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Article

Analysis of Ultraviolet Radiation Wavelengths Causing Hardening and Reduced Elasticity of Collagen Gels In Vitro

1
School of Bioscience and Biotechnology, Tokyo University of Technology, Tokyo 192-0982, Japan
2
Bionics Program, Tokyo University of Technology Graduate School, Tokyo 192-0982, Japan
Cosmetics 2018, 5(1), 14; https://doi.org/10.3390/cosmetics5010014
Submission received: 9 December 2017 / Revised: 14 January 2018 / Accepted: 17 January 2018 / Published: 22 January 2018

Abstract

:
Regular exposure of facial skin to sunlight promotes wrinkle formation; ultraviolet (UV) radiation causes the skin to harden and lose its elasticity. To study UV damage to the skin in vitro, a short-term in vitro photoaging model is required. Hence, the UV transmittance of excised human skin was measured. Changes in elasticity in the cheeks of humans of different ages were investigated. Moreover, changes in the hardness and elasticity of collagen gels following UV exposure were investigated. UV rays penetrated the upper layer of the dermis and UVA (330 nm) rays penetrated approximately 1.6 times farther than UVB (310 nm) rays. A correlation between age and lower cheek elasticity was observed. Upon exposure to UV rays, collagen gels hardened and their elasticity decreased; UVA rays exhibited a stronger effect than UVB rays. Wavelengths of 300–340 nm caused hardening and reduced elasticity of collagen gels; 330-nm radiation showed the most pronounced effect. These effects were not observed upon exposure to UV wavelengths over 350 nm. Investigating the UV-hardening mechanism of collagen showed increased tyrosine crosslinks (dityrosines) in the in vitro model of photodamage to collagen, suggesting that dityrosine formation contributes to hardening and reduced elasticity of collagen in photoaged skin.

1. Introduction

The skin is the largest organ in the body, located at the interphase between the external and internal environment, requiring development of efficient sensory and effector capabilities to differentially react to changes in the environment [1]. The dermis is a 1.0–3.0-mm-thick layer of the skin on the inner side of the epidermis. The dermis is partly composed of extracellular matrix components, such as collagenous fibers, elastic fibers, and proteoglycans (e.g., hyaluronic acid and chondroitin sulfate), that contribute to the elasticity and strength of the skin. The dry weight of the dermis is approximately 70% collagenous fibers and 1–2% elastic fibers, that form a 3D structural network that maintains the elasticity of the dermis. Long-term exposure to UVB and UVA radiation in sunlight denatures the collagenous fibers in the dermis decreasing skin elasticity and causing wrinkles. Research into the effects of UVB and UVA rays on the skin of hairless mice has shown that daily exposure of hairless mice to UVB and UVA rays for two months led to a permanent decrease in skin elasticity [2,3,4]. However, long-term exposure to sunlight is needed for UVB and UVA rays to reduce skin elasticity in this way, which makes the evaluation of anti-photoaging agents in vivo problematic.
Currently, two standard test methods for efficacy of UVA protection are used internationally: the observation of persistent pigment darkening (PPD), which presents as immediate pigment darkening (IPD) 2–24 h after exposure in humans with skin type II to IV (in vivo) [5,6,7,8]; and the creation of an absorption curve of thin film or Transpore™ tape that has had the test material applied to it (in vitro) [9,10,11]. However, there is currently no standard evaluation method for the determination of the efficacy of UVA protection that considers the reduction in skin elasticity, which is the main damaging effect caused by UVB and UVA rays. Additionally, there is currently no research that has directly elucidated the correlation between the elasticity and the effect of UV radiation on the structure and function of collagenous fibers.
As it is not possible to employ traditional experimental methods using cell cultures or diluted collagen solutions to investigate the mechanism of elasticity reduction as a result of sunlight, new methods are needed to discover the actual mechanism of the reduction in elasticity caused by UVA rays. Dr. Bissett reported that increased skin thickness and wrinkles were induced by UVB radiation from 300 to 310 nm; however, skin sagging was induced by UVA radiation from 320 to 380 nm in hairless mice [12]. Previously studies of protective efficacy against skin damage caused by UVA rays were investigated [13,14,15]. IPD and PPD induced by UVA rays were clarified that their peaked at 340 nm and decreased gradually as the wavelength increased to 400 nm [16,17,18]. However, whether the wavelengths that damage collagen are the same as the wavelengths that cause IPD or PPD is not clarified yet. Therefore, current standard in vivo test methods for UVA protective efficacy that use skin PPD as an indicator, do not tell us how effective the UV protection products are for the prevention of elasticity reduction in the skin. Thus, analysis of the UV wavelengths that induce elasticity reduction in collagen fibers is of great academic significance. The collagen fiber model was exposed to ultraviolet (UV) rays, following which (1) hardness and elasticity were evaluated, (2) the spectra of wavelengths that caused an increase in hardness and decrease in elasticity were analyzed, and (3) biochemical mechanisms responsible for the increase in hardness and the decrease in elasticity were investigated.

