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    • 专利摘要:
    The invention relates to a four-point bending mechanical test device of a specimen and to a method of using such a device. This device comprises: a) means for holding a first end of the test piece (27; 127; 28; 128) and means for holding a second end of the test piece (30, 31); b) traction means (25) and transformation means (16, 116) for converting a translation movement of said traction means into a rotational movement; c) converting means (26; 27; 126; 127) for converting said rotational movement into bending deformation of the specimen, said converting means including at least one first universal joint (26; 126) connected thereto; the means for holding the first end of the test piece.
    公开号:FR3023373A1
    申请号:FR1456479
    申请日:2014-07-04
    公开日:2016-01-08
    发明作者:Nathanael Connesson；Yohan Payan；Gabriel Antehrieu；Denis Favier
    申请人:Universite Joseph Fourier (Grenoble 1)；
    IPC主号:
    专利说明:

    [0001] TECHNICAL FIELD The invention relates to a mechanical test device in pure bending, also called circular bending, and a test method using such a device. The term pure bending is a term used in materials science and pure bending tests are widely used in experimental mechanics. The theory describing them theoretically is well established. These tests are the subject of numerous analytical and numerical studies. Pure bending tests induce a stress gradient in the thickness of the stressed specimens (ranging from tensile to local compression) while the bending moment applied is homogeneous along the specimen. In practice, during the bending test of a specimen, the specimen is subjected to stray forces in shear and torsion. However, it is possible to speak of 'pure bending' when the moments induced by these parasitic forces are rendered negligible in view of the bending moment to which the test piece is subjected. STATE OF THE PRIOR ART In order to be able to compare the experimental data with the theoretical / numerical results, it is essential to control the stress to which the sample is subjected. For this reason, particular care must be taken during the experiments, to ensure that the entire area of interest of the sample is well solicited in pure bending during the tests. Indeed, if parasitic forces are induced by the device (torsion, shear forces), the bending moment will not be homogeneous along the useful zone of the specimen. The lack of knowledge of the exact local demand to which the sample is subjected makes the results unusable. In practice, it is very difficult to perfectly stress a specimen in pure bending. Many precautions must be taken. It will be considered here that the specimen is solicited in pure bending when the parasitic forces are negligible and do not hinder the exploitation of the experimental results. Various pure bending devices have been described in the scientific literature and in patents. In certain "four-point" bending devices of the prior art, a test piece (also called sample) is arranged in suspension between two points of a fixed support. Two point supports of a moving part are brought into contact with the specimen between the two points of the fixed support and forces are applied on the specimen. The test piece is then deformed in pure bending between the two point supports. However, in these devices, a maximum displacement threshold in pure bending of the center of the sample is less than its thickness or the order of magnitude thereof. Bending causing displacement of the center of the sample above this threshold would cause the sample to slip at the support and distort the current measurements. When studying the mechanical properties of slender samples, a displacement of the center of the sample of this order of magnitude does not make it possible to solicit the samples in a sufficient deformation range: a system allowing large displacements is necessary to reach high deformations. These measurements are of prime interest for slender samples or made of superelastic materials, or when their manufacturing process does not allow to obtain other geometries. In the context of the present application, a slender sample (also called slender specimen) must be understood as being a sample whose length / diameter ratio is greater than or equal to 5, preferably but not exclusively, between 5 and 20, for example 8, 10 or 12.
    [0002] Some other bending devices, for example those described below, implement a "four-point" bending process in which a test specimen to be tested is held between two rotatably controlled supports. However, these devices allow to solicit part of the sample in pure bending only for small displacements and none seems able to achieve small radii of curvature. Typically, these devices can achieve radii of curvatures of the order of 10 cm. Characterization in pure bending of slender samples requires the ability to reach small radii of curvature. Such a suitability is not required for stocky test pieces, that is to say for example having a length / diameter ratio of less than 5, or when the test does not require high deformations: Bending test, for a fixed radius of curvature, the greater the characteristic diameter of the sample, the greater the maximum deformation experienced by the material, typically on the outer surface. Thus, to achieve the same state of deformation on a small sample, the required radius of curvature is much lower. Some publications or patented devices make it possible to study samples of reduced size. In the scientific literature, Kyriakides et al (Localization in NiTi tubes under pure bending, N. Bechle, JS Kyriakides, International journal of solids and structures, 2014, Vol 51, pp 967-980) presents results on tubes 3 mm in diameter. This bending device, however, has several limitations. The rotational actuators are fixed: the length of stressed material increases during a bending test. The sample slides in ball sleeves, which induces friction forces in the axis of the sleeves. This kinematics, associated with the resistance to movement, varies the bending moment along the specimen. This variation of the moment along the specimen changes during the test: the friction has little impact for a test-tube that is slightly deformed, that is to say almost rectilinear, but can induce wide variations in the moment of the test. bending along the specimen as the shape of the deformed specimen approaches a semicircle. This device does not allow to obtain a pure bending moment. This phenomenon will particularly impact measurements for small radii of curvature. In addition, the attainable radii of curvature are too great for samples of diameter of the order of 1 mm or less. The device described in Hoefnagels et al (A miniaturized contactless pure-bending device for in-situ SEM failure analysis, J.P.M Hoefnagels, C.A.
