using the micellar electrokinetic capillary electrophoresis (MEKC) method [30].
Analysis of water crystallization temperature (Tc): Water samples treated by cFIR for 5 min were used as experimental group to contrast with control group in Tc analysis (DDW without cFIR treatment). About 5 mg water sample was individually loaded into a volatile aluminum sample pan with cover and hermetically sealed. The specimen was placed in the chamber of the differential scanning calorimetry (DSC) apparatus (Model DSC2920, TA Instruments, Newcastle, Del., USA) and set the following procedures: cooling rate of -5°C/min from 40°C to -40°C, and then keep the temperature for 5 min. The procedure was repeated 5 times in a dry nitrogen environment. The enthalpy of crystallization during cooling ΔHc was measured.
pH value determination of weak acid: Glacial acetic acid (1 ml) was added to double-distilled (dd) H2O (9 ml) in a glass tube, to form a 10% acetic acid solution. After 2 min equilibration time, solution pH was measured and recorded. The glass tube was then covered with cFIR powder and irradiated for 2 min, the solution pH was recorded, and changes in pH were noted.
Statistical analysis
Measurements were performed in multiple tests. Statistical evaluation between cFIR and control groups was determined by the paired t test method, and data with a p value less than .05 were considered significant.
Fourier transforms infrared spectroscopy (FT-IR)
IR spectroscopy is one of the most precise methods to provide information on H-bonds. In this experiment, we found the quantitative difference of cFIR-irradiated DDW and non-cFIR DDW in the FIR region (3400 cm-1), with a significant decrease in the absorbance of cFIR-irradiated DDW. This result indicates a hydrogen bond weakening effect of DDW after cFIR irradiation (Figure 4).
Because of the unusually strong absorption of liquid water in this mid-IR region, this spectrum of liquid water mainly consists of three types of vibrations of H2O molecules: the most intense νs (O-H ???) stretch band with a maximum at approximately 3400 cm-1, the δH-O-H bending band (vibration of the H-O-H angle) with the maximum at approximately 1640 cm-1, and the “librational” band ρH2O at approximately 700 cm-1 (relative rotations of rigid H2O molecules, also called hindered rotations). The intra monomer bands ns and δH-O-H correspond to those of water vapor.
Fluid viscosity (by Brownian particle) or Effect of cFIR irradiation on fluid viscosity
We then investigate the relationships between MSD and time lag Δ t to evaluate the possible effect of cFIR on fluid viscosity at room temperature. Figure 5 showed the MSD plots of an optically trapped polystyrene bead in a fluid with (cFIR irradiation for three minutes, solid symbol) or without the effect of Cfir (empty symbol). We find that MSD and time lag Δ t is linear within Δ t = 40 ms; however, significant deviations from linearity have been found at time intervals above 80 ms due to the optical confinement. This relation revealed that the motion of optically trapped bead showed a random walk during short time interval. In addition, as we mentioned earlier that diffusion coefficient (D Δ T / Δ) could be obtained from the linear slope of 2-D MSD plot, namely, MSD=4DΔt, the present results showed that in short-time interval regime values of the linear slope of MSD plots in the experimental group (cFIR irradiation for three minutes) were larger than that in the control group (without cFIR irradiation), which implied cFIR irradiation decreased a fluid's viscosity, as can be seen in Figure 4. Note that the present result showed that change ratio of fluid's viscosity, (?w/o-?w/)/?w/o, ? 0.12, which implied fluid's viscosity is decreased to 12%, where ?w/o and ?w/ represent are fluid viscosity in the absence and presence of the effect of cFIR, respectively.
The flow time and kinematic viscosity of water samples determined by the capillary viscometer for the control water and the cFIRirradiated water were 300.37 ± 0.91 s and 293.39 ± 0.05 s, and 0.92 ± 0.00 cSt (centistokes) and 0.90 ± 0.01 cSt, respectively. The flow time and viscosity reduction for water treated by cFIR irradiation was statistically significant from that of the control group, implying the weakening of intermolecular hydrogen bonding, respectively (p<.01; Table 4).
Volatility result of GC-SPME analysis of sorghum wine irradiated either directly or indirectly by cFIR ceramic materials
We determined changes in volatility of the cFIR-irradiated alcoholwater mixture. Figure 6a shows elevation in ethanol volatility for the cFIR directly irradiated samples compared to the control group; Figure 6b shows elevation in ethanol volatility for the indirect cFIR-irradiated samples compared to the control group, as measured by GC-SPME. The change in mean volatility of the cFIR groups, expressed as the total amount of ethanol extracted, was significantly higher than that of the control group (p<.01).