2. Materials and Methods

2.1. Materials

An acidic collagen solution (native collagen bovine dermis; I-AC 3 mg/mL) from Koken Co., Ltd. (Tokyo, Japan) was used. Phosphate buffered saline (PBS) was prepared from PBS tablets (Takara Bio Inc., Shiga, Japan). Frozen Caucasian human breast skin disks 20 mm in diameter were purchased from KAC Co., Ltd. (Kyoto, Japan). A Capcell Pak C18 UG120 column (4.6 mm × 250 mm, C18 column; Shiseido Co., Ltd., Tokyo, Japan) was used for high-performance liquid chromatography (HPLC). All other materials were purchased from Wako Pure Pharmaceutical Industries Ltd. (Osaka, Japan).

2.2. Equipment

Dermaray 200 (Terumo Clinical Supply Co., Ltd., Tokyo, Japan) and Lightning Cure LC6 (150 W xenon lamp L8253; Hamamatsu Photonics K. K.; Hamamatsu, Japan) lamps were used as the UV sources. The long pass filter with 280 nm cutoff (A9616-03; Hamamatsu Photonics K. K.) was used in the Lightning Cure LC6. Elasticity was measured by a Cutometer MPA580 (Courage and Khazaka Electronic GmbH, Köln, Germany), and hardness was measured using a Rheo TEX SD-700 (Sun Scientific Co., Ltd., Tokyo, Japan). Edmund Optics 10-nm band-pass filters (300 nm, 310 nm, 320 nm, 330 nm, 340 nm, 350 nm, 360 nm, 370 nm, 380 nm), a high-performance liquid chromatography system (Shimadzu Corporation, Kyoto, Japan), and a high-speed centrifuge (Thermo Fisher Scientific, Waltham, MA, USA) were also used in the experiments.

2.3. Use of the Cutometer MPA580 and Rheo TEX SD-700

The probe of the Cutometer MPA580 was pressed to the skin surface, and using negative pressure suction the decrease in the internal pressure caused a skin bulge. The change in height of the bulge was accurately measured within 0.01 mm. This device measures displacement by repeated sudden decreases in pressure that are followed by sudden releases. Skin hardness and elasticity can be calculated from the maximal extension (Uf), which is the height of the skin that is induced by a constant negative pressure, and the immediate retraction (Ur) of the skin when the pressure is released. The smaller the ratio of the immediate retraction to the maximal extension (Ur/Uf) of the sample, the lower is the biological elasticity. Typical curves of normal skin and photoaged skin, as measured by the Cutometer MPA580, are shown in Figure 1. A difference between the normal skin and photoaged skin is observed (Figure 1). Cheek elasticity (Ur/Uf) decreases with age. Hardness can be measured using the Rheo TEX SD-700 by increasing the load on the measurement probe, once it reaches a fixed depth.

2.4. Exposure to UVB and UVA Lamps

Five different TL20W/12RS broadband UVB lamps (290–320 nm; peak, 305 nm; strength at 305 nm: 0.53 mW/cm2) and 10 FL20S BL/DMR lamps (320–400 nm; peak, 365 nm; strength at 365 nm: 8.20 mW/cm2) were used in the Dermaray 200. The collagen gels were exposed to UVB and UVA radiation. Unexposed collagen gels were covered with aluminum foil, and the foil-wrapped samples were then irradiated with UV rays for the same amount of time. The energy quantities in the experiments are detailed in Table 1. These exposures approximate 2 h of midsummer sun exposure, where solar UV rays consist of 0.75 J/cm2 UVB and 15 J/cm2 UVA (UVA-II 2.3 J/cm2, UVA-I 12.7 J/cm2). Given that only 10% of the absorbed UV rays penetrate to the dermis, the dermis is estimated to be exposed to 0.075 J/cm2 UVB and 1.5 J/cm2 UVA (UVA-II 0.23 J/cm2, UVA-I 1.27 J/cm2) radiation over this period. On the assumption that a year’s worth of exposure comprises 2 h per day for 30 days in the summer, the dermis is estimated to be exposed to 2.25 J/cm2 UVB and 45 J/cm2 UVA radiation (UVA-II 6.9 J/cm2, UVA-I 38.1 J/cm2) per year. Based on the same level of exposure over 2 and 3 years, the dermis is estimated to be exposed to 4.5 J/cm2 UVB and 90 J/cm2 UVA radiation (UVA-II 13.8 J/cm2, UVA-I 76.2 J/cm2), and 6.75 J/cm2 UVB and 135 J/cm2 UVA radiation (UVA-II 20.7 J/cm2, UVA-I 114.3 J/cm2), respectively. These estimated values were used as the exposure doses.

