The original article. "
Foam structures with a negative Poisson's ratio", Science, 235 10381040 (1987).
This is the first designed negative Poisson's ratio material.
Summary
A novel foam structure is presented, which exhibits a negative Poisson's ratio. Such a material expands laterally (gets fatter) when stretched. See the upper foam (cellular solid) in the above image. Such behavior is in contrast to ordinary materials such as the lower foam in the image above. For example, rubber has a Poisson's ratio approaching the isotropic upper limit 0.5 and therefore becomes substantially thinner when stretched. Negative Poisson ratio solids easily undergo volume changes. By contrast, rubbery materials easily undergo shape changes (shear deformation) but are much stiffer in relation to volume changes. The distinction is shown in a map adapted from Milton.
Foams with negative Poisson's ratios were produced from conventional low density opencell polymer foams by causing the ribs of each cell to permanently protrude inward, resulting in a reentrant structure. Specimens of conventional foam were compressed triaxially, i.e. in three orthogonal directions, and were placed in a mold. The mold was heated to a temperature slightly above the softening temperature of the foam material. Stress strain curves and curves of nonlinear behavior are given below. These foams are essentially isotropic; they do not depend on anisotropy to achieve the effects observed. Applications of novel, reentrant foams with negative Poisson's ratios may be envisaged in view of the above. An example of the practical application of a particular value of Poisson's ratio is the cork of a wine bottle. The cork must be easily inserted and removed, yet it also must withstand the pressure from within the bottle. Rubber, with a Poisson's ratio of 0.5, could not be used for this purpose because it would expand when compressed into the neck of the bottle and would jam. Cork, by contrast, with a Poisson's ratio of nearly zero, is ideal in this application. It is anticipated that reentrant foams may be used in such applications as sponges, robust shock absorbing material, air filters, biomaterials and
fasteners.
Negative Poisson's ratio effects can result from
nonaffine deformation, from certain
chiral microstructures, on an
atomic scale, or from structural hierarchy. Negative Poisson's ratio materials can exhibit slow decay of stress according
to SaintVenant's principle. Later writers have
called such materials antirubber, auxetic (auxetics), or dilatational. These materials are an example of extremal materials. They have also been called metamaterials by later writers.
Combined foam
animation shows normal and reentrant foams together.
Patents.
There are several U. S. patents as well as Canada and overseas patents.
If you are interested in commercial applications, please contact the Wisconsin Alumni Research Foundation (WARF), for information on U. S. and international patents and licensing.
Lakes, R. S.,"Foam structures with a negative Poisson's ratio", Science, 235 10381040 (1987). See summary above.
Lakes, R. S., "Negative Poisson's ratio materials", Science, 238 551 (1987).
The negative Poisson's ratio effect is not due to Cosserat elasticity. The classical theory of elasticity has no length scale. Negative Poisson's ratio is classically attainable and does not require the characteristic length scale present in Cosserat or micropolar elasticity.
Get pdf or gif. Further details are given here on Poisson's ratio in linear isotropic elasticity.
Friis, E. A., Lakes, R. S., and Park, J. B., "Negative Poisson's ratio polymeric and metallic materials", Journal of Materials Science, 23, 44064414 (1988).
Foam materials based on metal and several polymers were transformed so that their cellular architectures became reentrant, ie. with inwardly protruding cell ribs. Foams with reentrant structures exhibited negative Poisson's ratios as well as greater resilience than conventional foams. Foams with negative Poisson's ratios were prepared using different techniques and materials
and their mechanical behavior and structure evaluated.
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Chen, C. P. and Lakes, R. S., "Dynamic wave dispersion and loss properties of conventional and negative Poisson's ratio polymeric cellular materials", Cellular Polymers, 8(5), 343359 (1989).
This article describes experimental investigations of the dynamical behaviour of conventional and negative Poisson's ratio foamed materials in torsional vibration. Dispersion of standing waves and cutoff frequencies were observed. Consequently, foamed materials do not obey the classical theory of elasticity or viscoelasticity. The dynamical effects were attributed to microvibrations of the cell ribs in a structural view and were associated with microstructure or micromorphic elasticity in a continuum view. Cutoff frequencies were lower in reentrant foams with negative Poisson's ratios than in the conventional foams from which they were derived. An analytical structural model was developed in which the ribs of the conventional foams were modeled as freefree vibrating beams. The predicted cutoff frequencies were comparable to those observed experimentally.
