Ferroelectric polymer material in the form of a single crystalline film or fibre

Abstract: A ferroelectric polymer single crystalline body consists of a copolymer of ethylene trifluoride and/or ethylene tetrafluoride and vinylidene fluoride, in the form of a film or a fiber and is used in a piezoelectric, pyroelectric or nonlinear optical element. The single crystalline body is produced by crystallizing a stretched film of the single crystalline body at hexagonal phase while maintaining the stretched film surface at a free state.

Description: This invention relates to a ferroelectric polymer material having a strong piezoelectricity and a mechanical toughness in form of a crystalline film or fiber and a method of producing the same and use in piezoelectric, pyroelectric or nonlinear optical elements. It is well-known that polyvinylidene fluoride (PVDF), copolymer [P(VDF-TrFE)] of vinylidene fluoride (VDF) and ethylene trifluoride (TrFE), and copolymer [P(VDF-TeFE)] of vinylidene fluoride and ethylene tetrafluoride (TeFE) exhibit strong piezoelectricity through poling treatment. These polymers are used in signal and energy converting elements of electric systems and mechanical systems including ultrasonic transducers as a piezoelectric material, or in heat and radiation detecting elements as a pyroelectric material. Particularly, when vinylidene fluoride-ethylene trifluoride copolymers P(VDF-TrFE) having an adequate mol ratio range of vinylidene fluoride (VDF) to ethylene trifluoride (TrFE) are crystallized by a heat treatment within a particular temperature range, they are materials having greatest electromechanical conversion efficiency among the existing known piezoelectric polymer materials. That is, the vinylidene fluoride-ethylene trifluoride copolymers P(VDF-TrFE) containing about 60-90 mol% of vinylidene fluoride (VDF) are crystallized by a heat treatment at a paraelectric phase (hexagonal phase) and subjected to poling to provide high-performance piezoelectric and pyroelectric materials. As to these materials, the following are known from various studies by Ohigashi et al (H. Ohigashi and K. Koga, Jpn. J. Appl. Phys., 21(1982), L455-L457; K. Koga and H. Ohigashi, J. Appl. Phys., 56(1986), 2142-2150; H. Ohigashi and T. Hattori, Jpn. J. Appl. Phys., 28(1989), L1612-L1615; K. Koga, N. Nakano and H. Ohigashi, J. Appl. Phys., 67(1990), 965-974; H. Ohigashi et al., J. Appl. Phys., 71(1) (1992), 506-508; and the like) up to the present. That is, the vinylidene fluoride-ethylene trifluoride copolymers P(VDF-TrFE) having the above composition are orthorhombic crystal at room temperature. However, stable paraelectric phase (hexagonal phase) appears at a higher temperature when the content of vinylidene fluoride (VDF) is not more than about 82 mol%, while when the VDF content is more than 82 mol% but not more than about 90 mol%, metastable paraelectric phase appears at a higher temperature except for a special case. In the paraelectric phase, a lamellar crystal of 0.1-1 µm in thickness having properties as an extended chain crystal considerably grows to attain a film crystallinity of not less than 90%. Furthermore, columnar or plate-shaped single crystals having a size of few µm are developed on the lamellar crystal as a substrate, though the number of these crystals is few. The piezoelectricity of the copolymer is created when molecular dipole is cooperatively (ferroelectrically) oriented in a direction nearest to a direction of an electric field among directions obtainable in the crystal if there is existent the electric field larger than the coercive field. Therefore, it is considered that the strong piezoelectricity results from the growth of thick lamellar crystal. As a heat treatment for the growth of the lamellar crystal, there has hitherto been used a method wherein isothermic crystallization is carried out by dropping down the copolymer from a molten state or raising from the orthorhombic phase into the hexagonal phase at a state that a stretched or unstretched film is closely contacted with a glass plate or a metal plate or the film is sandwiched between flat plates or curved rigid bodies. Such a heat treatment is effective to promote the growth of the lamellar crystal and to avoid the deformation of the film because the paraelectric phase is a liquid crystal state and the film becomes considerably flexible. However, the well grown film of the lamellar crystals has some drawbacks as mentioned below. Since the lamellar crystal is grown at a lamination state, the resulting film becomes brittle and is easily broken by bending or tensile stress (i.e. the lamellar crystals are separated by a small stress because a high polymer chain is not existent between the lamellar crystals). Furthermore, the lamellar crystal does not develop in a certain direction in the film during the growth of the lamellar crystal, so that the orientation distribution of molecular chain axis is considerably degraded from an ideal