2.5. Measurement of Skin Transmittance for Different Wavelengths

Frozen 50-μm sections of Caucasian skin were sliced from the stratum corneum side, and sections of the stratum corneum side overlapping every 50 μm were exposed to UV rays from a xenon light source (Xe lamp L8253, 150 W, Lightning Cure LC6, Figure 2) that emits a UV spectrum similar to that of solar UV rays. The light detector of a spectroradiometer (USR-45, Ushio Co., Tokyo, Japan) contacted the opposite side of the tissue and measured the light output.

2.6. Measurement of Elasticity (Ur/Uf) in Humans of Various Ages

The biological elasticity (Ur/Uf) of the cheeks of 136 Japanese females (skin phototype II–IV, [19], average age: 37 years), ranging in age between 8 and 78, was measured under the following conditions. After face washing, the subjects were kept at constant temperature and humidity (22 °C ± 1.1 °C, 40% ± 2%) for 20 min and biological elasticity (Ur/Uf) was measured using the Cutometer MPA580 (pressure, 380 mbar; probe aperture, 2 mm; on-time, 2 s; off-time, 3 s; repetitions, 3; pre-time, 5 s). All volunteers had given their informed consent to participate, and the study protocol was approved by the ethics committee.

2.7. Measurement of Hardness and Elasticity of Collagen Gels

Sodium bicarbonate (NaHCO3), purified water, and acidic collagen solution (0.3%) were added to 10× PBS in 35-mm dishes to produce collagen gels. The gels were exposed to 3.2 J/cm2, 6.4 J/cm2, and 9.6 J/cm2 UVB by the Dermaray 200 with the TL20W/12RS broadband UVB lamps. They were also exposed to 49 J/cm2, 98 J/cm2, and 147 J/cm2 UVA from the FL20S BL/DMR lamps. Moreover, hardness of the collagen gels was measured using the Rheo TEX SD-700 (measurement parameters: distance, 1.0 mm; weight, 15 g), and elasticity (Ur/Uf) of the collagen gels was measured using the Cutometer MPA580.

2.8. Changes in the Hardness and Elasticity of Collagen Gels at Specific UV Wavelengths

Collagen gels were exposed to UV radiation at 10-nm intervals from a xenon lamp (Lightning Cure LC6) as a light source and a 10-nm band pass filter (300 nm, 310 nm, 320 nm, 330 nm, 340 nm, 350 nm, 360 nm, 370 nm and 380 nm) at the energies shown in Table 2. Exposure energies were determined based on the intensity of each wavelength in solar radiation. Furthermore, the exposure intensity of each band-pass filter was measured with a spectroradiometer. Hardness of the collagen gels was measured using the Rheo TEX SD-700, and biological elasticity (Ur/Uf) was measured using the Cutometer MPA580.

2.9. Measurement of Tyrosine Dimers in Collagen Gels

An aqueous solution of tyrosine made with L-tyrosine diluted in purified water to a concentration of 0.01 mg/mL was exposed to 330-nm UVA rays (26 J/cm2). Tyrosine reacted with horseradish peroxidase and hydrogen peroxide solution to form dityrosines [20]. Horseradish peroxidase (15 μg/mL), 5.25 mmol/L hydrogen peroxide, and 5 mmol/L of L-tyrosine were dissolved in 50 mL of 0.2 mol/L borate buffer (pH 9.5) and allowed to react at 37 °C. After neutralization with hydrochloric acid, dityrosine was collected by filtration through a C18 cartridge. Unreacted tyrosine, horseradish peroxidase, and hydrogen peroxide were washed away with 2 mL of purified water, and dityrosine was eluted with 5 mL of 20% methanol.
Five 330 nm UVA-exposed (26 J/cm2) collagen gel samples and five control non-exposed collagen gel samples were prepared using a 5 mm Dermapunch. The collagen samples were placed in 0.5 mol/L acetic acid for separation into acetic acid-soluble collagen and acetic acid-insoluble collagen. After the samples were concentrated by centrifugation, water was discarded and the samples were hydrolyzed with 6 mol/L hydrochloric acid. Two hundred microliters of the HCl-treated liquid were adjusted to pH 2 by the addition of 300 μL of 2 mol/L NaOH. Fluorescence intensities (Ex: 283 nm, Em: 415 nm) of the HCl hydrolysate of the UVA-exposed acetic acid-insoluble fraction of the collagen gels, the HCl hydrolysate of the UVA-exposed acetic acid-soluble fraction of the collagen gels, and the HCl hydrolysate of the non-exposed acetic acid-soluble fraction collagen gels were measured by HPLC.
HPLC was conducted on the Capcell PAK C18 UG120 column (4.6 mm × 250 mm, φ5 μm) with a flow rate of 0.8 mL/min and an injection volume of 5 μL, and fluorescence intensity of the eluents was detected (Ex: 283 nm, Em: 415 nm). The mobile phase was composed of (A) 0.5% acetic acid and (B) methanol (A:B = 24:1).