In more recent parlance, these materials may be referred to as locally resonant metamaterials.
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Chen, C. P. and Lakes, R. S., "Holographic study of conventional and negative Poisson's ratio metallic foams: elasticity, yield, and microdeformation", J. Materials Science, 26, 53975402 (1991)
This article presents an experimental study by holographic interferometry of the following material properties of conventional and negative Poisson's ratio copper foams: Young's moduli, Poisson's ratios, yield strengths, and characteristic lengths associated with inhomogeneous deformation. The Young's modulus and yield strength of the conventional copper foam were comparable to those predicted by microstructural modelling on the basis of cellular rib bending. The reentrant copper foam exhibited a negative Poisson's ratio as indicated by the elliptic contour fringes on the specimen surface in the bending tests. Inhomogeneous, nonaffine deformation was observed holographically in both foam materials.
Get pdf; holographic bend fringe images.
Choi, J. B. and Lakes, R. S., "Design of a fastener based on negative Poisson's ratio foam", Cellular Polymers, 10, 205212 (1991).
In this article we make use of the negative Poisson's ratio of recently developed cellular solids or spongy materials in the design of a pressfit fastener. Insertion of the fastener is facilitated by the lateral contraction which negative Poisson's ratio materials exhibit under compression. Removal of the fastener is resisted by the corresponding elastic expansion under tension.
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Lakes, R. S., "Experimental micro mechanics methods for conventional and negative Poisson's ratio cellular solids as Cosserat continua", J. Engineering Materials and Technology, 113, 148155 (1991).
Continuum representations of micromechanical phenomena in structured materials are described, with emphasis on cellular solids. These phenomena are interpreted in light of Cosserat elasticity, a generalized continuum theory which admits degrees of freedom not present in classical elasticity. These are the rotation of points in the material, and a couple per unit area or couple stress. Experimental work in this area is reviewed, and other interpretation schemes are discussed. The applicability of Cosserat or micropolar elasticity to cellular solids and fibrous composite materials is considered as is the application of related generalized continuum theories. New experimental results are presented for foam materials with negative Poisson's ratios.
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Lakes, R. S., "Deformation mechanisms of negative Poisson's ratio materials: structural aspects", J. Materials Science, 26, 22872292 (1991).
Poisson's ratio in materials is governed by the following aspects of the microstructure: the presence of rotational degrees of freedom, nonaffine deformation kinematics, or anisotropic structure. Several structural models are examined. The nonaffine kinematics are seen to be essential for the production of negative Poisson's ratios for isotropic materials containing central force linkages of positive stiffness. Noncentral forces combined with preload can also give rise to a negative Poisson's ratio in isotropic materials. A chiral microstructure with noncentral force interaction or nonaffine deformation can also exhibit a negative Poisson's ratio. Toughness and damage resistance in these materials may be affected by the Poisson's ratio itself, as well as by generalized continuum aspects associated with the microstructure.
Choi, J. B. and Lakes, R. S., "Nonlinear properties of polymer cellular materials with a negative Poisson's ratio", J. Materials Science, 27, 46784684 (1992). Cover issue.
Negative Poisson's ratio polymeric cellular solids (reentrant foams) were studied to ascertain the optimal processing procedures which give rise to the smallest value of Poisson's ratio. The nonlinear stress  strain relationship was determined for both conventional and reentrant foams; it depended upon the permanent volumetric compression achieved during the processing procedure. Poisson's ratio measured as a function of strain was found to have a relative minimum at small strains. The toughness of reentrant foam increased with permanent volumetric compression, hence density.
Stressstrain curve
Diagram.
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Lakes, R. S., "The time dependent Poisson's ratio of viscoelastic cellular materials can increase or decrease", Cellular Polymers, 11, 466469, (1992).
In viscoelastic materials, the Poisson's ratio is not a material constant but can depend upon time. For polymeric solids, the shear modulus relaxes much more than the bulk modulus, therefore, the Poisson's ratio n(t) is an increasing function of time. In this article we demonstrate that such time dependence is not a necessary consequence of the theory of viscoelasticity. Viscoelastic composite microstructures are presented which result in n(t) which decreases with time.