    [0003] Buizer, M.G.D Geers, Experimental and Applied Mechanics, 2011, Vol. 6, pp 587-596) theoretically makes it possible to solicit the sample in pure bending: the device imposes on the sample a kinematics of its ends corresponding to that of a pure bending under the assumption of a homogeneous mechanical behavior along the specimen. The major limitation of this device lies in the assumptions required to define the kinematics of the system. Indeed, if the mechanical properties of the sample are heterogeneous, a case frequently encountered experimentally, the kinematics imposed by the mechanism will not induce a pure bending along the sample. The forces, the state of deformation and the state of local stress in the material will then be unknown and the experimental results can not be analyzed correctly. The device described in document FR2843633 fulfills the conditions for soliciting two specimens in pure bending. Engines that urge both specimens are supported by various means, so that they can move freely in space. This freedom of movement allows them to avoid the appearance of parasitic forces, which ensures a state of homogeneous stress in the samples solicited. However, there are several limitations imposed by this system. Firstly, in the configuration where the motors are suspended by cables so that the forces due to the movements of the motors are zero, the length of the cables must be theoretically infinite and the cables must be insensitive to the movements of the ambient air. This therefore makes the device relatively bulky, not transportable, and poorly adapted to a low ceiling room. In general, this device is difficult to adapt to a conventional test machine. In addition, it is primarily intended for flat geometry samples such as plates and requires simultaneously soliciting two strictly identical samples (geometry, homogeneity of material between the two samples, etc.). These constraints are difficult to obtain experimentally. The invention therefore aims to provide an improved mechanical device for soliciting a sample, preferably slender, or a specimen, preferably slender, bending.
    [0004] Advantageously, such a device is simple and inexpensive.
    [0005] DISCLOSURE OF THE INVENTION Thus, the invention relates to a mechanical test device in bending at four points of a test piece, this device comprising: a) means for holding a first end of a test piece and means for maintaining a second end of the test piece; b) traction means and transformation means for converting a translation movement of said traction means into a rotational movement; c) converting means for converting said rotational movement into flexural deformation of the specimen, said converting means comprising at least a first universal joint, connected to the holding means of the first end of the specimen. During the bending deformation of a specimen, the use of a universal joint combined with the conversion means makes it possible to compensate for the spurious stray forces appearing in the specimen by a free and large displacement of the end of the specimen. a test tube. This displacement takes place until the disappearance of the effort giving rise to it. When the mechanical equilibrium is reached the parasitic forces in torsion and shear in the test tube are negligible. It is thus possible to test specimens in pure bending over a range of particularly large radii of curvature, from a linear geometry to very small radii of curvature, less than 1 cm, without the deformation of the specimen being hampered by the components of the device. The invention is furthermore usable on filiform samples having a diameter equal to or less than 1 mm, for example between 0.1 mm and 1 mm.
    [0006] During a bending test using the device according to the invention, the tested length of a test piece is constant and is subjected to a pure bending moment (homogeneous) over its entire length. Pure bending is used if the shear and torsional stresses to which the test piece is subjected induce moments and gradients of negligible moments for the measurements (and therefore that the moment is homogeneous over the entire length of the test piece). This allows a uniform deformation of the specimen, that is to say in a circular arc in the elastic domain of the specimen material if the material is homogeneous. In particular, uniform deformation can be qualified if the following assumptions are respected: pure and homogeneous moment, constant section, homogeneous material.
    [0007] Whatever the behavior of the specimen and its heterogeneity of materials, the margin of error is particularly small in the measurement of the bending moment applied to it, of the order of 10 -4 Nm for a device implemented. at the plaintiff's. The use of a universal joint makes it possible to obtain a particularly simple structure, inexpensive and having a reduced number of components compared to the existing one. In addition, this structure has the advantage of being usable with a conventional traction machine. Advantageously, the conversion means comprise a second universal joint. This second universal joint may itself include a bearing, for example ball. This bearing may be common to the means for holding a first end of a test piece and to the conversion means.
    [0008] Alternatively or cumulatively, the second universal joint may comprise other low-friction pivot connection members which are common to the means for holding a first end of the test piece and to the conversion means, such as spiked connections. metal on sapphire, or needle links pivotally mounted in respective bores.
    [0009] The second universal joint forms a low-friction joint and further minimizes the impact of parasitic forces. Alternatively, the first cardan joint is connected to the holding means of a first end of the test piece, the means for holding a first end of the test piece comprising at least one member provided with a bore intended to receive a end of a specimen. The member concerned is located behind the first universal joint in the drive train connecting the actuator wire to the test piece, starting from the actuator wire. This is for example an arm fixed on a hoop of the first universal joint. This structure is particularly advantageous in terms of costs.
