RESIN COMPOSITION QUALITY CONTROLLING METHOD, CABLE AND TUBE QUALITY CONTROLLING METHOD, DETERMINATION DEVICE, INSPECTION SYSTEM, CABLE, AND TUBE

Abstract

A resin composition quality controlling method includes a step of measuring a Raman spectrum of a resin composition composed of first TiO.sub.2 particles of anatase type TiO.sub.2 and second TiO.sub.2 particles of rutile type TiO.sub.2 by irradiation with laser, and determining a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition based on an intensity of a first peak assigned to lattice vibration in the anatase type TiO.sub.2 and an intensity of a second peak assigned to lattice vibration in the rutile type TiO.sub.2 in the Raman spectrum.

Claims

1. A resin composition quality controlling method, comprising: measuring a Raman spectrum of a resin composition comprising first TiO.sub.2 particles comprising anatase type TiO.sub.2 and second TiO.sub.2 particles comprising rutile type TiO.sub.2 by irradiation with laser, and determining a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition based on an intensity of a first peak assigned to lattice vibration in the anatase type TiO.sub.2 and an intensity of a second peak assigned to lattice vibration in the rutile type TiO.sub.2 in the Raman spectrum.

2. The resin composition quality controlling method according to claim 1, wherein the first peak comprises a peak exhibiting a highest intensity in a range of not less than 365 cm.sup.−1 and not more than 425 cm.sup.−1 or a peak exhibiting a highest intensity in a range of not less than 485 cm.sup.−1 and not more than 545 cm.sup.−1 in the Raman spectrum, and wherein the second peak comprises a peak exhibiting a highest intensity in a range of not less than 205 cm.sup.−1 and not more than 265 cm.sup.−1 or a peak exhibiting a highest intensity in a range of not less than 415 cm.sup.−1 and not more than 475 cm.sup.−1 in the Raman spectrum.

3. The resin composition quality controlling method according to claim 1, wherein in the determining, a peak height ratio of the first peak to the second peak is obtained from the Raman spectrum, and a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition is determined by referring to a relationship obtained in advance between the peak height ratio and the concentration ratio.

4. The resin composition quality controlling method according to claim 1, wherein in the determining, an integral intensity ratio of the first peak to the second peak is obtained from the Raman spectrum, and a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition is determined by referring to a relationship obtained in advance between the integral intensity ratio and the concentration ratio.

5. A cable and tube quality controlling method, comprising: determining a concentration ratio in an insulator being provided on a cable or a tube and comprising the resin composition by the resin composition quality controlling method according to claim 1.

6. A determination device configured to perform the determining in the resin composition quality controlling method according to claim 1.

7. An inspection system, comprising: a Raman measurement device configured to perform the measuring in the resin composition quality controlling method according to claim 1; and a determination device configured to perform the determining in the resin composition quality controlling method according to claim 1.

8. A cable, comprising: an insulator comprising a resin composition comprising first TiO.sub.2 particles comprising anatase type TiO.sub.2 and second TiO.sub.2 particles comprising rutile type TiO.sub.2.

9. A tube, comprising: an insulator comprising a resin composition comprising first TiO.sub.2 particles comprising anatase type TiO.sub.2 and second TiO.sub.2 particles comprising rutile type TiO.sub.2.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0019] FIG. 1 is a vertical cross-sectional view showing a resin composition according to the first embodiment of the present invention.

[0020] FIG. 2 is a graph showing Raman spectra of anatase type TiO.sub.2 and rutile type TiO.sub.2.

[0021] FIG. 3 is a schematic plan view showing a configuration of an ultrasonic probe cable in the second embodiment of the invention.

[0022] FIG. 4A is a radial cross-sectional view showing a cable of the ultrasonic probe cable.

[0023] FIG. 4B is a radial cross-sectional view showing the ultrasonic probe cable taken along line A-A shown in FIG. 3.

[0024] FIG. 5 is a radial cross-sectional view showing a medical tube in the second embodiment of the invention.

[0025] FIGS. 6A and 6B are schematic side and top views showing a configuration example of a cable inspection system used for a method for controlling the quality of a cable.

[0026] FIG. 7 is a schematic diagram illustrating a probe portion of a Raman measurement device that includes a circumference measuring unit.

[0027] FIGS. 8A and 8B are graphs showing Raman spectra of resin compositions including first TiO.sub.2 particles composed of anatase type TiO.sub.2 and second TiO.sub.2 particles composed of rutile type TiO.sub.2.

[0028] FIG. 9A is a graph showing a relationship between a value of a ratio of a peak height of a peak A2 to a total of the peak height of the peak A2 and a peak height of a peak B2 (a peak height ratio) and a mass fraction of the first TiO.sub.2 particles in TiO.sub.2 particles 11.