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Lakes, R. S., "Saint Venant end effects for materials with negative Poisson's ratios", J. Applied Mechanics, 59, 744746 (1992).
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In this article we analyze SaintVenant end effects for materials with negative Poisson's ratios. We present an example of slow decay of stress arising from selfequilibrated stress at the end of a circular cylinder of elastic material with a negative Poisson's ratio. By contrast a sandwich panel containing rigid face sheets and a compliant core exhibits no anomalous effects for negative Poisson's ratio, but exhibits slow stress decay for core Poisson's ratio approaching 0.5. In sandwich panels with stiff but not perfectly rigid face sheets, slow decay of stress is known to occur; a negative Poisson's ratio results in end stress decay which is faster than it would be otherwise.
Choi, J. B. and Lakes, R. S., "Nonlinear properties of metallic cellular materials with a negative Poisson's ratio", J. Materials Science, 27, 53735381 (1992).
Negative Poisson's ratio copper foam was prepared and characterized experimentally.
The transformation into reentrant foam was accomplished by applying sequential permanent compressions above the yield point to achieve a triaxial compression. The Poisson's ratio of the reentrant foam depended on strain and attained a relative minimum at strains near zero. Poisson's ratio as small as 0.8 was achieved. The strain dependence of properties occurred over a narrower range of strain than in the polymer foams studied earlier. Annealing of the foam resulted in a slightly greater magnitude of negative Poisson's ratio and greater toughness at the expense of a decrease in the Young's modulus.
Get pdf; metal auxetics.
Lakes, R. S., "No contractile obligations", Nature, 358, 713714, (1992).
Stretch most materials and you will expect to see their cross section shrink. But Alderson and Evans have synthesized a microporous polymer that swells as it is stretched, and Milton has designed a laminated composite that does the same. These advances in the newly developing science of materials with a negative Poisson's ratio promise improved control of properties and open the door to a new class of applications. Get pdf
Lakes, R. S., "Design considerations for negative Poisson's ratio materials" ASME Journal of Mechanical Design, 115, 696700, (1993).
This article presents a study of the implications of negative Poisson's ratios in the design of load bearing structural elements. Stress concentration factors are reduced in some situations, and unchanged or increased in others, when the Poisson's ratio becomes negative. Stress decay according to Saint Venant's principle can occur more or less rapidly as the Poisson's ratio decreases. Several design examples are presented, including a core for a curved sandwich panel and a flexible impact buffer.
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Curvature of negative Poisson's ratio honeycomb during bending is convex in contrast to the saddle shape usually seen for positive Poisson's ratio, and is shown in the animation at the right and in this video
Lakes, R. S., "Advances in negative Poisson's ratio materials" , Advanced Materials (Weinheim, Germany), 5, 293296, (1993).
This article presents a review of recent developments in negative Poisson's ratio materials based on foams, laminates, microporous materials, and materials with structural hierarchy. Get pdf. By this time the term auxetic material had been introduced.
Rosakis, P., Ruina, A., and Lakes, R. S., "Microbuckling instability in elastomeric cellular solids", J. Materials Science, 28, 46674672 (1993).
Compressive properties of elastic cellular solids are studied via experiments upon foam and upon single cell models. Open cell foam exhibits a monotonic stressstrain relation with a plateau region; deformation is localized in transverse bands. Single cell models exhibit a forcedeformation relation which is not monotonic. In view of recent concepts of the continuum theory of elasticity, the banding instability of the foam in compression is considered to be a consequence of the nonmonotonic relation between force and deformation of the single cell.
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Chen, C. P. and Lakes, R. S., "Viscoelastic behaviour of composite materials with conventional or negative Poisson's ratio foam as one phase", J. Materials Science, 28, 42884298, (1993).
This article describes experimental investigations of viscoelastic properties of composites consisting of conventional and reentrant negative Poisson's ratio copper foam as a matrix, with high loss filler materials: viscoelastic elastomer, solder, and indium. Viscoelastic properties of gallium and several ferrites were determined as well. The loss tangent of the copper elastomer composite substantially exceeded the (lower) Voigt limit; the loss tangent of the coppersolder and copperindium composites were close to the (upper) Hashin limit for two solid phases and one pore phase.