    [0010] The sets of connections between the specimen and the perimeter of the bore advantageously replace the second universal joint. The friction between the specimen and the perimeter of the borehole is quite negligible for the measurement of the bending moment. The transformation means may comprise a wheel, the first universal joint connecting the wheel and the means for holding a first end of the specimen. In a particular embodiment, the first universal joint is connected to at least one structure, for example comprising an arm, which passes through the transformation means. This structure may further comprise balancing means so that the weight of the device does not weigh on the biased sample, for example carry a balancing mass. This structure may also comprise two branches arranged in fork, the transformation means comprising a wheel, the wheel being provided with two through openings, each branch passing through a respective one of the two openings and being connectable to the first universal joint. The above device may further comprise measuring means for measuring a force exerted on the traction means or measuring means for measuring a torsional force on a downstream member to which the first universal joint is connected. The invention also relates to a mechanical flexural test system, comprising a traction machine and a mechanical flexural test device as described above, the traction machine comprising a traction mechanism connected to the traction means of the device. test, the mechanism being configured to apply a traction force on these traction means. The invention also relates to a method of mechanical test in bending of a specimen using a mechanical test device as described above, comprising the steps of: - setting up a first end of the test piece in the means for holding a first end of a test piece, and a second end of the test piece in the means for holding a second end of the test piece; - application of a tension on the traction means; determination of the bending moment by measuring means for measuring a force exerted on the traction means or by measuring means for measuring a torsional force on a downstream member to which the first universal joint is connected.
    [0011] Advantageously, the introduction of the specimen comprises the following steps: - clamping a first ring on a first end of the specimen against the holding means of the first end of a specimen; tightening a second ring on a second end of the test piece against the means for holding the second end of the test piece; the first and second rings being tightened on the respective ends of the test piece outside the zone between the holding means of the first and the second end of the test piece. A device or a method according to the invention is advantageously applied to a slender sample whose length / diameter ratio is greater than or equal to 5, for example between 5 and 20. A device or a method according to the invention makes it possible to obtain a large deformation, of the test piece, of at least a few%, for example at least 3% or at least 5%, this being a function of the nature of the material. For example, a deformation of 5% of a steel test piece is large, a deformation of between 10% and 15% for NiTi is also large.
    [0012] BRIEF DESCRIPTION OF THE DRAWINGS The invention will be better understood on reading the detailed description which follows, non-limiting examples of implementation thereof, as well as the examination of the appended figures, diagrammatic and partial. , in which: - Figure la is a side view of a portion of a test device according to the invention; FIG. 1b is a front view of the device of FIG. 1a showing a specimen in a particular bent state during a test; - Figure 2a is a side view of a variant of the device of Figure la; - Figure 2b is a partial front view of the device of Figure 2a showing a test piece at rest, here rectilinear, housed in the device; FIG. 2c is a front view of the device of FIG. 2a showing a bending test specimen; - Figures 3a and 3b are side and front views of another variant of the device of Figure 1, Figure 3b showing a test piece at rest, here rectilinear, housed in the device; FIG. 4 is a measurement record taken during a bending test for two steel wires of different diameters; FIGS. 5a and 5b are photographs of specimens deformed in flexion in the device of FIGS. 2a to 2c; FIG. 6 is a diagram of a universal joint implemented in the variant of the device illustrated in FIGS. 3a and 3b; FIG. 7 is a side view of another variant of the device of FIG. FIG. 8 is a schematic and enlarged representation of the local deformation of a specimen deformed in pure bending.
    [0013] DETAILED DESCRIPTION OF PARTICULAR EMBODIMENTS A four-point bending test device 10 is illustrated in FIGS. 1a and 1b. The device 10 here comprises a frame 20, a pulley 16 or pulley system, an actuator wire 25, two cardan joints 26 and 27, a shaft 28 (or arm) which connects the two cardan joints 26 and 27, and a support 30 (Figure 1b). A specimen 15, also called sample, whose flexural properties are to be measured, is also illustrated at rest in FIG. 3b or in flexion in FIG. The test piece 15 may be for example a wire or a tube whose diameter is less than 1 mm, for example metallic but not exclusively. The test piece 15 may be a slender test piece whose length / diameter ratio is, for example, greater than or equal to 5, preferably but not limited to between 5 and 20, for example equal to or of the order of 8. , or 10 or 12. As will be seen later with reference to Figure lb, when the specimen 15 is in flexion, the specimen 15 is in four-point contact with the device 10, namely the points 32a, 32b , 274a and 274b in the embodiment shown in FIG. The frame 20 comprises a bearing 21, here a ball bearing, delimiting an orifice 22. Similarly, the support 30 comprises a bearing 31, here a ball bearing, defining an orifice 32. The frame 20 and the support 30 may be either directly attached to each other, that is to say manufactured from the same block, or fixed to one another, or both fixed to a frame stationary of an external testing machine such as a traction machine. The frame 20 and the support 30 serve for example fixed reference during the bending tests.