[0029] FIG. 9B is a graph showing a relationship between a value of a ratio of the integral intensity of the peak A2 to a total of the integral intensity of the peak A2 and the integral intensity of the peak B2 (an integral intensity ratio) and the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11.

[0030] FIG. 10A is a graph showing a relationship between a value of a ratio of the peak height of the peak A2 to a total of the peak height of the peak A2 and a peak height of a peak B1 (a peak height ratio) and the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11.

[0031] FIG. 10B is a graph showing a relationship between a value of a ratio of the integral intensity of the peak A2 to a total of the integral intensity of the peak A2 and the integral intensity of the peak B1 (an integral intensity ratio) and the mass fraction of the first 102 particles in the TiO.sub.2 particles 11.

[0032] FIG. 11A is a graph showing a relationship between a value of a ratio of a peak height of a peak A1 to a total of the peak height of the peak A1 and the peak height of the peak B2 (a peak height ratio) and the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11.

[0033] FIG. 11B is a graph showing a relationship between a value of a ratio of the integral intensity of the peak A1 to a total of the integral intensity of the peak A1 and the integral intensity of the peak B2 (an integral intensity ratio) and the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11.

DESCRIPTION OF EMBODIMENTS

First Embodiment

[0034] (Configuration of Resin Composition)

[0035] FIG. 1 is a vertical cross-sectional view showing a resin composition 1 in the first embodiment of the invention. The resin composition 1 includes a resin 10 as a base material such as silicone rubber, and TiO.sub.2 particles 11, which are included in the resin 10.

[0036] The TiO.sub.2 particles 11 as an ultraviolet light shielding material to shield UV-C light by absorption and/or scattering are added to the resin composition 1. TiO.sub.2 has a higher scattering coefficient for ultraviolet light than white pigment ZnO or silicone resin and has an excellent ultraviolet light shielding function. A particle diameter of the TiO.sub.2 particles 11 is, e.g., 10 to 500 nm.

[0037] The TiO.sub.2 particles 11 include TiO.sub.2 particles composed of anatase type TiO.sub.2 (referred to as first TiO.sub.2 particles) and TiO.sub.2 particles composed of rutile type TiO.sub.2 (referred to as second TiO.sub.2 particles). Anatase type TiO.sub.2 has a higher absorbance of ultraviolet light in the UV-C region (200 to 280 nm) than rutile type TiO.sub.2. Meanwhile, the rutile type TiO.sub.2 can absorb longer wavelength ultraviolet light, as compared to anatase type TiO.sub.2 (rutile type TiO.sub.2 can absorb ultraviolet light at about not more than 400 nm, while anatase type TiO.sub.2 can absorb ultraviolet light at about not more than 370 nm).

[0038] Thus, since the TiO.sub.2 particles 11 include both the first TiO.sub.2 particles composed of anatase type TiO.sub.2 and the second TiO.sub.2 particles composed of rutile type TiO.sub.2, the resin composition 1 has excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range. When resistance to UV-C light is particularly important, a proportion of the first TiO.sub.2 particles should be increased, that is, a value of a ratio of the mass of the first TiO.sub.2 particles to the mass of the second TiO.sub.2 particles should be increased. When resistance to long-wavelength ultraviolet light (UV-A, etc.) is particularly important, a proportion of the second TiO.sub.2 particles should be increased, that is, a value of a ratio of the mass of the first TiO.sub.2 particles to the mass of the second TiO.sub.2 particles should be decreased.

[0039] As the resin 10, it is possible to use, e.g., silicone rubber, polyethylene, chlorinated polyethylene, chloroprene rubber, polyvinyl chloride (PVC), polyurethane, etc. Of those, silicone rubber and chloroprene rubber are preferable from the viewpoint of chemical resistance and heat resistance. Meanwhile, silicone rubber is preferable from the viewpoint of resistance to ultraviolet light. When the resin composition 1 is used as a cable sheath material, common compounding agents such as various cross-linking agents, cross-linking catalysts, antioxidants, plasticizers, lubricants, fillers, flame retardants, stabilizers, and colorants may be added to the resin 10.

[0040] The resin composition 1 can be in a variety of forms depending on its intended use. The resin composition 1 is molded into, e.g., a tube shape when used as an insulator of a cable or a tube, and is molded into a sheet shape when used as a highly UV-resistant sheet for constant temperature house or an ultraviolet shielding sheet (ultraviolet shielding curtain) to shield against ultraviolet light leakage from a sterilization chamber, etc.

[0041] (Method for Controlling the Quality of Resin Composition)

[0042] In the resin composition quality controlling method in the first embodiment, a concentration ratio of the first TiO.sub.2 particles composed of anatase type TiO.sub.2 to the second TiO.sub.2 particles composed of rutile type TiO.sub.2 included in the resin composition 1 can be measured by Raman scattering measurement in a non-destructive, non-contact manner while maintaining the original shape of the resin composition 1. The concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles can be expressed by, e.g., a mass fraction of the first TiO.sub.2 particles or the second TiO.sub.2 particles in the TiO.sub.2 particles 11.