state. Moreover, the film becomes opaque owing to the presence of the lamellar crystal, so that it can not put into practical use though there is existent a secondary nonlinear optical effect. It is, therefore, an object of the invention to provide a transparent film or fiber of copolymer [P(VDF-TrFE)] of vinylidene fluoride and ethylene trifluoride or copolymer [P(VDF-TeFE)] of vinylidene fluoride and ethylene tetrafluoride having mechanical toughness and high piezoelectricity and pyroelectricity. In a first aspect the invention provides a ferroelectric polymer crystalline body consisting of a copolymer of ethylene trifluoride and/or ethylene tetrafluoride and vinylidene fluoride, in the form of a film or fiber, characterised in that the film or fiber consists of a single crystal. In a second aspect the invention provides a method of producing a ferroelectric polymer crystalline body, which comprises stretching a ferroelectric polymer film or fiber consisting of a copolymer of ethylene trifluoride and/or ethylene tetrafluoride and vinylidene fluoride and crystallizing the copolymer at a paraelectric or hexagonal phase thereof, characterised in that the crystallization is carried out while maintaining the stretched surface of the film or fiber substantially unrestrained, so that a body consisting of a single crystal results from the crystallization. Such a body is referred to below as a single crystalline body. The body is free of amorphous portions and lamellar crystals. During crystallization, the surface of the body is in an unrestrained or free state, i.e. the surface is substantially free of externally applied shearing stress or compressive stress. The ferroelectric polymer single crystalline bodies according to the invention can generally be used as a piezoelectric or pyroelectric material after the poling. That is, they can be used as an electromechanical converting element having a high conversion efficiency such as piezoelectric sensors, actuators and audio and ultrasonic transducers over a frequency range of from zero to high frequency (GHz) within a temperature range of from cryogenic temperature (mK) to Curie temperature or melting point (for example, melting point is lower than Curie point in P(VDF-TrFE) containing not less than 82 mol% of VDF). In this case, the above single crystalline body may include shearing deformation or stress in addition to stretching or compression as mechanical deformation or stress (e.g. matrix components in piezoelectric constant e of the single crystalline body are e 31 , e 32 , e 33 , e 15 and e 24 when selecting the 1-axis in the stretching direction and the 3-axis in the polarization direction, and all of them have industrially utilizable values). Furthermore, they can be used as a pyroelectric element within the above temperature range. Moreover, they can be used as a secondary nonlinear optical element such as light modulating element or second harmonic generation element. The invention will be described with reference to the accompanying drawings, wherein: Fig. 1 is a graph showing a relation between intensity and 2 in X-ray diffraction of a single crystalline film of Example 1 as measured by a symmetrical reflection process; and Fig. 2 is an X-ray diffraction pattern of a single crystalline film of Example 1 when an incidence of the X-ray is in parallel to a stretching direction of the film. DESCRIPTION OF THE PREFERRED EMBODIMENTS Heretofore, it has been considered that the crystal growing at the hexagonal phase (paraelectric phase) is a thick lamellar crystal having properties near to the extended chain crystal. In this connection, the inventors have made studies with respect to the crystallization course at this phase and confirmed that the hexagonal phase is not a satisfactory condition for growing the thick lamellar crystal and it is necessary to apply a mechanical restraint or stress to the film when the crystallization is conducted by raising the temperature from the orthorhombic phase to the hexagonal phase. That is, when the stretched film is crystallized at the hexagonal phase, the film is fixed to a support substrate or sandwiched between fastening plates and then heat-treated to attain the growth of the thick lamellar crystal in the film. Alternatively, the growth of the lamellar crystal is attained even if the crystallization is conducted by cooling from a molten state to the hexagonal phase. This is considered due to the fact that shearing stress or shearing strain produced by thermal contraction or expansion of the film is applied to a group of molecular chains being at a liquid crystal state at a temperature above a temperature region near to a transition point from orthorhombic phase to hexagonal phase (Curie point) to grow the lamellar crystal. Now, the inventors have made further studies with respect to the crystallization condition for obtaining a well double-oriented film of a copolymer [P(VDF-TrFE)] of vinylidene fluoride and ethylene