2.10. Statistical Analysis

An independent t-test for significance of the measured values was computed by Microsoft Excel.

3. Results

3.1. Skin Transmittance at Different Wavelengths

Figure 3 shows skin transmittance at different wavelengths of UV radiation. As the thickness of the human epidermis is approximately 100–200 μm and the thickness of the dermis is approximately 1000–2000 μm, UV radiation with wavelengths ≥300 nm reached the upper layer of the dermis. In the papillary dermis, at 200 μm, transmittance was calculated to be 5% of the 310-nm radiation the skin was exposed to, 8% of the 330-nm radiation, and 8.5% of the 340-nm radiation. Additionally, Table 3 shows the calculated values for the UVA (330 nm) and UVB (310 nm) transmittance in skin. The ratio of UVA transmittance to UVB transmittance was 1.20 in the epidermis at a depth of 100 μm, 1.60 at a depth of 200 μm (in the dermis), and 1.67 at a depth of 300 μm (in the dermis). In the dermis, at a depth of 300 μm, the effect of UVA radiation was 1.67 times bigger than that of UVB radiation.

3.2. Biological Elasticity (Ur/Uf) of the Cheek by Age in Humans

Figure 4 shows the relationship of biological elasticity (Ur/Uf) of cheek samples to the subject’s age in Japanese females. Data from 136 Japanese females, who were between 8 and 78 years old, showed that biological elasticity (Ur/Uf) decreased with age and that there was a correlation between increased age and decreased cheek elasticity.

3.3. Measurement of Collagen Gel Hardness and Elasticity

Collagen gels were exposed to UV rays using the TL20W/12RS broadband UVB lamps (290–320 nm; peak, 305 nm), and gel hardness was measured using the Rheo TEX SD-700 (Figure 5). The collagen gels that were exposed to 3.2 J/cm2, 6.4 J/cm2 and 9.6 J/cm2 UV radiation from the TL20W/12RS broadband UVB lamps were all significantly harder than the non-exposed collagen gels. Hardness of the collagen gels increased as the level of UV exposure from the TL20W/12RS broadband UVB lamps was increased: exposure to 3.2 J/cm2 increased the hardness by a factor of 1.4; exposure to 6.4 J/cm2 increased the hardness by a factor of 1.5; and exposure to 9.6 J/cm2 increased the hardness by a factor of two, compared to the unexposed control gels. Ur/Uf values were significantly decreased after exposure to 3.2 J/cm2, 6.4 J/cm2 and 9.6 J/cm2 UVB radiation, which indicated that the elasticity of the collagen gels decreased (Table 4).
Results of the collagen gel hardness measurements collected with the Rheo TEX SD-700 after exposure to the FL20S BL/DMR lamps (320–400 nm; peak, 365 nm) are shown in Figure 5. Exposure of the collagen gels to 49 J/cm2, 98 J/cm2, and 147 J/cm2 of UV rays from the FL20S BL/DMR lamps significantly increased hardness of the gels compared to the unexposed control gels. Hardness of the collagen increased with a higher level of exposure to UV rays from the FL20S BL/DMR lamps: exposure to 49 J/cm2 increased the hardness by a factor of two; exposure to 98 J/cm2 increased the hardness by a factor of 10; and exposure to 147 J/cm2 increased the hardness by a factor of 50, compared to the unexposed control gels. Effects of exposure to UVA radiation from the FL20S BL/DMR lamps on collagen elasticity were measured by the Cutometer MPA580 and are shown in Table 4. The Ur/Uf values were significantly decreased after exposure to 49 J/cm2, 98 J/cm2 and 147 J/cm2 UVA, which indicated that the elasticity of the collagen gels decreased.