[0043] The resin composition quality controlling method in the first embodiment includes, e.g., a measurement step of measuring a Raman spectrum of the resin composition 1 by irradiation with laser, and a determination step of determining the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 based on the intensity of a peak assigned to lattice vibration in the anatase type TiO.sub.2 (referred to as a first peak) and intensity of a peak assigned to lattice vibration in the rutile type TiO.sub.2 (referred to as a second peak) in the measured Raman spectrum. Here, the intensity of the peak in the Raman spectrum in the embodiments means peak height or integral intensity.

[0044] The intensity of the first peak in the Raman spectrum varies with the content of the anatase type TiO.sub.2 in the resin composition 1, and the intensity of the second peak varies with the content of the rutile type TiO.sub.2 in the resin composition 1. Therefore, based on these intensities, it is possible to determine the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1.

[0045] The first peak assigned to lattice vibration in the anatase type TiO.sub.2 is, e.g., a peak exhibiting the highest intensity in a range of not less than 365 cm.sup.−1 and not more than 425 cm.sup.−1 (referred to as a peak A1), or a peak exhibiting the highest intensity in a range of not less than 485 cm.sup.−1 and not more than 545 cm-n (referred to as a peak A2), in the Raman spectrum. Meanwhile, the second peak assigned to lattice vibration in the rutile type TiO.sub.2 is a peak exhibiting the highest intensity in a range of not less than 205 cm.sup.−1 and not more than 265 cm.sup.−1 (referred to as a peak B1), or a peak exhibiting the highest intensity in a range of not less than 415 cm.sup.−1 and not more than 475 cm.sup.−1 (referred to as a peak B2), in the Raman spectrum. In this regard, wavenumbers at which the first peak and the second peak exhibit the highest intensities can shift within the above-mentioned ranges depending on the temperature of the resin composition 1, etc., at the time of measurement. The wavenumber range for the highest intensity of the peak A1 partially overlaps that of the peak B2 as described above, but the two can be distinguished since the peak B2 always appears on the long wavelength side of the peak A1.

[0046] FIG. 2 is a graph showing Raman spectra of the anatase type TiO.sub.2 and the rutile type TiO.sub.2. In the Raman spectrum of the anatase type TiO.sub.2, the peak A1 exhibiting the highest intensity at about 395 cm.sup.−1 is a peak resulting from lattice vibration B.sub.1g in the anatase type TiO.sub.2, and the peak A2 exhibiting the highest intensity at about 515 cm.sup.−1 is a peak resulting from lattice vibrations A.sub.1g, B.sub.1g in the anatase type TiO.sub.2. Meanwhile, the peak B2 exhibiting the highest intensity at about 443 cm.sup.−1 is a peak resulting from lattice vibration E.sub.g in the rutile type TiO.sub.2.

[0047] In this regard, Raman spectrum peaks of the anatase type TiO.sub.2 other than the peaks A1, A2, or Raman spectrum peaks of the rutile type TiO.sub.2 other than the peaks B1, B2 (vibrational modes are indicated in parentheses in FIG. 2) may be used to determine the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles.

[0048] By examining in advance a correlation between an intensity ratio of the first peak to the second peak and the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1, the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 can be obtained from the intensity ratio of the measured first peak to the measured second peak. In this regard, the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 can be obtained by, e.g., measuring the respective weights of the first TiO.sub.2 particles and the second TiO.sub.2 particles, or by analysis using X-ray diffraction technique or TEM-EELS method (electron energy-loss spectroscopy) which can identify respective crystal structures of the first TiO.sub.2 and the second TiO.sub.2, etc. Then, the correlation between the intensity ratio of the first peak to the second peak and the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 can be examined by conducting Raman scattering measurement on the resin composition 1 for which the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles has been measured.

[0049] Here, the integral intensities and the peak heights of the first peak and the second peak are computed using a peak profile obtained by fitting analysis using a statistical distribution function such as the Pseudo-Voigt function, Lorentz function, or Gauss distribution function, and are obtained after background correction of the peak profile. The background correction is conducted to eliminate background effects that are not due to the molecular structures of the resin 10 and the TiO.sub.2 particles 11 but attributed to unavoidable light such as generated fluorescence, Rayleigh and Mie scattered light originating from irradiation laser light, and disturbing light other than the irradiation laser light, etc., and is performed by subtracting the background profile (baseline), which is obtained by fitting analysis using a polynomial function or a spline function, from the peak profile described above. The integration range in determining the integral intensities of the first peak and the second peak is a range between two intersections of the peak profile described above and the background profile.