Chen, C. P. and Lakes, R. S., "Holographic study of nonaffine deformation in copper foam with a negative Poisson's ratio 0.8", Scripta Metall et Mater., 29, 395399, (1993).
Microdeformation studies of conventional and negative Poisson's ratio copper foams were conducted holographically. Inhomogeneous, nonaffine deformation was observed holographically in both foam materials. The negative Poisson's ratio material with a permanent volumetric compression ratio 2.2 exhibited a substantially greater nonaffine deformation than the conventional material, in contrast to foam with compression ratio 3.0 examined earlier.
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Lakes, R. S. and Elms, K., "Indentability of conventional and negative Poisson's ratio foams", J. Composite Materials, 27,11931202, (1993).
The indentation resistance of foams, both of conventional structure and of a novel reentrant structure giving rise to negative Poisson's ratio, was studied using holographic interferometry. In holographic indentation tests, reentrant foams had higher yield strengths sigma _{y } and lower stiffness E than conventional foams of the same original relative density. Damage in both kinds of foam occurred primarily directly under the indenter. Calculated energy absorption for dynamic impact is considerably higher for reentrant foam than conventional foam.
Lakes, R. S., "Materials with structural hierarchy", Nature, 361, 511515 (1993). Cover issue.
New hierarchical microstructures are presented for cellular materials, in which the structural elements themselves are cellular. The compressional strength of low density hierarchical materials can be thousands of times greater than that of a conventional cellular material of the same density. The use of hierarchical structure to achieve negative Poisson's ratio is reviewed.
Choi, J. B. and Lakes, R. S., "Nonlinear analysis of the Poisson's ratio of negative Poisson's ratio foams", J. Composite Materials, 29, (1),113128, (1995).
This article contains analytic study of Poisson's ratio of reentrant foam materials with negative Poisson's ratio. These materials get fatter when stretched and thinner when compressed. The Poisson effect is so fundamentally important to the properties of a material that a large change in the value of the ratio will have significant effects on the material's mechanical performance. Isotropic foam structures with negative Poisson's ratio have been fabricated through a permanent volumetric transformation. The cells were converted from the convex polyhedral shape of conventional foam cells to a concave or "reentrant" shape. Mechanical behavior of a reentrant open cell foam material will differ from that of a conventional foam in ways not addressed by existing theoretical treatment. Poisson's ratio as a function of strain is obtained by modeling the three dimensional unit cell as an idealized polyhedron unit cell. Poisson's ratio is predicted to approach the isotropic limit of 1 with increasing permanent volumetric compression ratio of idealized cells, in comparison with experimental values as small as  0.8.
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Chen, C. P., and Lakes, R. S., "Micromechanical analysis of dynamic behavior of conventional and negative Poisson's ratio foams", J. Engineering Materials and Technology, 118, 285288 (1996).
Both conventional and negative Poisson's ratio foams exhibit dispersion of acoustic waves as well as cutoff frequencies at which the group velocity tends to zero. This macroscopic behavior is attributed to microvibration of the cell ribs. The purpose of this article is to develop a micromechanical model of the cutoff frequency. This model is based on the resonance of ribs which may be straight, curved, or convoluted.
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Choi, J. B. and Lakes, R. S., "Fracture toughness of reentrant foam materials with a negative Poisson's ratio: experiment and analysis", Int. J. Fracture, 80, 7383, (1996).
Fracture toughness of reentrant foam materials with a negative Poisson's ratio is explored experimentally as a function of permanent volumetric compression ratio, a processing variable. Values of J toughness of negative Poisson's ratio open cell copper foams are enhanced by 80%, 130%, and 160% for permanent volumetric compression ratio of 2.0, 2.5, and 3.0, respectively, compared to the J value of the conventional foam (with a positive Poisson's ratio). Analytical studies are based on idealized polyhedral cell structures approximating the shape of the conventional and reentrant cells. For conventional foam, analysis shows toughness increasing with density. For reentrant foam, the analysis shows toughness increasing as Poisson's ratio becomes more negative.
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Prall, D. and Lakes, R. S., "Properties of a chiral honeycomb with a Poisson's ratio 1", Int. J. of Mechanical Sciences, 39, 305314, (1996).