3.4. Changes in Collagen Gel Hardness/Elasticity Due to Exposure to Different UV Wavelengths

The effects of different UV wavelengths on collagen gel hardening were observed by the exposure of the gels to the radiation energies shown in Table 2 at wavelengths spaced at approximately 10-nm intervals between 300–380 nm. The hardness of the collagen gels was measured using the Rheo TEX SD-700. The wavelengths from 300–340 nm caused collagen gel hardening, with the maximum effect observed at 330 nm. Wavelengths of 350–380 nm did not have any effect on collagen gel hardening (Figure 6). Additionally, the wavelengths of UV rays that affected the elasticity of the collagen gels were observed by exposure of the gels to the radiation energies shown in Table 2 at wavelengths with approximately 10-nm intervals between 300–380 nm. The elasticity of the collagen gels (Ur/Uf) was measured using the Cutometer MPA580. UV wavelengths of approximately 300–330 nm decreased the elasticity of collagen gels, with the maximum change occurring at 330 nm. Exposure to wavelengths between 340–380 nm did not reduce the elasticity of the collagen gels (Figure 7).

3.5. Measurement of Tyrosine Dimers in the Acetic Acid-Soluble Fraction and Acetic Acid-Insoluble Fraction of Collagen Gels Exposed to 330-nm UV Radiation

Retention times for synthesized dityrosine and for a solution of dityrosines formed by the exposure of tyrosine to 330 nm UV radiation were identical (Figure 8A), which showed that a tyrosine solution forms dityrosines upon exposure to 330 nm UV radiation. Unexposed collagen gels were completely dissolved in 0.5 mol/L acetic acid, but collagen gels that were exposed to 330 nm UV radiation yielded fractions that were insoluble in 0.5 mol/L acetic acid. In HPLC analysis, fluorescence intensity (Ex: 283 nm, Em: 450 nm) of the HCl hydrolysate of this insoluble fraction showed a peak with the same retention time as that of dityrosine (Figure 8B). Conversely, there was no peak at that retention time for the HCl hydrolysate of the acetic acid-soluble fraction (Figure 8C). Collagen gels that were not exposed to UVA rays did not have a dityrosine peak (Figure 8D).

3.6. Comparison of Wavelengths that Damage Collagen and Wavelengths that Induce IPD (Skin Type III)

The PA (Protection Grade for UVA), which is listed on cosmetic UV protection products in Japan, is based on the PFA (Protection Factor of UVA). The PFA uses PPD as an indicator. The literature-derived immediate pigment darkening (IPD) spectrum [15,17], PPD spectrum [17] and the spectra of UVB and UVA-II rays that cause hardening/reduced elasticity in collagen are shown in Figure 9; the hardness/elasticity reduction spectra are different from the IPD spectrum and the PPD spectrum.