[0050] In the Raman scattering measurement in the resin composition quality controlling method in the first embodiment, a spot diameter of laser irradiated onto a surface of the resin composition 1 is a measuring area, hence, evaluation can be performed within a microscopic region with a diameter of not more than 1 μm (e.g., 0.4 to 1.0 μm). That is, it is possible to obtain not only average information about the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 but also information for each microscopic region, enabling more precise control of the quality of the resin composition 1. In this regard, the above-mentioned value is not the limit value for the laser spot diameter. In principle, the laser spot diameter is determined by the wavelength of a laser source and the numerical aperture of an objective lens. Therefore, when Raman spectroscopy analysis is performed on the resin composition 1 by using the laser with a shorter wavelength and an objective lens with a large numerical aperture, it is possible to measure in even smaller microscopic regions of less than 0.4 μm.

[0051] In addition, in the Raman scattering measurement in the resin composition quality controlling method in the first embodiment, a wavenumber region where the first peak that is assigned to lattice vibration in the anatase type TiO.sub.2 and the second peak that is assigned to lattice vibration in the rutile type TiO.sub.2 are observed is separated from a wavenumber region where peaks assigned to stretching or bending vibrations characteristic of a resin constituting the resin 10, such as silicone rubber (fingerprint region: about 800 to 1300 cm.sup.−1), are observed. Therefore, it is possible to obtain the precise concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1.

[0052] In addition, the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 in various forms can be measured by using a gun-type Raman measurement device of which the probe portion including a laser emitting portion and a scattered light receiving portion can be moved freely.

Second Embodiment

[0053] The second embodiment of the invention relates to a cable or a tube that includes an insulator composed of the resin composition 1 in the first embodiment. Next, an example of such a cable used for a medical ultrasonic probe cable will be described.

[0054] FIG. 3 is a schematic plan view showing a configuration of an ultrasonic probe cable 2 in the second embodiment of the invention. As shown in FIG. 3, the ultrasonic probe cable 2 is configured such that an ultrasonic probe 32 is attached to an end portion of a cable 20 via a boot 31 protecting the end portion. Then, a connector 33 to be connected to a main body of an ultrasonic imaging device is attached to the other end of the cable 20.

[0055] FIG. 4A is a radial cross-sectional view showing the cable 20 of the ultrasonic probe cable 2. Inside the cable 20, e.g., plural electric wires 21 typified by coaxial cable are housed and a shield 22 such as a braided shield is provided so as to cover the plural electric wires 21. Then, a sheath 23 is provided so as to cover the shield 22.

[0056] FIG. 4B is a radial cross-sectional view showing the ultrasonic probe cable 2 taken along line A-A shown in FIG. 3. As shown in FIG. 4B, the boot 31 is attached to the sheath 23 via an adhesive layer 34 so as to cover the sheath 23. The adhesive layer 34 is composed of, e.g., a silicone-based adhesive or an epoxy-based adhesive. Meanwhile, the boot 31 is composed of, e.g., PVC, silicone rubber or chloroprene rubber, etc., and preferably contains TiO.sub.2 to shield UV-C light or an organic UV light absorbing agent.

[0057] The sheath 23 of the cable 20 is composed of the resin composition 1. That is, the cable 20 includes an insulator (the sheath 23) composed of the resin composition 1 including the first TiO.sub.2 particles composed of the anatase type TiO.sub.2 and the second TiO.sub.2 particles composed of the rutile type TiO.sub.2. The TiO.sub.2 particles 11 in the sheath 23 are not shown in the drawing.

[0058] By using the resin composition 1 having excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range as a material of the sheath 23, it is possible to obtain the cable 20 which has excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range. The cable 20 may additionally have a coating film composed of the resin composition 1 on a surface of the sheath 23. In this case, the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles may be different between the coating film and the sheath 23.

[0059] Next, an example of a method for manufacturing the ultrasonic probe cable 2 in the second embodiment will be described. Firstly, plural (e.g., not less than one hundred) electric wires 21 are bundled together. Then, the shield 22 is formed to cover the bundled electric wires 21. Subsequently, the sheath 23 composed of the resin composition 1 is formed to cover the shield 22. The sheath 23 is formed by, e.g., extrusion using an extruder.

[0060] Next, a configuration of a tube (a hollow tube) used for medical applications such as a catheter will be described as another example of the cable or tube including an insulator composed of the resin composition 1.

[0061] FIG. 5 is a radial cross-sectional view showing a medical tube 4 in the second embodiment of the invention. The medical tube 4 includes an insulating tube main body 40 composed of the resin composition 1. That is, the medical tube 4 includes an insulator (the tube main body 40) composed of the resin composition 1 including the first TiO.sub.2 particles composed of the anatase type TiO.sub.2 and the second TiO.sub.2 particles composed of the rutile type TiO.sub.2. The TiO.sub.2 particles 11 in the tube main body 40 are not shown in the drawing.