Result of diffusion model using drug (Indomethacin) pass through artificial membrane
Figure 7 shows the transdermal diffusion of Indomethncin without and with cFIR irradiation in Franz cell experimental model. Under cFIR irradiation, the indomethacin solution was found significantly facilitated passed through the artificial skin membrane monitored by the Franz cell experimental model (p<.01).
Surface tension
The water contact angles of cFIR-irradiated water and control water are shown in Figure 8. The average results of cFIR-irradiated water had a lower contact angle than that of the control water. The change of surface tension may be the main reason for the different contact angle (p<.05).
Hydrogen peroxide dissociation
Figure 9 shows that the mean absorbance of the control and cFIR groups found a significant decrease in the cFIR group (n=31). The extent of H2O2 disappearance in the cFIR group is larger than that in the control group with a 10.26% decrease. This result confirms that H2O2 can be scavenged directly by cFIR treatment.
Results of cFIR irradiation on the green tea solution, measured by capillary electrophoresis (CE): In this study, CE was used to verify the categories and the quantity of each catechin. A mixture of 13 main standards (GC, caffeine, EGCG, EGC and EC) in tea was successfully analyzed by micellar electrokinetic capillary electrophoresis (MEKC). By comparing with the standard mixtures in the electropherogram, the constituents of green tea were identified. Figure 10 shows the separation profile of green tea prepared from two different water sources. The results show that these five peaks of green tea prepared by cFIR-treated water are higher than the control. Figure 10 also shows the comparisons of peak area analysis in these five major components (GC, caffeine, EGCG, EGC, and EC). Each component of green tea treated by cFIR is greater than the control. The average increase is 9.05% for the five representing constituents.
Temperature of crystallization (Tc) determination
The result of a DSC experiment is about heat flux versus temperature or versus time. There are two different conventions: exothermic reactions in the sample are shown with a positive or negative peak. T?he curves can be used to calculate enthalpies of transition of water. In our study, we used DSC to precisely measure the different phases of transition energy released or absorbed of the different water samples to prove our previous deduction that cFIR is capable of changing the physical properties of water.
During this study, generally, the temperature program for DSC analysis is designed such that the sample holder temperature increases linearly as a function of time. The reference sample should have a welldefined heat capacity over the range of temperatures to be scanned. Our result of DSC analysis on the water sample without cFIR treatment showed an obvious change of heat flow (ΔHc; Table 3) during the transit from the liquid phase (water) to the solid phase (ice).
Changes in pH on weak acid solution following cFIR irradiation
Samples of 10% acetic acid solution without and with cFIR irradiation were measured for pH values. The results showed 1.8612 ± 0.55 (without cFIR) and 1.8458 ± 0.54 (with cFIR) respectively (n=24). The observed decrease in pH for the irradiated group is significantly higher than that for the control group (Figure 10a; p<.05).
According to our observation, cFIR exhibits its biological and medical effects not necessary for liquid water [31]. However, since living tissues of plants or animals are composed of water, we deduce those benefits of cFIR should be directly or indirectly through water’s effect.
IR spectroscopy is by far the most precise method to provide information on hydrogen bonding which has a significant influence on the peak shape and intensity, generally causing peak broadening and peak shifting to lower frequencies (red-shift). Unlike the water molecule having a very small moment of inertia on rotation in vapor phase which gives rise to rich combined vibrational-rotational spectra, the FI-IR rotational spectra for liquid water molecules tend to be restricted by hydrogen bonds. IR spectroscopy was generally considered to be able to provide only qualitative and semi-quantitative analyses of common samples. However, the development of reliable FTIR instrumentation and strong computerized data-processing capabilities have greatly improved; thus, modern infrared spectroscopy has been accepted as a reliable tool for quantitative analysis [32].