trifluoride without the growth of lamellar crystal and found out the following point which is very important scientifically and technologically. That is, it has been found that a highly biaxial stretched film is obtained by crystallizing a double-oriented film of the copolymer P(VDF-TrFE) at the hexagonal phase (paraelectric phase) while maintaining a free surface without restraining the surface. Furthermore, it has been confirmed that the resulting double-oriented film is a single crystal as a result of analyzing the structure of the film through X-ray diffraction, electron ray diffraction and polarization microscope. In the film before the poling, c-axis of the crystal (crystallographic axis [001] in a direction of molecular chain) is parallel with the stretching axis and the direction of crystallographic axis [100] or [110] meets with a normal direction of the film surface, while the direction of crystallographic axis [110] in the film after the poling meets with the normal direction. Moreover, there is a possibility that a ferroelectric domain is existent in the single crystal as mentioned in the following Example 1 and there may be distribution of molecular chain distance in the single crystal. In the invention, therefore, the single crystal may be a crystal having a domain structure or a crystal having a disturbed arrangement of twin and molecular chain. According to the invention, it is possible to produce fibrous single crystal. That is, the fibrous single crystal having a c-axis parallel to an axis of fiber can be obtained by promoting the crystallization of uniaxial stretched fiber of the copolymer P(VDF-TrFE) at the hexagonal phase while maintaining the side surface of the fiber at a free state. Crystallization of the film or fiber while maintaining an unrestrained or free surface state means the crystallization at the hexagonal phase, without sandwiching the film or fiber between fastening plates, at a state that shearing stress or excessive compression stress is not applied to the surface of the film or fiber from exterior. Both ends of the film in the c-axis direction may be fixed or may not be fixed, but it is favorable that both ends of the film are fixed or a certain tension is applied to the film in order to obtain anon-bent uniform film. Furthermore, in order to obtain anon-disturbed single crystal, it is preferable that the stretched film is preliminarily subjected to a heat treatment at a temperature lower than the transition point from orthorhombic phase to hexagonal phase prior to the crystallization at hexagonal phase. Ideally, the crystallization is carried out under vacuum, or in a gas or a liquid. However, the crystallization may be carried out by placing the film or fiber of the copolymer P(VDF-TrFE) at paraelectric phase on a tack-free material such as polyethylene tetrafluoride (Teflon, trade name) or the like. Although the mechanism of forming the single crystal according to the invention is not yet clear, the following are considered from knowledge elucidated up to the present. That is, the polymer film according to the invention at a state of the hexagonal phase possesses liquid properties in a direction of molecular chain and solid properties in a direction perpendicular to the molecular chain, so that the molecular chain can easily move in the stretching direction but the perpendicular movement is difficult as much as shearing stress is not applied to the molecular chain from the exterior. On the other hand, the perpendicular movement of the molecular chain is required for the growth of the lamellar crystal and also the surface energy of the lamellar crystal becomes high owing to the folding of the molecule. In the uniaxially oriented molecular chain aggregate having a free surface not applied by shearing strain, therefore, it is considered that a system of forming the single crystalline film by the sliding in the direction of the molecular chain and the slight movement in perpendicular direction becomes lower in the free energy than a system of forming the lamellar crystal at the hexagonal phase. In the single crystalline film, it is considered that the arrangement of making the zigzag plane of the molecular chain parallel to the film surface is lowest in the energy at the free surface and the single crystalline film having (100) plane parallel to the film surface is formed by crystallizing the molecular chains in the film surface under the condition of such an arrangement. As the copolymer capable of forming the single crystalline film according to the method of the invention, there are a copolymer P(VDF-TrFE) of vinylidene fluoride and ethylene trifluoride (preferably containing about 60-90 mol% of vinylidene fluoride) and a copolymer P(VDF-TeFE) of vinylidene fluoride and ethylene tetrafluoride (preferably containing 70-90 mol% of vinylidene fluoride). Furthermore, a terpolymer of vinylidene fluoride, ethylene trifluoride and ethylene tetrafluoride exhibiting a hexagonal