The Effect of Trifluoroethanol and Glycerol on the Thermal Properties of Collagen Using Optical Displacement-Enhanced Heterodyne Polarimeter

Abstract

An angular displacement-enhanced heterodyne polarimeter has been employed to investigate the interplay between trifluoroethanol (TFE) and glycerol on the thermal denaturation of type I collagen. The concentration of the collagen solution was fixed at 0.341 (mg/mL), and was heated from 25 °C to 55 °C. TFE solutions with concentrations of 5%, 10%, 15%, 20%, 40% and 80% (v/v) were prepared and the phase change was recorded for the determination of thermal denaturation. It was observed that the thermal denaturation temperature (T_d) is decreased with increasing TFE concentration due to the partial cleavage of the triple-helical structure. With TFE concentration higher than 20% (v/v), the degree of optical rotation appears to be nearly the same, reflecting that the collagen triple helices have been completely destructed. Moreover, the addition of glycerol in inhibiting the thermal denaturation of collagen is investigated. It has been shown that glycerol can improve the thermal denaturation of both collagen and TFE-mixed collagen. Experimental results show that, in the presence of 2 M glycerol, the T_d of collagen remained at around 41.9 °C, meanwhile the T_d of 20% (v/v) TFE-mixed collagen is significantly restored to 32.8 °C.

1. Introduction

Collagen is the major component of the human proteome and plays a key role in the structural connection of tissues, such as ligaments, tendons, ocular sclera, bone, and skin. Collagen has a unique structure in which the hierarchical structure is composed of the triple helices consisting of twisted polypeptide chains. The collagen-derived biomaterials have been widely developed in the applications of medical cosmetology and tissue repairing, and regeneration engineering. In the preparation of these biomaterials, trifluoroethanol (TFE) is used as a co-solvent. For instance, collagen-glycosaminoglycan scaffold [1,2] and collagen nano-fibers [3] used for tissue reconstruction can be prepared from aqueous TFE mixture. Shanmugam et al. [4] have summarized the effect of TFE induced in proteins, which can stimulate the conformational transition between random coil, α-helix, and β-sheet in proteins and peptides. Shanmugam et al. [4] also investigated the effect of TFE on type I collagen structure using circular dichroism (CD) and Fourier transfer infrared (FTIR) spectroscopy techniques. The results of thermal melting revealed that the stability of triple helix in collagen was decreased even at a low concentration of TFE (5%, v/v) by the observation of decreased optical density [4]. Furthermore, the results of the turbidity measurements revealed that the collagen structure is dissociated by inhibiting the fibril formation under the circumstance of higher TFE concentration [4].

Glycerol is a hyperosmotic agent used to adjust the optical scattering properties of turbid tissues. Yeh et al. [5] have reported that the use of glycerol screens intermolecular interactions between low-order structure in collagen and leads to fiber disassembly. D. Cooper et al. [6] used glycerol as a stabilizer to increase the denaturation temperature up to 0.96 °C. Penkova et al. [7] have investigated the stabilizing effect of glycerol on the thermal denaturation of several type I collagens in urea ranging from 20 to 50 °C using a UV-spectroscopy. It was found that the denaturation temperature (T_d) increased proportionally to the glycerol concentration, indicating that the collagen was stabilized in the presence of glycerol. It was further investigated that the combined effect of glycerol and urea with concentration ranged from 1 to 3 M; the results clearly showed that the thermal denaturation induced by urea was improved by the addition of glycerol. Thermal stability of collagen cross-linked with different organic solutions has been studied by C.A. Miles et al., using differential scanning calorimetry (DSC) [8]. It was reported that the improvement in the thermal stability related to the level of fiber dehydration is brought about by the cross-link drawing of collagen molecules. The degree of hydration in collagen could lead to the thermal transition between helix and coil structures [9]. G. Na [10] has studied the interaction of calfskin collagen with glycerol and suggested that the surface interaction of native collagen with glycerol is more favorable than that with water from the three-component solution thermodynamics. Glycerol can be considered as a “thermodynamic inhibitor” against the self-association of fiber collagen since glycerol weakens the fibril assembly reaction through a weak mutual attraction with the protein [10]. G. Na [10] further proposed that the driving force responsible for the stabilization of the triple-helical structure mainly depends on the interaction of native collagen with glycerol, while it was claimed that the denatured collagen unfavorably interacted with glycerol according to the unchanged chemical potential. M. Schoulders et al. [11] also investigated the stability of triple helices and polypeptide chains in collagen, and pointed out that the stabilization is preferentially dependent on the hydrogen bonding, which existed between N-H Gly and neighboring O=C strands [3,10].