A theoretical and experimental investigation is conducted of a twodimensionally chiral honeycomb. The honeycomb exhibits a Poisson's ratio of 1 for deformations inplane. This Poisson's ratio is maintained over a significant range of strain, in contrast to the variation with strain seen in known negative Poisson's ratio materials.
Lee, T. and Lakes, R. S., "Anisotropic polyurethane foam with Poisson's
ratio greater than 1", Journal of Materials Science, 32, 23972401, (1997).
Anisotropic polymer foams have been prepared, which exhibit a Poisson's ratio exceeding 1, and ratios of longitudinal to transverse stiffness exceeding 50. The foams are as much as 20 times stiffer in the longitudinal direction than the foams from which they were derived. The transformation process involved applying to opencell polyurethane foam an axial strain of 25% to 45%, at a temperature above the softening point, followed by cooling under axial strain.
Get pdf,
Fig. 7,
Fig. 8.
Loureiro, M. A. and Lakes, R. S., "Scaleup of transformation of negative Poisson's ratio foam: Slabs, Cellular Polymers, 16, 349363, (1997).
This paper presents an experimental study performed on the scaleup of processing of negative Poisson's ratio foam. These materials become thinner under compression and fatter under tension, opposite to ordinary materials. The transformation process consists of triaxial compression combined with heat treatment. Transformed foam cells have a concave or "reentrant" shape. Scaleup is achieved by use of a modified mold assembled around the foam slab and longer processing times. Foam with a distribution of cell sizes was transformed in small block and large slab forms. These blocks and slabs exhibited a negative Poisson's ratio.
Lakes, R. S. and Lowe, A. "Negative Poisson's Ratio Foam as Seat Cushion Material", Cellular Polymers, 19, 157167, (2000).
Negative Poisson's ratio foam was used in the development of seat cushions which exert reduced peak pressure upon the skin of seated persons. Foam processing techniques were scaled up. A longer processing time was required for cushion size samples in comparison with small samples. Pressure distributions on a seated subject were measured using a pressuresensitive array. Seated pressure distribution became more favorable with decreasing sample density for both conventional and reentrant foam blocks. Foam thickness played a small role in the seated pressure performance of foam cushions. Reentrant foam at densities of between 2 and 4 lb/ft^{3} (0.032 to 0.064 g/cm^{3}) performed better (lower maximum seating pressure) than conventional foam samples of comparable density.
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Lakes, R. S., "Lateral Deformations in Extreme Matter", perspective, Science, 288, 1976, June (2000).
article link,
pdf
Lakes, R. S., "A broader view of membranes", Nature, 414, 503504, 29 Nov. (2001). 
pdf. Interpretation of an advance in auxetic membranes.
Brandel, B. and Lakes, R. S., "Negative Poisson's ratio polyethylene foams", J. Materials Science, 36, 58855893, July (2001). Various polyethylene foams were subjected to thermomechanical processing with the aim of transforming them into reentrant materials exhibiting negative Poisson's ratio. Following transformation, large cell foams (cell sizes of 1 and 2 mm) exhibited reentrant cell structure and negative Poisson's ratio over a range of processing times and temperatures. Poisson's ratio vs. strain for these foams was similar to prior results for reticulated polyurethane foams. Following processing, microcellular polyethylene foam was densified but cells remained convex; it did not exhibit a substantial negative Poisson's ratio. This foam had a different transition temperature as determined via DSC than the large cell foams.
pdf
Wang, Y. C., Lakes, R. S., and Butenhoff, A., "Influence of cell size on reentrant transformation of negative Poisson's ratio reticulated polyurethane foams", Cellular Polymers, 20: 373385, (2001). Several foams of different cellsize, including Scott Industrial polyurethane foam with large cells (20 pores per inch, ppi, or 1.2 mm per pore, black), medium cells (65 ppi, or 0.4 mm per pore, green), and nearmicrocellular (100 ppi, 0.25 mm per pore, white), were processed over various time and temperature regimes to ascertain the role of cell size in transformation to negative Poisson's ratio materials. These foams were transformed successfully, and exhibited negative Poisson's ratio behavior. Poisson's ratio was measured using a new laser based setup. For all asreceived (unprocessed) foams with different cell sizes, Poisson's ratio decreased with compressive axial strain and increased with tensile strain up to a maximum. The maximum Poisson's ratio in tension decreased as cell size increases. The strain at which maximum Poisson's ratio occurs, increased with cell size. In negative Poisson's ratio foams, minimum Poisson's ratios of 0.8, 0.5, and 0.4 for 20 ppi, 65 ppi, and 100 ppi foams, respectively were observed.