[0062] By using the resin composition 1 having excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range as a material of the tube main body 40, it is possible to obtain the medical tube 4 which has excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range. The medical tube 4 may additionally have a coating film composed of the resin composition 1 on an inner surface, or an outer surface, or the inner and outer surfaces of the tube main body 40. In this case, the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles may be different between the coating film and the tube main body 40.

[0063] (Method for Controlling the Quality of Cable or Tube)

[0064] According to the second embodiment, as the cable and tube quality controlling method with an insulator composed of the resin composition 1, it is possible to provide a cable and tube quality controlling method, in which the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the insulator is determined using the resin composition quality controlling method described above.

[0065] FIGS. 6A and 6B are schematic side and top views showing a configuration example of a cable inspection system 50 used for a method for controlling the quality of a cable. The cable inspection system 50 is configured to inspect a cable 70 including an insulator including the first TiO.sub.2 particles and the second TiO.sub.2 particles, such as the cable 20 described above and configured to measure the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the insulator.

[0066] The cable inspection system 50 includes an introduction reel 51 to introduce the cable 70 into the cable inspection system 50, a sending reel 52 to send out the cable 70 introduced by the introduction reel 51 to the measuring area for Raman scattering measurement, a receiving reel 53 to receive the cable 70 which passed through the measuring area, a wind-up coil 54 to wind up the cable 70 received by the receiving reel 53, a sending guide jig 55 placed between the introduction reel 51 and the sending reel 52 to guide advance of the cable 70, a receiving guide jig 56 placed between the receiving reel 53 and the wind-up coil 54 to guide advance of the cable 70, a support 57 to support the sending reel 52 and the receiving reel 53, etc., and a Raman measurement device 58 to perform measurement on the insulator of the cable 70 between the sending reel 52 and the receiving reel 53.

[0067] Regarding the Raman measurement device 58, only a probe portion thereof is schematically shown in FIGS. 6A and 6B. The probe portion of the Raman measurement device 58 has an objective lens 59 that focuses laser light L to the insulator of the cable 70.

[0068] With the cable inspection system 50, it is possible to measure the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the insulator in the original state of the cable 70 without destroying the cable 70.

[0069] The probe portion of the Raman measurement device 58 may include a circumference measuring unit 60 which has plural objective lenses 59 arranged to surround the cable 70, as shown in FIG. 7. Raman scattering measurement can be performed over the entire circumference of the cable 70 by using the circumference measuring unit 60. Alternatively, the circumference measuring unit 60 may have a structure to perform Raman scattering measurement over the entire circumference of the cable 70 by moving one objective lens 59 along the circumferential direction of the cable 70. In addition, the Raman measurement device 58 may be a gun-type Raman measurement device of which the probe portion can be moved freely.

[0070] The Raman measurement device 58 may be connected to a determination device that determines the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the insulator of the cable 70 based on the intensity of the first peak assigned to lattice vibration in the anatase type TiO.sub.2 and intensity of the second peak assigned to lattice vibration in the rutile type TiO.sub.2 in the Raman spectrum. This determination device is, e.g., a personal computer with a program to perform the above-mentioned determination stored in storage. This determination device can be also used for quality control of the resin composition 1 in a form other than the insulator of the cable 70. That is, according to the invention, it is possible to provide a determination device configured to perform the above-described determination step in the method for controlling the quality of the resin composition 1.

[0071] The Raman measurement device 58 also can perform the measurement step by Raman measurement in the method for controlling the quality of the cable in the second embodiment. The Raman measurement device 58 can be also used for measurement of the resin composition 1 in a form other than the insulator of the cable 70. That is, according to the invention, it is possible to provide an inspection system that includes the Raman measurement device 58 configured to perform the above-described measurement step in the method for controlling the quality of the resin composition 1, and the determination device configured to perform the above-described determination step in the method for controlling the quality of the resin composition 1.

[0072] (Effects of the Embodiments)

[0073] According to the first embodiment, to provide a resin composition having excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range, the concentration ratio of the anatase type TiO.sub.2 to the rutile type TiO.sub.2 in the resin composition 1 can be determined using Raman scattering measurement.

[0074] According to the second embodiment, it is possible to provide a cable or a tube that includes an insulator including the first TiO.sub.2 particles composed of the anatase type TiO.sub.2 and the second TiO.sub.2 particles composed of the rutile type TiO.sub.2 and has excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range. In addition, according to the second embodiment, to provide a cable or a tube having excellent resistance to UV-C light and resistance to ultraviolet light in a wide wavelength range, the concentration ratio of the anatase type TiO.sub.2 to the rutile type TiO.sub.2 in the insulator of the cable or the tube can be determined using Raman scattering measurement.

[0075] In addition, the resin composition quality controlling method, the cable and tube quality controlling method, and the determination device and the inspection system used in the cable and tube quality controlling method, etc., according to the embodiments described above can be also applied to material development using Materials Informatics (MI) which uses machine learning or artificial intelligence (AI), etc., to analyze data.