    [0014] The pulley 16 here comprises a shaft 23 (or arm) and a wheel 24. The wheel 24 is fixed on the shaft 23 and integral in rotation thereof. The actuator wire 25 is wound in a central groove 241 that comprises the wheel 24. The central groove 241 preferably has a flat bottom so that the actuator wire does not slip in the groove 241, the wire does not overlap itself. same, and that the distance between the center of rotation of the pulley and the wire remains constant regardless of the angular position. Sliding or overlapping the wire on itself, such as contact of the actuator wire with itself, could cause friction and measurement errors. The term actuator wire may refer to a wire itself or a cable in the case of a device of larger size. The shaft 23 is housed in the orifice 22 and fixed on the inner race of the bearing 21. The shaft 23 and the wheel 24 are therefore rotatable relative to the frame 20. The actuator wire 25 is for example fixed by a first end to a pulling mechanism of an external traction machine not shown. This wire 25 is used to convert a translation movement, here provided by the traction machine, into a rotational movement of the wheel 24 and the shaft 23. The other end of the actuator wire 25 may for example be left free. or be attached to a movable part for the translation of the wire 25 of the traction mechanism.
    [0015] A first three-dimensional reference Oxyz is defined fixed relative to the frame 20 (Figure la), the z-axis coinciding with the longitudinal orientation of the shaft 23 and the x and y axes being transverse to each other and to the z axis. A second three-dimensional reference Ooxoyozo is defined fixed relative to the shaft 28 (Figure la), the axis zo coinciding with the longitudinal orientation of the shaft 23 and the axes xo and yo being transverse to each other and to the axis zo. The axis z also coincides with the axis zo of the arm 28 when it is in the position illustrated in FIG. 1a, while the x and y axes are parallel to xo and yo, respectively. It should be understood that the orientation of the various components of the device 10 may vary during a bending test and no longer coincide with the axes of the Oxyz mark. The first universal joint 26 is here of the cross type. The seal 26 shown comprises two arches 261 and 263 (that is to say two U-shaped pieces) and a spider 262. The spider 262 has two branches 262a and 262b transverse to each other and joined in their medium. In the position of the shaft 28 illustrated in FIG. 1a, the branch 262a is oriented along the x axis and the branch 262b is oriented along the y axis. The spider 262 is mounted in pivot connection with the arches 261 and 263 respectively by its branches 262a and 262b. Thus, in the Oxyz mark, the shaft 23 is rotatable about the x and y axes. The universal joint 26 allows the transmission of a torsional torque between the one and the other of the shafts 23 and 28, including when these are inclined or arranged at an angle relative to each other , and efforts along the x, y and z axes. A rotational movement of the shaft 28 about its axis will be transmitted to the shaft 23, that is to say a torque applied to the shaft 28 will be transmitted to the shaft 23. Conversely, a movement The three forces transmitted along the x, y and z axes are canceled by the positions taken by the other links of the system, namely here the universal joint 27 and the Pivot connection 32. Alternatively and without limitation, the universal joint 26 can be replaced by a cardan joint of another type such as the universal joint 27 bearing or the ring universal joint 126 described below or cardan joints having other types of low-friction pivot links such as metal spikes on or in sapphires (in English lewel bearing '). The second universal joint 27 here comprises a hoop 271, two pivot pins 272 and a ball bearing 273 having an inner race 273a and an outer race 273b. The pivot pins 272, stuck on either side in the outer race of the bearing 273, connect it in pivot connection to the hoop 271. The pivot axes 272 are here oriented along the x-axis in the position illustrated in FIG. figure the. The inner race 273a of the ball bearing 273 delimits a receiving orifice 274 sized to receive the end of a test piece 15 whose flexural properties are to be tested. The arch 261 is for example fixed to the shaft 23 or manufactured in one piece with the shaft 23. The hoop 263 of the universal joint 26 and the hoop 271 of the universal joint 27 are for example attached to the arm 28 which connects or manufactured one or the other or both, a room with the arm 28. In the Oxyz mark, the outer track 273b is rotatable about an axis coincident with the axis x in the position shown in figure la. The inner track 273a offers an additional degree of freedom in rotation along its own longitudinal axis, here transverse to the x-axis. When a specimen 15 is housed in the receiving orifice 274, the universal joint 27 allows the transformation of the torsional torque to which the shaft 28 is subjected by traction on the actuator wire 25, at a bending moment on the test piece 15 via two bearing points, such as the points 274a and 274b described below, the shaft 28 and the test piece 15 being inclined or arranged at an angle relative to each other . A rotational movement of the shaft 28 around the axis of the specimen 15, and a torque applied to the shaft 28 around this axis, will be transmitted to the test piece 15. Conversely, a rotational movement of the specimen 15 will be transmitted to the shaft 28. To test the bending properties of the specimen 15, this specimen 15 is placed in the attachment points formed by the orifice 32 and the orifice 274, here by inserting its ends into the attachment points (see Figure lb). At rest, the specimen 15 being rotatable in the bearing 31 relative to the frame 30, the shearing forces along the axis zo potentially transmitted by the arm 28 result in a rotation of the plane of flexion of the specimen. This rotation of the bending plane of the specimen is carried out until the position of the system and the specimen 15 allows this shear force following zo to cancel. When the specimen is rectilinear, the shearing forces are assumed to be zero during assembly of the specimen 15 by fine adjustment of the position