pdf
Lakes, R. S. and Witt, R., "Making and characterizing negative Poisson's ratio materials", International Journal of Mechanical Engineering Education, 30, 5058, Jan. (2002). We present an introduction to the use of negative Poisson's ratio materials to illustrate various aspects of mechanics of materials. Poisson's ratio is defined as minus the ratio of transverse strain to longitudinal strain in simple tension. For most materials, Poisson's ratio is close to 1/3. Negative Poisson's ratios are counterintuitive but permissible according to the theory of elasticity. Such materials can be prepared for classroom demonstrations, or made by students.
pdf
Wang, Y. C. and Lakes, R. S., "Analytical parametric analysis of the contact problem of human buttocks and negative Poisson's ratio foam cushions", International Journal of Solids and Structures, 39, 48254838 Sept. (2002). Analytical investigations on the contact problems between two homogeneous and isotropic soft bodies were performed to simulate the contact of human buttocks and seat cushions. The cushion materials' Poisson's ratio were allowed to be negative. The human buttocks were modeled as an ideal sphere with radius 15 cm, and assumed to have a low Young's modulus and a Poisson's ratio close to 0.5. These parameters were held constant during our analysis. Peak contact pressure was reduced by adjusting the contour curvature of cushions according to Hertz theory, as expected. Moreover, analysis by both the Hertz model and a finite thickness 3D elasticity model showed that using negative Poisson's ratio cushions could further reduce the pressure. Negative Poisson's ratio cushions may be beneficial in the prevention of pressure sores or ulcers in the sick and in reduction of pressureinduced discomfort in seated people.
pdf
Wang, Y. C. and Lakes, R. S., "Composites with inclusions of negative bulk modulus: extreme damping and negative Poisson's ratio", J. Composite Materials, 39, 16451657, (2005).
The effect of a negative bulk modulus phase in elastic composites is studied. Negative bulk modulus K < 0 is shown to be possible in selected unit cells. In isotropic solids, K < 0 can be attained for negative Poisson's ratio sufficiently small, below the stability limit (for stress control) Poisson's ratio = 1. Such materials, if used as inclusions, are predicted to be stable with respect to band formation, even if they are large. Composites with spherical inclusions of negative bulk moduli are shown to exhibit negative Poisson's ratio and anomalies in composite bulk modulus and Young's modulus (and in the corresponding mechanical damping) but not in the shear modulus. pdf
Martz, E. O., Lakes, R. S., Goel, V. K. and Park, J. B. "Design of an artificial intervertebral disc exhibiting a negative Poisson's ratio", Cellular Polymers, 24, 127138, (2005). An artificial intervertebral disc exhibiting an anisotropic negative Poisson's ratio has been designed and characterized in the laboratory. This disc prosthesis incorporates negative Poisson's ratio to prevent bulge which might impinge on nerves, as well as the duplication of compressive axial stiffness of the natural lumbar intervertebral disc. The disc is also compliant in bending and torsion. No claim is made regarding possible clinical benefit is made based on this laboratory research. No tests upon living animals or humans were done in this project.
Lakes, R. S. and Wineman, A., "On Poisson's ratio in linearly viscoelastic solids", Journal of Elasticity, 85, 4563 (2006). Poisson's ratio in viscoelastic solids is in general a time dependent (in the time domain) or a complex frequency dependent quantity (in the frequency domain). We show that the viscoelastic Poisson's ratio has a different time dependence depending on the test modality chosen; interrelations are developed between Poisson's ratios in creep and relaxation. The difference, for a moderate degree of viscoelasticity, is minor. Correspondence principles are derived for the Poisson's ratio (also called the Poisson coefficient or Poissonzahl) in transient and dynamic contexts. The viscoelastic Poisson's ratio need not increase with time, and it need not be monotonic with time. Physical examples are given of material microstructures which give rise to designed time dependent Poisson's ratios. Some of these microstructures give rise to negative Poisson's ratio over part of the time scale.