Recently, an enhanced angular displacement system has been developed using a heterodyne light source and a common-path optical setup for small optical rotation angle detection of glucose [12] and other optically active medium [13]. This is a noninvasive and real-time approach, in which the heterodyne light source consists of two component beams with different frequencies, and the polarization of each component beam is orthogonal to the other. For instance, a beam parallel to the plane of incidence is the TM mode, and the other is the TE mode. Additionally, the heterodyne light source has the electric field represented by the Jones matrices, and is separated into two paths, the measurement path and the reference path, by a beam splitter [13]. However, these true phase measurements are not sensitive enough to detect a small optical rotation angle [14,15,16]. In this regard, Wu et al., further modified the measurement with a high optical resolution of 1 × 10⁻⁴⁰ to monitor the blood glucose using an angular displacement-enhanced heterodyne polarimeter [13].

In this paper, we made an attempt to employ an angular displacement-enhanced heterodyne polarimeter to precisely monitor the effect of TFE on the thermal denaturation properties of collagen in rat tails. The TFE aqueous solution with wide range of concentration from 5% to 80% (v/v) was used to investigate the interaction of TFE and triple helical structures. Moreover, the inhibiting effect of glycerol on the thermal degradation of TFE-mixed collagen is investigated. The inhibiting mechanism of glycerol with three hydroxyl groups for the stabilization of the triple helix is discussed.

2. Experimental Section

2.1. Experimental Setup

For the optical measurement, a He-Ne laser with a wavelength of 632.8 nm was employed as the light source. When the light was passing through the first half wave-plate (HWP1) (NTHU, Hsinchu, Taiwan), the polarization state was adjusted parallel to the incident plane, then divided by a beam splitter (BS1) and fed into a pair of acousto-opto-modulators (AOM1 and AOM2) (NTHU, Hsinchu, Taiwan). A beam combiner (PBS) (NTHU, Hsinchu, Taiwan) was used to combine the output beams from each AOM, and then the heterodyne light source could be obtained. The heterodyne light source consisted of two component beams with frequencies ω₁ and ω₂, and the polarization of each beam was orthogonal to the other. The one perpendicular to the incidence plane is called the TE mode, while the other is in TM mode. The prototype of an angular displacement-enhanced heterodyne polarimeter has been built and the theoretical analysis has been discussed in [13], in which two angles represent the optical rotation and the phase difference. The relationship between the phase difference φ and the intensity of the beam of the laser onto the HWP1 can be expressed as following [13]:

$$I_m=k_{a1}^2+k_{a2}^2+2k_{a1}{k}_{a2}\text{cos}[({\text{ω}}_1-{\text{ω}}_2)t+\text{φ}],$$

(1)

where

$$k_{a1}={\left(1-{\text{cos}}^2\frac{\text{δ}}{2}\text{sin}2\text{β}+{\text{sin}}^2\frac{\text{δ}}{2}\text{sin}(4\text{θ}+2\text{β}\right)}^{\frac{1}{2}}$$

(2)

$$k_{a2}={\left(1+{\text{cos}}^2\frac{\text{δ}}{2}\text{sin}2\text{β}-{\sin }^2\frac{\text{δ}}{2}\text{sin}(4\text{θ}+2\text{β}\right)}^{\frac{1}{2}}$$

(3)

and phase difference φ can be further obtained from

$$\text{φ}={\text{tan}}^{-1}\left[\frac{\text{sinδcos}2\text{θ}}{{\text{cos}}^2\frac{\text{δ}}{2}\text{cos}2\text{β}-{\text{sin}}^2\frac{\text{δ}}{2}\text{cos}(4\text{θ}+2\text{β})}\right]$$

(4)