of the frame 30 and the functional clearances between the specimen 15 and the bearings 31 and 273. The radius initial curvature of the specimen 15 is irrelevant as will be explained below with reference to the trace 301. A voltage, for example vertical, is applied to the actuator wire 25. The rotational movement of the wheel 24 induced by the translation movement of the actuator wire 25 is transmitted via the cardan joints 26 and 27 to the test piece 15. The test piece 15 then moves until it comes into contact at four points with the device 10: on the one hand the points 274a and 274b located respectively on a first annular edge 273a1 and on a second annular edge 273a2 of the track 273a, diagonally opposite on either side of the orifice 273; on the other hand the points 32a and 32b situated respectively on a first annular edge 31a1 and on a second annular edge 31a2 of the inner race 31a of the bearing 31, diagonally opposite on either side of the orifice 32 (see points 32a , 32b, 274a, 274b in FIG. 1b). These points of contact remain and transmit forces to the test piece resulting in a "four-point" flexion. The shear or twisting forces parasitic on the test piece are made negligible by the different members of the test device 10. The spurious shearing forces must be understood as inducing different moments of the moment in pure bending, for example the moments in torsion or shear forces. In the device 10, the parasitic forces appearing in the specimen 15 during a bending test result in a rotation of the bearing 31, the universal joint 27 - whose bearing 273 - and the universal joint 26 ( figure lb). In other words, the cardan joints 26 and 27 make it possible to render negligible in the specimen 15 at the same time the parasitic forces in shear transversely to the arm 28, that is to say along the transverse xo and yo axes. arm 28, as shown in Figure la, and torsional moments. The bearings 273 and 31 make it possible to minimize and render negligible in the specimen 15 the forces along the longitudinal axis zo of the arm 28 and the torsional moments in torsion. For reasons of readability, only the wheel 24, the wire 25, the universal joint 27 and the support 30 are illustrated in front view in FIG. Thanks to the degrees of freedom allowed by the cardan joints 26 and 27 and the bearing 31, the test piece 15 is subjected to a so-called pure bending moment. The test piece 15, in the case of a homogeneous material, is thus deformed in a perfect circular arc between the attachment points formed by the bearings 273 and 31 (see median lines 303 of the test pieces 15 represented in FIGS. 5a and 5b. with reference to variant 11 detailed below). This bending moment applied to the test piece 15 is then known by measuring the tension force of the actuator wire 25, for example by means of a measuring cell that comprises the traction machine. An alternative solution for knowing the bending moment is to use directly a device for measuring the torsional deformation of the arm 28.
    [0016] In fact, low friction, negligible, appear in the universal joints 26 and 27. A significant length L between the universal joints 26 and 27, here between the branch of the spider 262 and the axis 272 on which the arm 28 is mounted, further minimizes the impact of friction in the universal joints 26 and 27 on the measurements. The maximum deformation Emax at the surface of the test piece corresponds to the following equation: Emax = Rmax * (a6 / as) = Rmax * [(1 / Rc) - (1 / Ro)], in which the Emax deformation can be for example expressed as a percentage, and Rmax is the radius of the specimen, at 0 / ss or (1 / Rc) - (1 / Ro) are the variation in radius of curvature between the undistorted state and the deformed state, where 0 is the local variation of angle between two sections of the specimen spaced by a distance as, Rc is the radius of curvature reached during the maximum deformation, Ro is the initial radius of curvature (see Figure 8 on which 400 is the center line of a specimen 15 in the plane of flexion, 401 is the inner line, deformed in compression, and 402 is the outer line, deformed in tension). In the present application, the term "high deformations" corresponds to an Emax value of greater than a few%, for example 5%, or else 10% for a 0.25 mm radius of the specimen Rmax. A variant 11 of the device 10 is illustrated in FIG. 2a. The elements 20 to 26 are generally the same as in the device illustrated in FIG. The universal joint 27 is here replaced by a single bore 127 formed in the arm 28. The bore 127 then forms a specimen receiving orifice or point of attachment. The bore 127 must be chosen to have a diameter greater than the diameter of the test piece 15. The functional clearances thus present between the test piece 15 and the internal surface of the bore 127 offer the same degrees of freedom as the bearing 273 and the universal joint 27. The transverse friction with the test piece 15 is slightly greater but nevertheless still negligible in the measurement of the bending moment with which the test piece 15 is subjected and still allows to speak of a pure bending moment. As in the device 10, when the test piece 15 is biased in flexion in the device 11, it is in four-point contact with the device 11: the points 374a and 374b on the edges of the hole 127 and the points 32a and 32b on the bearing 31 (see Figure 2c). The central section of the specimen 15, that is to say between the points 374b and 32b facing each other between the arm 28 and the support 30, is subjected to a homogeneous moment. This is proven experimentally, for example by means of shots, such as those reproduced schematically in FIGS. 5a and 5b. A digital treatment of such shots indeed makes it possible to demonstrate the circular geometry reached during the bending of a specimen 15. Such a geometry is the proof of both a deformation in pure bending and the homogeneity of the material. . In the particular example of FIG. 5b, the radius of curvature Rd reached is equal to 4.3 mm. A still lower radius of curvature can be reached, the lower limit being reached when the arm 28 is in contact with the support 30. In the sections between the points 32a and 32b on the one hand and 374a and 374b on the other hand, the bending moment theoretically varies linearly.