4. Discussion

This study clearly showed that decreased cheek elasticity (Ur/Uf) was correlated with increased age in Japanese females as previously reported for Caucasian [21]. As cheeks receive significant exposure to solar UV radiation, solar UV radiation may contribute to this correlation; in addition, the natural aging process may contribute to this correlation. The results of our investigation into the transmittance of different wavelengths through the skin specimen showed that both UVB and UVA radiation reached the papillary layer and subpapillary layer of dermis. UVA (330 nm) transmittance was calculated to be 1.60 times higher than that of UVB (310 nm) in the dermis at a depth of 200 μm, and 1.67 times higher in the dermis at a depth of 300 μm; longer wavelengths penetrate more effectively to the dermis. It is thought that the ultraviolet ray transmissivity of the dermis changes according to the difference in the thickness of stratum corneum layers. Skin transmittance of different wavelengths of UV radiation is the result of carrying out by frozen skin specimen. By comparing with the experimental result in fresh human skin, skin transmittance of UV radiation will become clearer. Our collagen fiber model was exposed to 10 times the daily exposure of UVB and UVA rays using UVB lamps (290–320 nm; peak, 305 nm) and UVA lamps (320–400 nm; peak, 365 nm), which led to hardening of the collagen and a decrease in its elasticity. We found that UV radiation between 300–340 nm (UVB and UVA-II rays) caused these effects (with the maximum effect observed at 330 nm), while radiation at the wavelengths from 350–380 nm (UVA-I rays) did not have an effect. This system of evaluation considered one portion of the skin hardening and the elasticity reduction mechanism from continued exposure to UVB and UVA-II rays in vivo. In order to validate the data obtained from collagen gels, the evaluation is going to study ex vivo skin samples.
In addition to physiological damage that accompanies aging, skin is aged by the damage caused by long-term exposure to sunlight, especially UV rays, which is called photoaging. With aging, the collagen producing ability of dermal fibroblasts decreases, which results in decreased collagen in the dermis [22]. Conversely, in skin inflammation that arises from excessive UVB exposure, there is a transient increase in the inactivation of collagenases that degrade collagen that decreases the amount of collagen in the skin. However, it is not clear whether collagenases contribute to the breakdown of collagen in skin aging that results from chronic UVA exposure (i.e., photoaged skin that does not accompany inflammation). Instead, UVA rays are thought to exert a direct influence on the structure of collagen. This photoaging element has been shown to qualitatively alter collagenous fibers in the dermis. Solar UV rays that reach the Earth’s surface include wavelengths of 320–400 nm (UVA) and 290–320 nm (UVB). UVA rays have a longer wavelength than UVB rays, so UVA rays penetrate more deeply, as reflected by the changes observed in the collagen gels. Similarly, photoaged skin is harder and our collagen gel experiments suggested that regular exposure of the face to solar rays leads to skin hardening and reduced elasticity as a result of UV ray exposure, a process that promotes wrinkle formation. Metabolic turnover of collagen protein is slow; and the half-life of collagen in the skin is 14.8 years (95% confidence interval; 9.4–22.3 years), as calculated from the rate of racemization of aspartic acid [23]. Collagen damage accumulates from long-term exposure to solar rays, which reduce skin elasticity. Our model indicated that photoaging may be partially responsible for this cumulative damage. UV radiation at 330 nm hardens collagen and reduces its elasticity, suggesting that solar UV rays at this wavelength is likely to cause photoaging.
The International Commission on Illumination defined the standard doses of different wavelengths of UV radiation needed to cause erythema (skin reddening). According to the commission, the UVB range (280–300 nm) has a relatively large influence on erythema. Longer wavelengths (UVA rays; 300–320 nm) become rapidly less important, and wavelengths over 320 nm have virtually no effect on erythema. If the influence of the wavelengths in the 280–300 nm range is considered to be one, the relative influence of wavelengths in the UVA-II range, 320 nm and 340 nm, is 0.01 and 0.001, respectively. However, approximately five times more solar UV radiation in the UVA-II (320–340 nm) range reaches the Earth’s surface than UV radiation in the UVB (280–320 nm) range, so the influence of UVA-II rays cannot be ignored. Consequently, the most effective way to prevent photoaging is to avoid exposure to solar UV radiation of wavelengths shorter than 340 nm. It is also reported that UVA-I and UVA-II show a difference in the regulation of the immune function of the skin. Although UVA-II causes immune suppression like UVB, UVA-I may offer partial protection against UVB-induced immune suppression in human skin [24].
Dr. Kligman, a professor in the dermatology department of the University of Pennsylvania, used the term “photoaging skin” in 1986 to describe skin on the face, neck, and back of the hands that is repeatedly exposed to sunlight for long periods; this popularized the use of the word “photoaging” [25]. Skin photoaging is different from skin aging that occurs naturally with the passage of time. The skin loses its texture, becomes yellowed, loses its glossiness, multiple spots appear, and there is an increase in thick and deep wrinkles due to epidermal hyperplasia. Our results suggest that this increase in thick, deep wrinkles is caused by UVB and UVA radiation of wavelengths shorter than 340 nm. UVB and UVA are the only terms used to expediently differentiate between certain wavelengths; in practice, all wavelengths of solar UV radiation shorter than 340 nm are likely to cause photodamage to collagen. Consequently, the best way to prevent photodamage to collagen is to avoid exposure to solar UV rays of wavelengths lower than 340 nm.
Intermolecular crosslinking is necessary for collagenous fibers to maintain elasticity [26]. It is important to note that qualitative and quantitative changes in collagen fibril crosslinks occur naturally with age [27]. Through the measurement of fluorescence, researchers have found that the amount of collagen that can be digested by pepsin increases with age but is decreased by photoaging [28]. As collagen does not contain tryptophan, its fluorescence upon excitation by UVA irradiation mainly arises from tyrosine. Dityrosine crosslinking of collagen fibrils is known to increase with long-term exposure to UVA rays [29]. Our measurements of tyrosine dimers in collagen gels supported this, as dityrosines were formed in collagen gels upon exposure to UVA rays [30]. Dityrosines are not present in normal collagen; they may be rogue crosslinks formed by UVA exposure. Our experiments on UVA exposure of acetic acid-soluble and acid-insoluble collagen gels showed that tyrosine dimers (dityrosines) were formed in UVA-exposed acetic acid-insoluble gels.
Persistent pigment darkening (PPD) or persistent pigmentation (PP) as a result of UVA radiation peaked at 340 nm and gradually decreased at longer wavelengths up to 400 nm [7,15,17]. However, the wavelengths that damaged collagen gels were different from the spectrum of wavelengths that cause PPD or PP, so it remains unclear how much wrinkle protection is provided by UV protection products that have been evaluated by the current standard in vivo test methods for UVA protective efficacy (which use skin PPD as an indicator). Also, the PA (Protection Grade of UVA), which is listed on cosmetic UV-protection products in Japan, is based on the PFA (Protection Factor of UVA). PFA uses PPD as an indicator. The spectra of UV rays that caused hardening and reduced elasticity in collagen gels differed from the PPD spectrum. Thus, the efficacy of PA-rated products for protection against UVA radiation cannot be used to estimate the damage to collagen, which is representative of wrinkles, caused by UV radiation in the skin, and a new method to determine the protective efficacy of sunscreen products is required. Skin sagging is mainly caused by aging, and it is reported to be also caused by UVA radiation in the 320 to 380 nm range [12]. Elastin is a long-lasting protein like the collagen [31]. Accumulation of abnormal elastin is thought to be involved in sagging skin. Since elastase is participating in a rejuvenation of abnormal elastin just like collagenase is participating in a rejuvenation of abnormal collagen, development of an in vitro evaluation system containing collagen, elastin, and fibroblasts will be needed in future.