The double-distilled water (ddH₂O) was injected into the sample tube and used as control. Due to the nature of optical inactivity, the change of the angular displacement is zero (i.e., β = 0). The phase difference φ can be simplified as the following [13]:

$${\text{φ}}_{\text{β}=0}={\text{tan}}^{-1}\left[\frac{\text{sinδcos}2\text{θ}}{{\text{cos}}^2\frac{\text{δ}}{2}-{\text{sin}}^2\frac{\text{δ}}{2}\text{cos}(4\text{θ})}\right]$$

(5)

For all optical measurement, the phase retardation δ of 178.5° and azimuth θ = 23.2° was set to maintain the larger amplification with great signal-to-noise (SNR). Equation (4) was employed to calculate φ, between the reference signal and measurement signal, and with adjustment, β varied from 0° to 0.01° by increasing 0.001° for each measurement. The amplification factor defined by the ratio of φ over β is about 42.1. The thermoelectric cooler (TEC) (NTHU, Hsinchu, Taiwan) was used to heat the sample tube to a temperature from 25 °C to 55 °C. The temperature deviation during the measurements was less than ±0.3 °C. A Soleil-Babinet compensator (SBC) (NTHU, Hsinchu, Taiwan) was employed to enhance the optical displacement. This SBC was controlled to rotate 0.05° azimuth degrees per second (i.e., rotate 180° within 60 min), and the sampling frequency is 0.5 Hz. Finally, the phase difference φ as a function of phase retardation δ, azimuth θ of the δ-WP, and angular displacement β can be simply read by the lock-in amplifier (LIA). Figure 1 shows a schematic drawing of the applied setup.

Figure 1. (a) Schematic diagram of the optical displacement-enhanced heterodyne polarimeter and sampling system; (b,c) show photos of real experimental apparatus and setup. M: mirror, BS: beamsplitter, PBS: polarizing cube beamsplitter, PhD: photodetector, SBC: Soleil-Babinet compensator, HWP: half-wave plate, AOM: acousto-optic modulator, Pol: polarizer, TEC: thermoelectric cooler, LIA: lock-in-amplifier, PC: personal computer.

Figure 1. (a) Schematic diagram of the optical displacement-enhanced heterodyne polarimeter and sampling system; (b,c) show photos of real experimental apparatus and setup. M: mirror, BS: beamsplitter, PBS: polarizing cube beamsplitter, PhD: photodetector, SBC: Soleil-Babinet compensator, HWP: half-wave plate, AOM: acousto-optic modulator, Pol: polarizer, TEC: thermoelectric cooler, LIA: lock-in-amplifier, PC: personal computer.

2.2. Sample Preparation and Measurement of Thermal Denaturation

The collagen samples purchased from BD Bioscience Co. (Franklin Lakes, NJ, USA) with the product number 354236 are type I collagen extracted from rat tails. The initial concentration was 3.41 mg/mL, which was then diluted to 0.341 mg/mL using 0.02 M acetic acid (pH value = 3.3) as a solvent. Trifluoroethanol (TFE) with 99.9% purity was purchased from Alfa Aesar Co. (Lancashire, United Kingdom) (product number: 10175784); glycerol (99.9% in purity) is a product of J. T. Baker Co. (Center Valley, PA, USA) with product number of 2136-01. All reagents were of analytical grade.

For the measurement of the thermal denaturation, the collagen solution with a concentration of 0.341 mg/mL was mixed with 0.157, 0.333, 0.529, 0.75, 2, and 12 mL TFE to obtain 5%, 10%, 15%, 20%, 40%, and 80% (v/v) TFE-mixed collagen solution, respectively. The samples were maintained at 25 °C for 5 min and then heated up to 55 °C with a heating rate of 1 °C/min using a TEC. 1 M and 2 M glycerol were used to mix with 10% and 20% (v/v) TFE-mixed collagen to investigate the inhibiting effect of the amount of glycerol molecules on the collagen degraded by low and high TFE concentration, respectively. The phase change φ was recorded with increasing time and under elevated temperatures as well. The denaturation temperature (T_d) was then determined from a transition point, where a significant temperature drop should be observed from the phase change vs. temperature plot.