    [0017] The bending moment is not homogeneous. The deformation of the specimen 15 between the points 374a and 374b (respectively 32a and 32b) results in a different angle contact between the specimen 15 and the contact surface at each of the points 374a and 374b. This difference in angle can therefore induce efforts along the axis of the specimen between the points 374a and 374b.
    [0018] Advantageously, rings 100 may therefore be provided, clamped on the ends of the test piece 15, against the arm 28 and the frame 30, outside the zone between the arm 28 and the frame 30 (FIG. 2b). The rings 100 have the role of preventing the longitudinal sliding of the test piece 15 by adding a longitudinal force against the perimeter of the bore 127 for balancing the normal forces at 374a and 374b (respectively 32a and 32b) respectively. The rings 100 thus make it possible to maintain a constant test piece length between the bearings 21 and 31 during the bending test. Another variant 12 of the device 10 is illustrated in FIGS. 3a and 3b. Elements similar to the embodiments described above have the same references in the figures and are not redescribed.
    [0019] In this variant 12, the pulley system 116, the universal joint 126 and the structures 123 and 128 are substituted for the system 16, the universal joint 26, the shaft shaft 23 and the arm 28 of the device 10. The structure 123 comprises a shaft 1231 and a sleeve 1232. The shaft 1231 is fixed on the frame 20. The sleeve 1232 is pivotally mounted on the shaft 1231, by means of a bearing, for example a ball bearing , not shown. The pulley system 116 comprises a wheel 124. Two openings 1241 pass through the wheel 124 longitudinally, between its two lateral faces. The wheel 124 is fixed on the sheath 1232.
    [0020] The structure 128 comprises an arm 1280, two branches 1281, a balancing mass 1282, here in the form of two weights. The arm 1280 is connected at one end to the universal joint 27. At the end of the arm 1280 opposite the seal 27, the two branches 1281 extend in fork, symmetrically, that is to say in mirror image, by report to the plan yz. Each branch 1281 has here since the arm 1280 a portion at an angle, a portion parallel to the arm 1280 and finally another portion at an angle, here non-limitatively parallel to the first portion at an angle. Each branch 1281 passes through a respective opening 1241 of the wheel 124. With the universal joint 126 described below, the branches 1281 are rotatable about two axes transverse to the longitudinal axis of the sleeve 1232, and transverse one to the other. Each branch 1281 here carries a balance weight 1282 at its distal end opposite to the arm 1280. The counterweights 1282 counterbalance the weight of the arm 1280 so that in the absence of the specimen 15, the arm 1280 is at the same time. balance, substantially horizontally. In other words, the weights 1282 make it possible to make the influence of the weight of the arm 1280 and the universal joint 27 negligible. The balancing masses 1282 can be replaced by other balancing masses such as an annular element connecting the branches 1281. The universal joint 126 here comprises a ring 1260, two pivot pins 1261 and two pivot pins 1262 (see Figure 6). The pivot axes 1261 and 1262 have for example but not limited to a needle shape. The pins 1262 pivotally connect the ring 1260 to the sheath 1232. The shafts 1261 pivotally connect the ring 1260 to each of the branches 1281 on the side of the pulley 16 opposite the universal joint 27. This advantageously makes it possible to increase the length L between the cardan joints 126 and 27, that is to say here between the axes 1261 and the axis 272, keeping a size of the device 12 similar to that of the device 10. The dimensions of the figures are not not limiting. It is possible for example to choose an arm 28 or 1280 of greater length. Another variant 13 of the device 10 is illustrated in FIG.
    [0021] In this variant, the frame 20, the pulley 16, the cardan joints 26 and 27 are the same as previously described. The device 13 comprises a structure 228 close to the structure 128 described above. The structure 228 comprises an arm 2280 which connects the cardan joints 26 and 27, two branches 2281 which extend in fork on either side of the arm 2280, a balancing mass 2282, here in the form of two mounted weights. respectively by each branch 2281 at its distal end opposite to the arm 2280. The branches 2281 do not pass through the wheel of the pulley 16. The 2282 weights have the same role of balancing the arm 2280 with respect to the cardan joint 26 that the weights 1282 with respect to the universal joint 126.