EXAMPLE

[0076] This Example shows an example of a step of determining the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the insulator of the cable based on the intensity of the first peak assigned to lattice vibration in the anatase type TiO.sub.2 and the intensity of the second peak assigned to lattice vibration in the rutile type TiO.sub.2 in the Raman spectrum.

[0077] The resin composition 1 formed using silicone rubber as the resin 10 and shaped into a sheet shape was prepared and Raman scattering measurement was performed. The Raman scattering measurement was performed using RAMANforce Standard VIS-NIR-HS available from Nanophoton Corporation under the following measurement conditions: a wavelength of the laser was 532 nm, a width of an incident slit of a spectrometer was 50 μm, the number of rulings in a diffraction grating was 300 gr/mm, a value of a ratio of the amount of light after attenuation to the maximum amount of laser light of an ND filter (an attenuation ratio) was 250/255, magnification, numerical aperture (NA) and theoretical measurement diameter of an objective lens were respectively 5×, 0.15 and 2.2 μm, and counting time was 1 second×20 cycles. In addition, the Raman scattering measurement was performed in an environment where the temperature was 20° C. (an average value from a 2-point measurement in an analysis laboratory), the humidity was 28 RH % (an average value from a 3-point measurement in the analysis laboratory), and air pressure was normal pressure (so-called atmospheric pressure).

[0078] FIGS. 8A and 8B are graphs showing Raman spectra of the resin compositions 1 including the first TiO.sub.2 particles composed of the anatase type TiO.sub.2 and the second TiO.sub.2 particles composed of the rutile type TiO.sub.2. FIGS. 8A and 8B show the same Raman spectra. The numerical values on the right side of each Raman spectrum in FIGS. 8A and 8B indicate the mass fraction (%) of the first TiO.sub.2 particles in the TiO.sub.2 particles 11.

[0079] FIG. 9A is a graph showing a relationship between a value of a ratio of the peak height of the peak A2 to the total of the peak height of the peak A2 and the peak height of the peak B2 (a peak height ratio) and the mass fraction of the first TiO.sub.2 particles in TiO.sub.2 particles 11 obtained by measuring respective weights of the first TiO.sub.2 particles and the second TiO.sub.2 particles. FIG. 9B is a graph showing a relationship between a value of a ratio of the integral intensity of the peak A2 to the total of the integral intensity of the peak A2 and the integral intensity of the peak B2 (an integral intensity ratio) and the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 obtained by measuring respective weights of the first TiO.sub.2 particles and the second TiO.sub.2 particles. The mass fraction (%) of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 here is expressed by the mass of the first TiO.sub.2 particles/(the mass of the first TiO.sub.2 particles and the mass of the second TiO.sub.2 particles)×100.

[0080] Table 1 below shows the peak height ratio and the integral intensity ratio for each mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 for each plotted point in FIGS. 9A and 9B, and the peak height and the integral intensity of each of the peak A2 and the peak B2 for each mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 which were used to calculate the ratios.

TABLE-US-00001 TABLE 1 Peak A2 Peak B2 Peak Integral Peak Integral Peak Integral height intensity height intensity height intensity ratio ratio Mass  0% 0 0 23769 1644682 0 0 fraction 10% 422 2922 22205 791024 0.019 0.004 of First 25% 1285 7890 22503 294511 0.140 0.071 TiO.sub.2 40% 1496 32094 3907 146127 0.277 0.180 particles 50% 1570 36325 2554 94429 0.381 0.278 60% 1621 39555 1659 60032 0.494 0.397 75% 1715 47497 793 27087 0.684 0.637 90% 1805 55974 211 5873 0.896 0.905 100%  2009 78064 0 0 1 1

[0081] An approximate curve in FIG. 9A is a curve obtained by polynomial approximation using the least-square method and is expressed by the equation y=0.4755x.sup.2+0.5695x−0.0224 where x is the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 and y is the peak height ratio, and its coefficient of determination R.sup.2 is 0.998. An approximate curve in FIG. 9B is a curve obtained by polynomial approximation using the least-square method and is expressed by the equation y=0.9062x.sup.2+0.1546x−0.0153 where x is the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 and y is the integral intensity ratio, and its coefficient of determination R.sup.2 is 0.9951.

[0082] A value of the ratio of the peak height of the peak A2 to the total of the peak height of the peak A2 and the peak height of the peak B2 is read to be 0.381 from the Raman spectra in FIGS. 8A and 8B, hence, it can be determined from the graph in FIG. 9A that the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 is 50%. Meanwhile, a value of the ratio of the integral intensity of the peak A2 to the total of the integral intensity of the peak A2 and the integral intensity of the peak B2 is read to be 0.289 from the Raman spectra in FIGS. 8A and 8B, hence, it can be determined from the graph in FIG. 9B that the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 is 50%.