3. Results and Discussion

3.1. Effect of TFE on the Thermal Denaturation of Collagen

Figure 2 shows the phase difference φ as a function of temperature. The T_d of the native collagen (as a control) is 40.2 °C from the onset of the significant drop in the phase difference. Figure 3 shows the effect of TFE concentration on the phase difference during the heating process. It can be seen that the onset of the significant drop in the phase difference is shifted to a lower temperature, indicating that the T_d of the TFE-mixed collagen is decreased from 37.3 °C to 28.4 °C. In this stage, the addition of TFE increases the heterogeneity of collagen in the aqueous buffer solutions due to the formation of unordered peptide carbonyl groups (−C=O) [4,17]. As the TFE concentration is higher than 40% (v/v), the significant drop in the phase difference diminishes and reveals that the collagen has been completely destructed. It has been suggested that the variation in the optical properties can be used to explore the thermal degradation of TFE-mixed collagen and the resulting structural destabilization [4]. Thus, we recorded the initial optical rotation as a function of TFE concentration from the displacement-enhanced heterodyne measurement, as shown in Figure 4a. It can be seen that initial optical rotation is reduced by 0.1° as TFE concentration increased to 15% (v/v), while this value is significantly reduced to less than 0.4°. It has been suggested that TFE introduces the α-helical structure in the aqueous TFE solution, and then causes the disruption of the inter-strand hydrogen boding (i.e., the bifurcated hydrogen bonding for C=O chains between the N-H and O-H group of TFE). As the TFE concentration further increases (40%~80%, v/v), the initial optical rotation of the TFE-mixed collagen remains almost unchanged, indicating that the inter-strand hydrogen bonding between the N-H Gly and neighboring C=O Xaa groups has been destructed and the fabrils in the collagen have been completely inhibited [4,18,19,20]. In this way, the triple helices have become destabilized by transforming the helical structure into an unordered structure, as proposed by Shanmugam [4] and Rajan [18]. The dependence of the denaturation temperature on the TFE concentration is illustrated in Figure 4b, revealing that T_d of the TFE-mixed collagen decreased proportionally to the TFE concentration in the solution.

Figure 2. The phase difference of collagen as a function of temperature. (Collagen concentration: 0.341 mg/mL).

Figure 2. The phase difference of collagen as a function of temperature. (Collagen concentration: 0.341 mg/mL).

Figure 3. Variation of phase difference with heating temperature under different Trifluoroethanol (TFE) concentration (v/v): (a) 5% (=0.157 mL); (b) 10% (=0.333 mL); (c) 15% (=0.529 mL); (d) 20% (=0.75 mL); (e) 40% (=2 mL) and (f) 80% (=12 mL). (Collagen concentration: 0.341 mg/mL) The inset T_d represents the denaturing temperature.

Figure 3. Variation of phase difference with heating temperature under different Trifluoroethanol (TFE) concentration (v/v): (a) 5% (=0.157 mL); (b) 10% (=0.333 mL); (c) 15% (=0.529 mL); (d) 20% (=0.75 mL); (e) 40% (=2 mL) and (f) 80% (=12 mL). (Collagen concentration: 0.341 mg/mL) The inset T_d represents the denaturing temperature.

Figure 4. (a) Initial optical rotation and (b) denaturation temperature (T_d) as a function of TFE concentration (%, v/v). (Collagen concentration: 0.341 mg/mL).

Figure 4. (a) Initial optical rotation and (b) denaturation temperature (T_d) as a function of TFE concentration (%, v/v). (Collagen concentration: 0.341 mg/mL).