Since the FT-IR measurement for non-cFIR DDW and cFIR irradiated DDW were carried out in a liquid cell with the same 150 μm -Teflon spacer, the intensities of absorption bands were linearly proportional to the molecular absorptivity which might be attributed to the influence of the cFIR irradiation. Our result indicates cFIR exhibiting hydrogen bond weakening effect. We also performed a series of experiments to demonstrate other physical and chemical characteristics of the hydrogen bond weakening effect and possible applications, listed as below:
Viscosity Changes in hydrogen bonding have particularly important effects on viscosity and diffusion, which are shown by the large changes occurring in normal water. Viscosity is particularly affected by the strengthening of water’s hydrogen bonds, increasing 10-fold. For example, with a value of 37°C, the increase in hydrogen bond strength is only 8%. While the Stokes–Einstein equation predicts that the diffusion coefficient of a solute will be inversely proportional to the viscosity of the solvent [33]. According to the results, viscosity decreased by the cFIR irradiation on DD water. In previous studies, the absorption of sound was proven to have a specific range of frequency and intensity in distilled water under various conditions of sample illumination, and treatment with a magnetic field and ultrasound. The difference in sound signal absorption in water under unequal conditions is explained by variations in viscosity because of changes in the structural state of water, in particular, the destruction or formation of clusters. A similar phenomenon is noted in cFIR under room temperature, without the necessity of electricity-supported instruments, such as ultrasounds and strong magnetic fields. In this viscosity study, a weakening effect of the cFIR on hydrogen bonds to achieve decreases in viscosity was shown [1].
Water cluster frequencies/Size
Other researchers have claimed that FIR rays can break hydrogen bonds (H-O bonds) by exciting, “stretching or bending,” vibrations in the water clusters; they can also reduce the size of the water clusters [7,8,16,18,19].
Hydrogen bonds are the weakest type of chemical bond and are easily broken by thermal energy. Previous researches considered hydrogen bonds broken if the bond length increases or the bond angle decreases [7,8,16,18,19]. The hydrogen bonding holds water molecules approximately 15% closer than if water were composed of simple liquid molecules interacting with each other through van der Waals forces. However, hydrogen bonds restrict the number of neighboring water molecules to approximately four, instead of the larger numbers found in simple liquids [1,34-36].
The hydrogen bond is one factor that determines volatility. Any liquid that possesses hydrogen bonds may evaporate more quickly if the hydrogen bonds are broken. The effects of the weakening or destruction of hydrogen bonds is a major event in the enhancement of liquid volatility and energy transfer in liquid water. Volatility is an important physical property, and changes in volatility of an alcoholwater mixture may reflect a transformation of physical properties that are independent of chemical changes [37]. In this study, we used the dynamic headspace solid-phase micro extraction (HS-SPME) and GC to determine quantitatively the changes in the volatility of cFIRirradiated sorghum wine and water. We conclude that the effects of cFIR irradiation on water molecules enhanced the volatility of the liquor solution by weakening the hydrogen bonds.
Diffusion of liquid varies inversely with viscosity; we found that molecular movements slow as viscosity increases. Several factors determine the rate of diffusion of a molecule across the membrane depending on the size, polarity, and charge of each particular molecule. For an uncharged polar molecule to leave the aqueous phase and enter the lipid phase, it must first break its hydrogen bonds with water before it can dissolve in the lipid phase. The number of hydrogen bonds a molecule forming to water is determined by the number of polar groups in the molecule, and the strength of the hydrogen bonds formed. Each additional hydrogen bond formed between a polar group and water results in a 40-fold decrease in the partition coefficient, and a resulting decrease in the molecular permeability through the cell membrane [38].
Surface tension (contact angle)
The surface tension and viscosity of water are related to the strength of the hydrogen bonds between water molecules. The unusually large heat capacity of water is also related to the strength of the hydrogen bonds (H-O bonds) between water molecules that determine the characteristics of high volatility and viscosity. The decrease of volatility in the alcohol-water mixture of our cFIR treated samples is a reflection of decreased surface tension. Water droplets are strongly attracted to solid surfaces if the droplet spreads out completely on the solid surface and the contact angle is decreased. The weaker hydrophilic form has a higher contact angle of up to 90°C.
Conversely, if a liquid is highly hydrophobic (less hydrophilic), the contact angle is larger. Because the water contact angle is proportionate to the water surface tension, a smaller water contact angle may be reflected by decreased surface tension [39]. Surface tension is caused by hydrogen bonds in the water sample holding tightly to one another and creating a type of structural rigidity [39,40]. Our results showed a significant reduction in the water contact angle of cFIR -treated water that was lower than the pretreated water (control group). Therefore, we deduce that cFIR material may induce water and related water mixtures to become lower in hydrophobicity and in lower surface tension, and perhaps weaken the hydrogen bonds. Particularly, this is the first study to show that the cFIR treated water can change the water contact angle.