phase at a high temperature may be used. Even if a copolymer has a composition not developing the hexagonal phase at atmospheric pressure among the above copolymers, the hexagonal phase appears at a higher pressure, so that the method according to the invention is applicable to a copolymer P(VDF-TrFE) containing not less than 90 mol% of polyvinylidene fluoride (PVDF) and a stretched film of PVDF in the crystallization under a high pressure. The single crystal according to the invention is generally poled by the conventionally known method. For example, static voltage or alternating voltage is applied to the single crystalline film after electrodes are deposited onto the film or contacted with the film. Furthermore, the poling may be carried out by corona discharge. A hysteresis curve between electric displacement (D) and field intensity (E) in the single crystalline film indicates more conspicuous characteristics of ferroelectric crystal as compared with that of the lamellar crystal film because the polarization reversal at coercive field is more steep. The following examples are given in illustration of the invention and are not intended as limitations thereof. Example 1 A film of a copolymer P(VDF-TrFE) of vinylidene fluoride (VDF) and ethylene trifluoride (TrFE) formed in dimethylformamide as a solvent having a molar fraction of VDF/TrFE of 75/25 and a molecular weight of about 200,000 is uniaxially stretched about 5 times at room temperature. The uniaxial stretched film has a Curie point of 123°C and a melting point of 150°C. After both ends of the stretched film (thickness: 70 µm) are fixed in a direction perpendicular to the stretching direction, the temperature is raised at a heating rate of about 5°C/min from room temperature to 140°C, crystallized at this temperature (hexagonal phase) in air for 2 hours, and then slowly cooled to room temperature. The thus obtained crystallized film is transparent and apparently uniform. Furthermore, this film has a homogeneous structure without lamellar crystal as a result of observation by means of a polarization microscope, in which the orientation is uniform over the whole of the film. According to X-ray diffraction, a strong reflection (d=4.40 Å) from the (110) plane or (200) plane is observed in the film as shown in Fig. 1. Since reflection of (400) plane or (220) plane is weak, disorder in lattice spacing inherent to the copolymer itself is existent, but the presence of amorphous portion is not observed. When incident X-ray is parallel to the stretching axis, 6 strong diffraction points are observed in a diffraction pattern shown in Fig. 2, from which it is clear that (110) plane or (200) plane is parallel to the film surface over the full region of the film. Moreover, there is a large possibility that both faces form a ferroelectric domain structure at an unpiling state. After the poling, (110) plane is parallel to the film surface. From the above results, it is apparent that the film may be a single crystal as a whole. Moreover, even if the crystallization is carried out at 130°C, the resulting film is a single crystal. Even when the stretched film having a thickness of 8 µm is crystallized, a single crystal is obtained. Fig. 1 shows a relation between intensity and 2 in the X-ray diffraction of the single crystalline film obtained in Example 1 as measured by symmetrical reflection process. In this case,  is the angle between the film surface and an incident (or reflective) X-ray. The stretching axis or c-axis of the crystal is perpendicular to incident and reflective faces of X-ray. Fig. 2 is an X-ray diffraction pattern of the single crystalline film of Example 1 when the incident X-ray is parallel to the stretching direction of the film. In this case, the film surface is arranged in up and down directions of the figure. Example 2 A film of a copolymer P(VDF-TrFE) of vinylidene fluoride and ethylene trifluoride prepared in a DMF solution is uniaxially stretched about 5.5 times to obtain a stretched copolymer film having a thickness of 50 µm. This film is placed on a Teflon sheet without fixing both ends and heated in an oven at a rate of 4°C/min from 80°C to 135°C and held at this temperature for 2 hours to conduct the crystallization. After the cooling, the film is sandwiched between two plates and reheated to 120°C for removing flexing of the film produced in the above heat treatment. The thus obtained film is a single crystal likewise Example 1. After a metal of Al is deposited on both surfaces of the film, poling is carried out by repeating polarization reversal at room temperature. The piezoelectricity of the thus poled film is measured by a piezoelectric resonance method to obtain results as shown in Table 1. The value of electromechanical coupling factor k t 33 for piezoelectric effect for thickness extensional vibration mode is larger than those of the conventionally known piezoelectric polymers. The longitudinal wave acoustic velocity propagating