    [0022] Other embodiments are still possible, for example by combining the cardan joint 126 and the single bore 127 in a single bending test device. In all the embodiments described, rings 100 may be implemented with the same benefits as previously described.
    [0023] The above devices have been tested and validated experimentally. Two lines 301 and 302 illustrated in FIG. 4 were obtained during a bending test in the elastic domain (thus linear) of two test pieces, here steel wires. The first plot 301 was obtained by testing a slender steel wire of diameter 0.3 mm, a second trace 302 was obtained by testing a slender steel wire with a diameter of 0.5 mm.
    [0024] The curvature, or more precisely the variation of curvature with respect to the original curvature, is read on the abscissa axis, while the corresponding bending moment is read on the ordinate axis. The different points of these plots 301 and 302 were obtained on the one hand by measuring the bending moment applied to the yarn concerned as explained above, and on the other hand by measuring the radius of curvature on photographs or shots. views made at corresponding times. It is apparent that the plot 301 is offset from the origin of the graph and has as a starting point a curvature of about 15 m-1. Indeed, the sample is stored as a coil and has a non-zero initial radius of curvature. In practice, this initial radius of curvature only has the effect of shifting the curve. The trace 301 could be easily corrected by deducing, from all the readings (1 / Rc), the value 1 / Ro, where Ro is the initial radius of curvature of the test piece 15. The test piece 15, when it comprises Initially a non-zero curvature, once mounted in the system, will naturally tend to find a position to minimize both its elastic potential energy and the elastic potential energy of the entire system thanks to the degrees of freedom offered for example by bearings 273 and 31. The test piece 15 will then deform from this position of the lowest elastic potential energy.
    [0025] To obtain the trace 301, the test device 10 was used up to a curvature of the order of 95 m-1, ie a radius of curvature of 1/95 m, that is to say about 1.05 cm. Experimental tests have validated the use of the device 10 up to a radius of curvature of 7 mm for other materials having better bending properties than steel. Depending on the shape and size of the elements of the devices 10, 11, 12 or their variants, even lower radii of curvature can be obtained until the means for holding the two ends of the test piece 15, such as the bearing 273, the shaft 28 provided with the bore 127 or the bearing 31, touch each other.
    权利要求:
    Claims (16)
    [0001]
    REVENDICATIONS1. Four-point bending mechanical test device of a test piece, said device comprising: a) means for holding a first end of the test piece (27; 127; 28; 128) and means for holding a test piece; second end of the specimen (30, 31); b) traction means (25) and transformation means (16, 116) for converting a translation movement of said traction means (25) into a rotational movement; c) converting means (26; 27; 126; 127) for converting said rotational movement into bending deformation of the specimen, said converting means (26; 27; 126; 127) having at least one first joint gimbal (26; 126) connected to the holding means of the first end of the test piece (27; 127; 28; 128).
    [0002]
    2. Device according to claim 1, wherein the conversion means (26; 27; 126; 127) comprise a second universal joint (27).
    [0003]
    3. Device according to the preceding claim, the second universal joint (27) having a bearing (273).
    [0004]
    4. Device according to the preceding claim, the bearing (273) further forming part of the means for holding a first end of the test piece (27; 28; 128).
    [0005]
    5. Device according to claim 1, the first universal joint (26; 126) being connected to the holding means of a first end of the test piece (27; 127; 28; 128), the means for maintaining a first end of the specimen (27; 127; 28; 128) having at least one member (28; 128) provided with a bore (127) for receiving an end of a specimen.
    [0006]
    6. Device according to one of the preceding claims, the transformation means (16) comprising a wheel (24), the first universal joint (26) connecting the wheel (24) and the means for maintaining a first end of the test piece (27; 127; 28).
    [0007]
    7. Device according to one of the preceding claims, the first universal joint (126) being connected to at least one structure (128) which passes through the transformation means (116).
    [0008]
    8. Device according to the preceding claim, the structure (128) having two branches (1281) arranged in fork, the transformation means (116) having a wheel (124), the wheel (124) being provided with two through openings (1241). ), each branch (1281) passing through a respective one of the two openings (1241).
    [0009]
    9. Device according to one of claims 7 and 8, the structure (128) further comprising balancing means (1282).
    [0010]
    10. Device according to the preceding claim, the balancing means (1282) comprising at least one balancing mass.
    [0011]
    11. Device according to one of the preceding claims, further comprising measuring means for measuring a force exerted on the traction means (25) or measuring means for measuring a torsional force on a downstream member (28; ) to which the first universal joint (26; 126) is connected.