[0083] FIG. 10A is a graph showing a relationship between a value of a ratio of the peak height of the peak A2 to the total of the peak height of the peak A2 and the peak height of the peak B1 (a peak height ratio) and the mass fraction of the first TiO.sub.2 particles in TiO.sub.2 particles 11 obtained by measuring respective weights of the first TiO.sub.2 particles and the second 102 particles. FIG. 10B is a graph showing a relationship between a value of a ratio of the integral intensity of the peak A2 to the total of the integral intensity of the peak A2 and the integral intensity of the peak B1 (an integral intensity ratio) and the mass fraction of the first TiO.sub.2 particles in the 102 particles 11 obtained by measuring respective weights of the first TiO.sub.2 particles and the second TiO.sub.2 particles.

[0084] Table 2 below shows the peak height ratio and the integral intensity ratio for each mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 for each plotted point in FIGS. 10A and 1B, and the peak height and the integral intensity of each of the peak A2 and the peak B1 for each mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 which were used to calculate the ratios. The values of the peak height and the integral intensity of the peak B1 are not listed since the peak B1 at the mass fraction of the first TiO.sub.2 particles of 90% had very low intensity and could not be detected.

TABLE-US-00002 TABLE 2 Peak A2 Peak B1 Peak Integral Peak Integral Peak Integral height intensity height intensity height intensity ratio ratio Mass  0% 0 0 9374 1398181 0 0 10% 422 2922 7593 601897 0.053 0.005 25% 1285 7890 2931 394369 0.836 0.598 40% 1496 32094 1225 146821 0.706 0.326 50% 1570 36325 655 74992 0.550 0.179 60% 1621 39555 318 26593 0.305 0.054 75% 1715 47497 67 1974 0.962 0.960 90% 1805 55974 — — — — 100%  2009 78064 0 0 1 1

[0085] An approximate curve in FIG. 10A is a curve obtained by polynomial approximation using the least-square method and is expressed by the equation y=−0.824x.sup.2+2.1293x−0.1612 where x is the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 and y is the peak height ratio, and its coefficient of determination R.sup.2 is 0.9986. An approximate curve in FIG. 10B is a curve obtained by polynomial approximation using the least-square method and is expressed by the equation y=2.49x.sup.2−0.6336x+0.0453 where x is the mass fraction of the first 1102 particles in the TiO.sub.2 particles 11 and y is the integral intensity ratio, and its coefficient of determination R.sup.2 is 0.9966.

[0086] A value of the ratio of the peak height of the peak A2 to the total of the peak height of the peak A2 and the peak height of the peak B1 is read to be 0.697 from the Raman spectra in FIGS. 8A and 8B, hence, it can be determined from the graph in FIG. 10A that the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 is 50%. Meanwhile, a value of the ratio of the integral intensity of the peak A2 to the total of the integral intensity of the peak A2 and the integral intensity of the peak B1 is read to be 0.351 from the Raman spectra in FIGS. 8A and 8B, hence, it can be determined from the graph in FIG. 10B that the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 is 50%.

[0087] FIG. 11A is a graph showing a relationship between a value of a ratio of the peak height of the peak A1 to the total of the peak height of the peak A1 and the peak height of the peak B2 (a peak height ratio) and the mass fraction of the first TiO.sub.2 particles in TiO.sub.2 particles 11 obtained by measuring respective weights of the first TiO.sub.2 particles and the second TiO.sub.2 particles. FIG. 11B is a graph showing a relationship between a value of a ratio of the integral intensity of the peak A1 to the total of the integral intensity of the peak A1 and the integral intensity of the peak B2 (an integral intensity ratio) and the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 obtained by measuring respective weights of the first TiO.sub.2 particles and the second TiO.sub.2 particles.

[0088] Table 3 below shows the peak height ratio and the integral intensity ratio for each mass fraction of the first 1102 particles in the TiO.sub.2 particles 11 for each plotted point in FIGS. 11A and 11B, and the peak height and the integral intensity of each of the peak A1 and the peak B2 for each mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 which were used to calculate the ratios.

TABLE-US-00003 TABLE 3 Peak A1 Peak B2 Peak Integral Peak Integral Peak Integral height intensity height intensity height intensity ratio ratio Mass  0% 0 0 23769 1644682 0 0 fraction 10% 5739 381582 22205 791024 0.205 0.325 of First 25% 3340 202606 7891 294511 0.297 0.408 TiO.sub.2 40% 2919 134064 3907 146127 0.428 0.478 particles 50% 2807 118323 2554 94429 0.524 0.556 60% 2739 109321 1659 60032 0.623 0.646 75% 2658 98738 793 27087 0.770 0.785 90% 2601 91001 211 5873 0.925 0.939 100%  2677 96047 0 0 1 1

[0089] An approximate curve in FIG. 11A is a curve obtained by polynomial approximation using the least-square method and is expressed by the equation y=−0.0442x.sup.2+1.0033x+0.0443 where x is the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 and y is the peak height ratio, and its coefficient of determination R.sup.2 is 0.993. An approximate curve in FIG. 11B is a curve obtained by polynomial approximation using the least-square method and is expressed by the equation y=−0.1573x.sup.2+1.0449x+0.1045 where x is the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 and y is the integral intensity ratio, and its coefficient of determination R.sup.2 is 0.9616.