5. Conclusions

Radiation at wavelengths between 300–340 nm caused hardening and reduced the elasticity of collagen gels; radiation at 330 nm had the greatest effect. Hardening and elasticity-reduction effects were not observed upon exposure of the collagen gels to UV wavelengths over 350 nm. Spectra of UV rays that caused hardening and reduced elasticity in collagen gels differed from the PPD spectrum. Since PPD, which is used as one of the human PFA methods of sunscreen products against UVA radiation. Investigations of the UV hardening mechanism of collagen showed that there was an increase in tyrosine crosslinks (dityrosines) in the in vitro model of photodamage to collagen, which suggests that dityrosine formation contributes to the hardening and reduced elasticity of collagen in photoaged skin.

Acknowledgments

The author gratefully acknowledges the technical assistance of Hiroaki Akiyama, Keiko Ibushi and Nanako Hamano. The study was supported by a grant from the JSPS KAKENHI Grant Number 22500724.

Author Contributions

Kazuhisa Maeda designed the study and performed the experiment and the data analysis. Kazuhisa Maeda interpreted the data and drafted the manuscript.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. The typical curves of normal skin and photoaging skin measured by the Cutometer MPA580.
Figure 1. The typical curves of normal skin and photoaging skin measured by the Cutometer MPA580.
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Figure 2. Spectral comparison of the energy of the Xe light source and the solar ultraviolet radiation.
Figure 2. Spectral comparison of the energy of the Xe light source and the solar ultraviolet radiation.
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Figure 3. Skin transmittance of different wavelengths of UV radiation.
Figure 3. Skin transmittance of different wavelengths of UV radiation.
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Figure 4. Biological elasticity (Ur/Uf) of Japanese female’s cheeks by age.
Figure 4. Biological elasticity (Ur/Uf) of Japanese female’s cheeks by age.
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Figure 5. Change in hardness of collagen gels irradiated with either UVB lamps or UVA lamps measured by the Rheo TEX SD-700. n = 6, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2, *** p < 0.001 vs. 0 J/cm2.
Figure 5. Change in hardness of collagen gels irradiated with either UVB lamps or UVA lamps measured by the Rheo TEX SD-700. n = 6, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2, *** p < 0.001 vs. 0 J/cm2.
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Figure 6. Dynamic spectrum of the hardness of collagen gels irradiated with UV rays measured by the Rheo TEX SD -700. n = 5, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2, *** p < 0.001 vs. 0 J/cm2.
Figure 6. Dynamic spectrum of the hardness of collagen gels irradiated with UV rays measured by the Rheo TEX SD -700. n = 5, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2, *** p < 0.001 vs. 0 J/cm2.
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Figure 7. Dynamic spectrum of the Ur/Uf value of collagen gels irradiated with UV rays. n = 5, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2, *** p < 0.001 vs. 0 J/cm2.
Figure 7. Dynamic spectrum of the Ur/Uf value of collagen gels irradiated with UV rays. n = 5, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2, *** p < 0.001 vs. 0 J/cm2.
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Figure 8. HPLC analysis of dityrosine in collagen gels irradiated by UVA (A) Dityrosine formation by tyrosine irradiated by UVA; (B) Dityrosine in acetic acid-insoluble collagen (collagen irradiated by UVA); (C) Dityrosine in acetic acid-soluble collagen (collagen irradiated by UVA); and (D) Collagen not irradiated by UVA.