3.2. Effect of Glycerol on the Thermal Denaturation of Collagen and TFE-Mixed Collagen

We first investigate the effect of glycerol on the thermal denaturation of collagen. As seen in Figure 5, the T_d is increased by increasing glycerol concentration. As for the 3 M glycerol, the T_d is increased to 42.4 °C and the stabilization of collagen is improved. Figure 6 shows the inhibiting effect of glycerol on the collagen degraded by 10% (v/v) TFE. It can be seen that the initial optical rotation is restored and the T_d value is increased to 36.4 °C as compared to the value of TFE-mixed collagen (T_d = 33.9 °C). This result provides evidence that glycerol has effective inhibiting abilities on the thermal denaturation of collagen degraded by TFE, even under low glycerol concentration. We further examine the inhibiting effect of glycerol on the high-concentration TFE (20%, v/v) mixed collagen, wherein the helical structures have been almost destructed. As shown in Figure 7, 1 M and 2 M glycerol can increase the T_d to 31.3 °C and 32.8 °C, respectively. Figure 8 shows the degradation of T_d in the presence of TFE and the inhibiting effect of glycerol under different concentrations. The result indicates that glycerol increases T_d by 2.2 °C in the absence of TFE, and further increases the T_d of TFE-mixed collagen at high concentration by 4.2 °C. This improvement is in agreement with the fact that glycerol plays a role of stabilizer in the calfskin collagen solution and increases its T_d by 0.96 °C [6]. It has been suggested that the inhibiting effect of glycerol on the thermal denaturation is achieved by the incorporation of its hydroxyl groups into the water-collagen molecular structure [7]. In other words, glycerol binds to the surface of collagen molecules through the formation of hydrogen bonding, which competes with the water molecules as a replacement for water-mediated hydrogen bonds. Subsequently, the extensive cross-linking structure inhibits collagen dissociation by glycerol [5]. Na obtained a negative chemical potential change of collagen binding with glycerol molecules using the Wyman linked function, and reported that the triple helical structure can be preserved due to the fact that glycerol interaction with the surface of native collagen is more energetically favorable than the interaction between water and collagen [10]. With increasing glycerol concentration, a large amount of hydroxyl groups containing additional and stabilizing hydrogen bonds is generated and leads to greater ability in the inhabitation of thermal denaturation. Similar results can be observed for the stabilizing effect of glycerol on the calfskin collagen degraded by urea [7], where about 1 °C increase of the denaturation temperature per 1 M glycerol was reported.

Figure 5. Effect of glycerol on phase difference of collagen as a function of temperature under (a) 1 M; (b) 2 M; (c) 3 M glycerol concentration (Collagen concentration: 0.341 mg/mL).

Figure 5. Effect of glycerol on phase difference of collagen as a function of temperature under (a) 1 M; (b) 2 M; (c) 3 M glycerol concentration (Collagen concentration: 0.341 mg/mL).

Figure 6. Effect of glycerol on phase difference of TFE (10%, v/v)-mixed collagen as a function of temperature under different glycerol concentration: (a) 1 M; (b) 2 M (Collagen concentration: 0.341 mg/mL). The inset T_d represents the denaturing temperature.

Figure 6. Effect of glycerol on phase difference of TFE (10%, v/v)-mixed collagen as a function of temperature under different glycerol concentration: (a) 1 M; (b) 2 M (Collagen concentration: 0.341 mg/mL). The inset T_d represents the denaturing temperature.

Figure 7. Effect of glycerol on phase difference of TFE (20%, v/v)-mixed collagen as a function of temperature under (a) 1 M; (b) 2 M. glycerol concentration (Collagen concentration: 0.341 mg/mL). The inset T_d represents the denaturing temperature.

Figure 7. Effect of glycerol on phase difference of TFE (20%, v/v)-mixed collagen as a function of temperature under (a) 1 M; (b) 2 M. glycerol concentration (Collagen concentration: 0.341 mg/mL). The inset T_d represents the denaturing temperature.

Figure 8. Stabilizing effect of glycerol in the presence of TFE on rat tail collagen. (a) 0 M glycerol; (b) 1 M glycerol; (c) 2 M glycerol.

Figure 8. Stabilizing effect of glycerol in the presence of TFE on rat tail collagen. (a) 0 M glycerol; (b) 1 M glycerol; (c) 2 M glycerol.

4. Conclusions

The effect of TFE on the optical properties and thermal denaturation of rat tail collagen have been investigated using an angular displacement-enhanced heterodyne polarimeter. The present results indicate that TFE affects the optical rotation and decreases the denaturation temperature due to the disruption of the inter-strand hydrogen bonding. As a result, the triple helices are transformed to an unordered structure in collagen, as evidenced by the decrease in the optical rotation. It is clearly observed that the stability of triple helices is significantly reduced at a TFE concentration higher than 15% (v/v). Furthermore, we demonstrated the inhibiting effect of glycerol on the thermal denaturation of the TFE-mixed collagen. It has been shown that the T_d is significantly increased with increasing glycerol concentration, indicating the TFE-mixed collagen has been stabilized through the extensive covalent cross-links in the presence of glycerol. The relationship between TFE and glycerol concentration on the optical properties is presented; the T_d can be restored to 32.8 °C by glycerol at 2 M and even under high TFE concentration (20%, v/v).