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Shang, X. and Lakes, R. S., "Stability of elastic material with negative stiffness and negative Poisson's ratio", Physica Status Solidi (b), 244, 10081026 (2007).
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Moore, B., Jaglinski, T., Stone, D. S., and Lakes, R. S., "On the bulk modulus of open cell foams", Cellular Polymers, 26, 110, March (2007). Bulk properties of open cell polyurethane foam are studied in a hydrostatic compression experiment under strain control. A linear region of behaviour is observed in the stressstrain curve, followed by a nonmonotonic region corresponding to a negative incremental bulk modulus. The bulk modulus in the linear region is in reasonable agreement with the value calculated from compressional Young's modulus and Poisson's ratio. The linear region of behaviour in hydrostatic compression corresponds to less than half the axial strain range observed in axial compression.
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Link to Rapra technology, journal site.
Lakes, R. S., "Solids with tunable positive or negative thermal expansion of unbounded magnitude", Applied Phys. Lett. 90, 221905 (2007).
Material microstructures are presented with a coefficient of thermal expansion larger in magnitude than that of either constituent. Thermal expansion can be large positive, zero, or large negative. Threedimensional lattices with void space exceed twophase bounds but obey three phase bounds; lattices and normal materials have a trend of expansion decreasing with modulus. Two phase composites with a negative stiffness phase exceed bounds that assume positive strain energy density. The author determined Young's modulus and its relation to thermal expansion. Behavior of these composites is compared with that of homogeneous solids in expansion modulus maps.
APL link
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Dong, L., Stone, D. S., and Lakes, R. S., "Broadband viscoelastic spectroscopy measurement of mechanical loss and modulus of polycrystalline BaTiO_{3} vs. temperature and frequency", Phys. Stat. Sol. (b), 245, 24222432, Nov. (2008). get pdf
Dong, L. Stone, D. S., Lakes, R. S., "Softening of bulk modulus and negative Poisson's ratio in barium titanate ceramic near the Curie point", Philosophical Magazine Lett. 90, 2333, Jan. (2010). Formal journal formatted reprints are available; if you want one, please request it.
Substantial softening in the bulk modulus (a factor of five) and a negative Poisson ratio (0.25) have been observed via broadband viscoelastic spectroscopy in the vicinity of the Curie point of a barium titanate ceramic. These effects were observed under electrical shortcircuit conditions at low deformation frequencies. Softening was less in an electric open circuit or at higher frequencies. Softening of individual elastic modulus tensor elements is known to occur near phase transformations, but softening of the bulk modulus has not previously been well reported.
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Dong, L., Stone, D. S., and Lakes, R. S., "Anlastic anomalies and negative Poisson's ratio in tetragonal BaTiO_{3} ceramics", Applied Phys. Lett. 96, 141904 (2010). Anelastic anomalies, sharp variations in modulus and damping with temperature, were observed in tetragonal BaTiO_{3} via broadband viscoelastic spectroscopy after aging at 50 deg C for 15 h. The effect was most pronounced under electrical short circuit condition, at low frequency and under small excitation strain 10^{6}. Softening in bulk modulus and negative Poisson's ratio were observed near 60 deg C. Effects are attributed to an oxygen vacancy mechanism. A relaxational model cannot account for sharp response at smaller strains. Heterogeneity of negative stiffness is considered as a cause.
APL link. get pdf.
Greaves, G. N., Greer, A. L., Lakes, R. S., and Rouxel, T., "Poisson's Ratio and Modern Materials", Nature Materials, 10, 823837 Nov. (2011).
In comparing a material's resistance to distort under mechanical load rather than alter in volume, Poisson's ratio offers the fundamental metric by which to compare the performance of any material when strained elastically. The numerical limits are set by 1/2 and 1, between which all stable isotropic materials are found. With new experiments, computational methods and routes to materials synthesis, we assess what Poisson's ratio means in the contemporary understanding of the mechanical characteristics of modern materials. Central to these recent advances, we emphasize the significance of relationships outside the elastic limit between Poisson's ratio and densification, connectivity, ductility and the toughness of solids; and their association with the dynamic properties of the liquids from which they were condensed and into which they melt. get pdf.