Hydrogen peroxide dissociation
Previous studies have demonstrated that the thermal FIR treatment has the capability of cleaving covalent bonds to liberate more antioxidant compounds, for example, carotene and polyphenols from rice hulls and medicinal plants. Therefore, the increased heat transfer efficiency of FIR-emitting ceramic material explains the direct and indirect effects on H2O2-scavenging capacity. In addition, the FIR can break hydrogen bonds (H–O bonds) by exciting the stretching vibrations in the water clusters, and decreases the size of the water clusters [37].
Hydrogen bonds can reduce the volatility of any liquid possessing hydrogen bonds, and are related to the reduction rate of H2O2, which exist in cluster forms in normal conditions, and not as a single molecule. Therefore, the weakening of hydrogen bonds by FIR may also explain why the FIR accelerated the H2O2 transformation, and released H2O and O2 from H2O2 molecular clusters.
Solubility of solid particles
We showed that the FIR treatment at room temperature had significant effects on the water used to prepare the green tea. The total phenol contents, each major constitute concentration, and antioxidant activities of green tea were all enhanced by the FIR treatment. The three experiments in this study corresponded with each other, and indicate that more available or soluble catechins contribute to promoting the antioxidant activity of the green tea. No obvious difference was found in catechin degradation between the standard solutions dissolved by the FIR-treated water and control water. This indicates that the FIR effect on increasing catechin contents by enhancing the extraction efficiency on the green tea leaves instead of preventing the degradation of catechins is major. This shows that the cFIR causes the destruction of water clusters, and then facilitates water in extracting more functional constitutes of green tea leaves, and hence, enhances the antioxidant activities of the green tea. The rate-determining steps in tea leaf infusion were determined by the diffusion of the solutes through the leaf matrix to the surface. Destroyed water clusters increase the total number of water clusters, provide larger specific surfaces, and raise more contact opportunities for water molecules and green tea leaves, to extract more solutes in the green tea infusion.
Water crystallization
The results of our DSC experiment suggest that the increase in the freezing temperature observed for the cFIR-irradiated water may be caused by energy transfer in the water cluster through the influence of hydrogen bonds, creating an environment less conducive to the solid state [38,39]. The weakening effect of cFIR on the hydrogen bond likely accelerates water molecules and allows them to form hexagonal ice crystals [1].
pH change on weak acid
Acetic acid (CH3-COOH) possesses the hydrogen (H) atom in the carboxyl group (−COOH), which gives off an H+ ion that produces its acidic character. Acetic acid is a weak acid, and hydrogen bonding effectively affects its acidity (Figures 11a and 11b). We deduced that the weakening of the intra-molecular hydrogen bond of the carboxyl group in acetic acid affected by the cFIR irradiation resulted in an increase in acidity [40].
Future application and researches
Water is the major constituent of living systems, such as the intracellular, extra cellular, and the circulation system. The influence of the cFIR on liquid water is probably a key explanation to the mysterious function of this specific spectrum of wavelengths toward living organisms. In the future, the cooperation of medical-biological and physical-chemical researchers is necessary for an in-depth study on this interesting topic.
We speculated that this phenomenon may be a consequence of a hydrogen bond-weakening effect and the unique 3D dynamic structural fluctuations and rearrangements of the hydrogen bonding network of water, which undergoes ultrafast structural reorientation and reorganization.
Because cFIR materials work on the "weakening of hydrogen bonds", the impact of this phenomenon contributes to different industrial applications relevant to its characteristics (Table 2).
We demonstrated the influence of room temperature cFIR irradiation weakening hydrogen bonds by using quantitative measurements of viscosity, water cluster size/frequency, volatility, diffusion, surface tension (contact angle), hydrogen peroxide dissociation, solubility of solid particles, temperatures of water crystallization, changes in the pH of acetic acid, and the Fourier transform infrared spectroscopy (FT-IR) to produce physical and chemical changes in aqueous samples. Our methods tried various ways to demonstrate the weakening changes of hydrogen bonds by the cFIR irradiation. These physical effects may be one of the initial physical-biological mechanisms we observed in our previous medical-biological studies [13-22]. In the future, we wish to study further on potential applications of this effect.
The authors gratefully acknowledge the support provided to this study by Ms. Francis Chou (Hou Kunt Biological Technology CO.LTD), Mr. Ping Tai Lin (Leader Culture Co.), Mr. Francis Chen (Franz Collection, Taipei, Taiwan), and Mr. Li Chien Chiu (Hocheng---HCG, Taipei, Taiwan).

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Figure 10   Figure 11a   Figure 11b
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