[0090] A value of the ratio of the peak height of the peak A1 to the total of the peak height of the peak A1 and the peak height of the peak B2 is read to be 0.535 from the Raman spectra in FIGS. 8A and 8B, hence, it can be determined from the graph in FIG. 11A that the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 is 50%. Meanwhile, a value of the ratio of the integral intensity of the peak A1 to the total of the integral intensity of the peak A1 and the integral intensity of the peak B2 is read to be 0.588 from the Raman spectra in FIGS. 8A and 8B, hence, it can be determined from the graph in FIG. 11B that the mass fraction of the first TiO.sub.2 particles in the TiO.sub.2 particles 11 is 50%.

[0091] Raman spectra do not need to be measured over a wide wavenumber range as shown in FIGS. 8A and 8B, and measurement may be performed only in the wavenumber ranges around the first and second peaks which are used to determine the concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles.

[0092] (Summary of the Embodiments)

[0093] Technical ideas understood from the embodiments will be described below citing the reference signs, etc., used for the embodiments. However, each reference sign, etc., described below is not intended to limit the constituent elements in the claims to the members, etc., specifically described in the embodiments.

[0094] According to the feature [1], a resin composition quality controlling method includes: measuring a Raman spectrum of a resin composition 1 composed of first TiO.sub.2 particles comprising anatase type TiO.sub.2 and second TiO.sub.2 particles comprising rutile type TiO.sub.2 by irradiation with laser; and determining a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition 1 based on the intensity of a first peak assigned to lattice vibration in the anatase type TiO.sub.2 and the intensity of a second peak assigned to lattice vibration in the rutile type TiO.sub.2 in the Raman spectrum.

[0095] According to the feature [2], in the resin composition quality controlling method defined by the feature [1], the first peak comprises a peak exhibiting the highest intensity in a range of not less than 365 cm.sup.−1 and not more than 425 cm.sup.−1 or a peak exhibiting the highest intensity in a range of not less than 485 cm.sup.−1 and not more than 545 cm.sup.−1 in the Raman spectrum, and wherein the second peak includes a peak exhibiting the highest intensity in a range of not less than 205 cm.sup.−1 and not more than 265 cm.sup.−1 or a peak exhibiting the highest intensity in a range of not less than 415 cm.sup.−1 and not more than 475 cm.sup.−1 in the Raman spectrum.

[0096] According to the feature [3], in the resin composition quality controlling method defined by the feature [1] or [2], in the determining, a peak height ratio of the first peak to the second peak is obtained from the Raman spectrum, and a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition is determined by referring to a relationship obtained in advance between the peak height ratio and the concentration ratio.

[0097] According to the feature [4], in the resin composition quality controlling method defined by the feature [1] or [2], wherein in the determining, an integral intensity ratio of the first peak to the second peak is obtained from the Raman spectrum, and a concentration ratio of the first TiO.sub.2 particles to the second TiO.sub.2 particles in the resin composition is determined by referring to a relationship obtained in advance between the integral intensity ratio and the concentration ratio.

[0098] According to the feature [5], a cable and tube quality controlling method includes: determining the concentration ratio in an insulator being provided on a cable 20 or a tube 4 and including the resin composition 1 by the method for controlling the quality of the resin composition 1 defined by any one of the features [1] to [4].

[0099] According to the feature [6], a determination device is configured to perform the determining in the resin composition quality controlling method defined by any one of the features [1] to [4].

[0100] According to the feature [7], an inspection system 50 includes: a Raman measurement device 58 configured to perform the measuring in the resin composition quality controlling method defined by any one of the features [1] to [4]; and a determination device configured to perform the determining in the resin composition quality controlling method defined by any one of the features [1] to [4].

[0101] According to the feature [8], a cable 20 or a tube 4 includes: an insulator composed of the resin composition 1 including first TiO.sub.2 particles composed of anatase type TiO.sub.2 and second TiO.sub.2 particles composed of rutile type TiO.sub.2.

[0102] Although the embodiments and Example of the invention have been described, the invention according to claims is not to be limited to the embodiments and Example described above, and the various kinds of modifications can be implemented without departing from the gist of the invention. In addition, the invention according to claims is not to be limited to the above-mentioned embodiments and Example. Further, please note that not all combinations of the features described in the embodiments and Example are necessary to solve the problem of the invention.