Figure 8. HPLC analysis of dityrosine in collagen gels irradiated by UVA (A) Dityrosine formation by tyrosine irradiated by UVA; (B) Dityrosine in acetic acid-insoluble collagen (collagen irradiated by UVA); (C) Dityrosine in acetic acid-soluble collagen (collagen irradiated by UVA); and (D) Collagen not irradiated by UVA.
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Figure 9. Comparison of the spectrum of UV radiation that damages collagen and the spectra of IPD, 24 h after irradiation of PP (PPD; persistent pigment darkening), PP (1 week after irradiation) [17].
Figure 9. Comparison of the spectrum of UV radiation that damages collagen and the spectra of IPD, 24 h after irradiation of PP (PPD; persistent pigment darkening), PP (1 week after irradiation) [17].
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Table 1. Irradiation energy of Dermaray 200.
Table 1. Irradiation energy of Dermaray 200.
TL20W/12RS Broadband UVB Lamps
(290 nm–320 nm, Peak 305 nm)
FL20S BL/DMR Lamps
(320 nm–400 nm, Peak 365 nm)
0 J/cm20 J/cm2
3.2 J/cm249 J/cm2
6.4 J/cm298 J/cm2
9.6 J/cm2147 J/cm2
Table 2. Spectral irradiation energy with a band pass filter of the radiation from the Light Source Lightning Cure LC6 (Xe lamp L8253).
Table 2. Spectral irradiation energy with a band pass filter of the radiation from the Light Source Lightning Cure LC6 (Xe lamp L8253).
Wavelength (nm)Irradiation Energy (J/cm2)
3002
31010
32032
33074
34084
35094
360108
370140
380150
Table 3. Relationship of the depth of the skin transmissivity of UVB and UVA radiation.
Table 3. Relationship of the depth of the skin transmissivity of UVB and UVA radiation.
Skin Transmissivity of UVTransmittance of UVB (%) (at 310 nm)Transmittance of UVA (%) (at 330 nm)The Ratio of UVA to UVB
Epidermis 100 μm30361.20
Epidermis 100 μm + Dermis 50 μm 18.522.51.22
Epidermis 100 μm + Dermis 100 μm 12151.25
Epidermis 100 μm + Dermis 200 μm 581.60
Epidermis 100 μm + Dermis 300 μm 351.67
Table 4. Change in elasticity (Ur/Uf) of collagen gels irradiated with either UVB lamps or UVA lamps measured by the Cutometer MPA580.
Table 4. Change in elasticity (Ur/Uf) of collagen gels irradiated with either UVB lamps or UVA lamps measured by the Cutometer MPA580.
Unexposed Collagen GelsUr/Uf0.59 ± 0.030.57 ± 0.020.59 ± 0.030.63 ± 0.14
TL20W/12RS Broadband UVB Lamps
(290 nm–320 nm, Peak 305 nm) Exposed Collagen Gels
Energy0 J/cm23.2 J/cm26.4 J/cm29.6 J/cm2
Ur/Uf0.59 ± 0.030.53 ± 0.05 *0.52 ± 0.02 **0.50 ± 0.04 **
FL20S BL/DMR Lamps
(320 nm–400 nm, Peak 365 nm) Exposed Collagen Gels
Energy0 J/cm249 J/cm298 J/cm2147 J/cm2
Ur/Uf0.60 ± 0.110.50 ± 0.01 **0.48 ± 0.02 **0.42 ± 0.04 **
n = 6, Mean ± S.D., * p < 0.05 vs. 0 J/cm2, ** p < 0.01 vs. 0 J/cm2.

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Maeda, K. Analysis of Ultraviolet Radiation Wavelengths Causing Hardening and Reduced Elasticity of Collagen Gels In Vitro. Cosmetics 2018, 5, 14. https://doi.org/10.3390/cosmetics5010014

AMA Style

Maeda K. Analysis of Ultraviolet Radiation Wavelengths Causing Hardening and Reduced Elasticity of Collagen Gels In Vitro. Cosmetics. 2018; 5(1):14. https://doi.org/10.3390/cosmetics5010014

Chicago/Turabian Style

Maeda, Kazuhisa. 2018. "Analysis of Ultraviolet Radiation Wavelengths Causing Hardening and Reduced Elasticity of Collagen Gels In Vitro" Cosmetics 5, no. 1: 14. https://doi.org/10.3390/cosmetics5010014

APA Style

Maeda, K. (2018). Analysis of Ultraviolet Radiation Wavelengths Causing Hardening and Reduced Elasticity of Collagen Gels In Vitro. Cosmetics, 5(1), 14. https://doi.org/10.3390/cosmetics5010014

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