in the direction of molecular chain (stretching direction) is considerably large reflecting the single crystal of the film. Piezoelectricity of single crystalline film of P(VDF-TrFE) (75/25) (25°C) Longitudinal wave acoustic velocity V 11 2950 m/s V 22 1838 m/s V 33 2180 m/s Lateral wave acoustic velocity V 44 1150 m/s V 55 1035 m/s Electromechanical coupling factor k t 33 0.31 k 31 0.10 k 32 0.18 k 15 0.16 k 24 0.20 As seen from the above, the single crystalline film according to the invention is considerably ideal in the orientation of molecular chain and the crystallinity as compared with the film aggregated from lamellar crystals according to the conventional method. Therefore, the poled film according to the invention indicates a larger polarization as compared with that of the conventional film and possesses large piezoelectric constant and electromechanical coupling factor. Furthermore, Young's moduli are large and dynamic loss factors are small, while tensile strength in the stretching direction and bending modulus are large. Moreover, the single crystalline film or fiber according to the invention maintains flexibility even at a lower temperature and is tough, while the lamellar crystal film is brittle at a low temperature (e.g. liquid nitrogen temperature) and is easily broken. And also, the film or fiber according to the invention is optically uniform and excellent in the light permeability. The single crystal according to the invention is obtained in form of a film or fiber, so that it can be made at various forms in accordance with the use purpose. Moreover, since the film is apt to broken in a direction parallel to the molecular chain, it is effective to prevent such a problem by laminating and adhering plural films without matching the stretching directions of these films with each other.

Claims: A ferroelectric polymer crystalline body consisting of a copolymer of ethylene trifluoride and/or ethylene tetrafluoride and vinylidene fluoride, in the form of a film or fiber, characterised in that the film or fiber consists of a single crystal. A body as claimed in claim 1, wherein the film or fiber is flexible at liquid nitrogen temperature. A method of producing a ferroelectric polymer crystalline body, which comprises stretching a ferroelectric polymer film or fiber consisting of a copolymer of ethylene trifluoride and/or ethylene tetrafluoride and vinylidene fluoride and crystallizing the copolymer at a paraelectric or hexagonal phase thereof, characterised in that the crystallization is carried out while maintaining the stretched surface of the film or fiber substantially unrestrained, so that a body consisting of a single crystal results from the crystallization. A method as claimed in claim 3, wherein the crystallization is carried out under vacuum or in a gas or a liquid. A method as claimed in claim 3 or 4, wherein the crystallization is carried out on a tack-free material. A method as claimed in any of claims 3 to 5, wherein prior to the crystallization, the stretched film is preliminarily subjected to a heat treatment at a temperature lower than a transition point from orthorhombic phase to hexagonal phase. A method as claimed in claim 3, comprising the sequential steps of: (a) stretching the ferroelectric polymer film or fiber at ambient temperature; (b) fixing opposite ends of the stretched film or fiber; (c) heating the film or fiber from ambient temperature to a temperature corresponding to a paraelectric phase of the polymer while maintaining the surface of the film or fiber substantially unrestrained; (d) crystallizing the film or fiber by maintaining the said temperature; and (e) slowly cooling the crystallized film or fiber to ambient temperature. A method as claimed in claim 3, comprising the sequential steps of: (a) stretching the ferroelectric polymer film or fiber at ambient temperature; (b) placing the stretched film or fiber on a sheet of tack-free material; (c) heating the film or fiber from ambient temperature to a temperature corresponding to a paraelectric phase of the polymer while maintaining the surface of the film or fiber substantially unrestrained; (d) crystallizing the film or fiber by maintaining the said temperature; and (e) slowly cooling the crystallized film or fiber to ambient temperature. A method as claimed in claim 8, further comprising the steps of: (f) sandwiching the crystallized film or fiber between two plates; and (g) heating the film to below the Curie point to remove flexing of the film or fiber caused by step (c). A piezoelectric, pyroelectric or nonlinear optical element comprising a ferroelectric polymer crystalline body according to claim 1, subjected to poling.

Inventors: GOMYO TERUHISA, OHIGASHI HIROJI, OMOTE KENJI, GOMYO, TERUHISA, OHIGASHI, HIROJI, OMOTE, KENJI
Applicants: UNIV YAMAGATA, YAMAGATA UNIVERSITY
Application year: 1995
Main classification: C08J5
IPC codes: B29C55, C08J5, H01L37, H01B3, H01L41, H01F1, D01F6, B29K27, C08L27