    [0012]
    Mechanical bending test system, comprising a traction machine and a mechanical bending test device (10; 11; 12) according to one of claims 1 to 11, the traction machine comprising a traction mechanism connected to the traction means (25) of the test device, the mechanism being configured to apply a traction force on these traction means.
    [0013]
    13. A method of mechanical test bending of a specimen using a mechanical flexural test device according to one of claims 1 to 11, comprising the steps of: - placing the test specimen in the means for holding a first end of a test piece (27, 273; 127) and in the means for holding a second end of the test piece (30, 31); - application of a tension on the traction means; determination of the bending moment by measuring means for measuring a force exerted on the traction means (25) or by measurement means for measuring a torsional force on a downstream member (28; 128) to which the first universal joint (26; 126).
    [0014]
    14. Method according to the preceding claim, the introduction of the specimen comprising the steps of: - clamping a first ring (100) on a first end of the specimen, against the means for holding the first end of a test piece (27, 273; 127); - Tightening a second ring (100) on a second end of the test piece against the holding means of the second end of the test piece (30, 31); the first and second rings (100) being clamped on the respective ends of the test piece outside the zone between the holding means of the first and the second end of the test piece.
    [0015]
    15. Method according to one of claims 13 or 14, wherein the specimen is slender.
    [0016]
    16. The method according to one of claims 13 to 15, wherein the specimen reaches a surface deformation of at least 3% or at least 5%.
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    同族专利:
    公开号 | 公开日
    WO2016001426A1|2016-01-07|
    US10508979B2|2019-12-17|
    EP3164690B1|2019-09-11|
    US20180202909A1|2018-07-19|
    EP3164690A1|2017-05-10|
    FR3023373B1|2016-08-19|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    GB409805A|1932-11-23|1934-05-10|Bernard Parker Haigh|Improved method and means for testing wires, wire ropes and rods by cyclic bending|
    US2170640A|1937-11-29|1939-08-22|John N Kenyon|Fatigue testing machine|
    FR2843633A1|2002-08-13|2004-02-20|Centre Nat Rech Scient|System for pure bending test, subjects two mutually identical items from a common specimen to antagonistic bending loads which are optionally alternating|
    US20130327152A1|2012-06-11|2013-12-12|Verizon Patent And Licensing Inc.|System and method for measuring cable bending force and cable kink force|
    US1443877A|1922-06-19|1923-01-30|Guelbaum David|Dynamometer for determining the modulus of elasticity|
    US5022273A|1990-06-11|1991-06-11|United States Surgical Corporation|Apparatus and method for testing the bending strength of needles|
    DE4104822A1|1991-02-16|1992-08-20|Telefunken Systemtechnik|TEST DEVICE FOR CARRYING OUT 4-POINT BEND CHANGING TESTS|
    RU2160892C2|1998-07-17|2000-12-20|Чернин Давид Борисович|Gear for pure bending test of samples|
    US20050109074A1|2003-11-21|2005-05-26|Olsen Vincent C.|Method and computer controlled apparatus for bending elongate material utilizing a pure bending moment|DE102016012677A1|2016-10-20|2018-04-26|Technische Universität Dortmund|Device and method for bending profiles or bar material, in particular unsymmetrical and open profiles or rod material|
    EP3318863B1|2016-11-07|2021-03-03|Airbus Operations S.L.|Systems and method for testing bonded joints|
    FR3081051B1|2018-05-14|2020-06-05|Centre Scientifique Et Technique Du Batiment|METHOD FOR CHARACTERIZING THE BEAM RESISTANCE TO A BEAM, AND ASSOCIATED SYSTEM|
    CN110346223B|2019-07-03|2021-08-10|中国商用飞机有限责任公司|Bending shear coupling test device|
    法律状态:
    2015-07-31| PLFP| Fee payment|Year of fee payment: 2 |
    2016-01-08| PLSC| Search report ready|Effective date: 20160108 |
    2016-07-29| PLFP| Fee payment|Year of fee payment: 3 |
    2017-07-31| PLFP| Fee payment|Year of fee payment: 4 |
    2018-07-30| PLFP| Fee payment|Year of fee payment: 5 |
    2019-07-30| PLFP| Fee payment|Year of fee payment: 6 |
    2020-07-31| PLFP| Fee payment|Year of fee payment: 7 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1456479A|FR3023373B1|2014-07-04|2014-07-04|PURE MECHANICAL TESTING DEVICE AND METHOD FOR IMPLEMENTING THE SAME|FR1456479A| FR3023373B1|2014-07-04|2014-07-04|PURE MECHANICAL TESTING DEVICE AND METHOD FOR IMPLEMENTING THE SAME|
    PCT/EP2015/065250| WO2016001426A1|2014-07-04|2015-07-03|Pure bending mechanical test device, and method for implementing same|
    EP15736423.3A| EP3164690B1|2014-07-04|2015-07-03|Pure bending mechanical test device, and method for implementing same|
    US15/322,591| US10508979B2|2014-07-04|2015-07-03|Pure bending mechanical test device and method for implementing same|
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