Jaglinski, T. and Lakes, R. S., "Resonant ultrasound spectroscopy of cylinders over the full range of Poisson's ratio" Rev. Sci. Instr. 82, 035105 (2011). Mode structure maps for freely vibrating cylinders over a range of Poisson's ratio, are desirable for design and interpretation of experiments using resonant ultrasound spectroscopy (RUS). The full range of isotropic Poisson's ratio (1 to +0.5) is analyzed here using a finite element method to accommodate materials with a negative Poisson's ratio. The fundamental torsional mode has the lowest frequency provided Poisson's ratio is between about 0.24 and +0.5. For any Poisson's ratio, the torsional mode can be identified utilizing the polarization sensitivity of the shear transducers. RUS experimental results for materials with Poisson's ratio +0.3, +0.16 and 0.3 and a previous numerical study for Poisson's ratio = 0.33 are compared with the present analysis. Interpretation of results is easiest if the length / diameter ratio of the cylinder is close to 1. Slight material anisotropy leads to splitting of the higher modes but not of the fundamental torsion mode.
get pdf. Journal link, online version.
Dong, L, and Lakes, R. S., "Frequency dependence of Poisson's ratio of viscoelastic elastomer foam", Cellular Polymers, 30, 277285, (2011). Poisson's ratio increases with frequency as a result of stress induced air flow. Air within the pores contributes to the overall bulk modulus at high frequency, but not at low frequency at which it easily flows when the foam is deformed. Such behaviour is the opposite of that of solid polymers in which the shear modulus varies with frequency much more than the bulk modulus. get pdf.
Dong, L, and Lakes, R. S., "Frequency dependence of Poisson's ratio of viscoelastic elastomer foam", Cellular Polymers, 30, 277285, (2011). All polymer foams are viscoelastic; for foams used in earplugs, this response is essential to their function. Poisson's ratio was inferred from viscoelastic response of earplug foam in torsion and bending. Poisson's ratio increases with frequency as a result of stress induced air flow. Air within the pores contributes to the overall bulk modulus at high frequency, but not at low frequency at which it easily flows when the foam is deformed. Such behaviour is the opposite of that of solid polymers in which the shear modulus varies with frequency much more than the bulk modulus. The frequency dependent Poisson's ratio is related by Fourier transform to the time dependent Poisson's ratio. get pdf.
Li, D., Dong, L., and Lakes, R. S., "Resonant ultrasound spectroscopy of cubes over the full range of Poisson's ratio", Rev. Sci. Instr. 83, 113902 (2012).
Methods are developed for study of isotropic cubes via resonant ultrasound spectroscopy. To that end, mode structure maps are determined for freely vibrating isotropic cubes via finite element method over the full range of Poisson's ratio (from 1 to +0.5). The fundamental torsional mode has the lowest frequency provided Poisson's ratio is between about 0.31 and +0.5. Experimental measurements for the mode structures of materials with Poisson's ratio +0.33, +0.3, +0.15, 0.15, and 0.72 are performed using resonant ultrasound spectroscopy and interpreted. Methods are developed to identify pertinent modes.
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Li, D., Jaglinski, T. M., Stone, D. S. and Lakes, R. S., "Temperature insensitive negative Poisson's ratios in isotropic alloys near a morphotropic phase boundary, Appl. Phys. Lett, 101, 251903, Dec. (2012). Poisson's ratio, shear modulus, and damping of polycrystalline indiumtin (InSn) alloys in the vicinity of the morphotropic gammagamma + beta phase boundary were measured with resonant ultrasound spectroscopy. Negative Poisson's ratios were observed from 24 C to 67 C for alloys near the phase boundary. Properties were unaffected by annealing at 100 C for 2 days. This isotropic fully dense negative Poisson's ratio material is temperature insensitive, in contrast to other materials that undergo phase transformation.
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Li, D., Dong, L., and Lakes, R. S., "The properties of copper foams with negative Poisson's ratio via resonant ultrasound spectroscopy", Physica Status Solidi , 250(10), 19831987 (2013). DOI number: 10.1002/pssb.201384229 (2013). The Poisson's ratios of reentrant Cu foams with different initial relative densities were studied by resonant ultrasound spectroscopy (RUS). Slight anisotropy in foam was detected by RUS and removed by a small unidirectional compression. The transformation into the reentrant foam was accomplished by applying a sequence of permanent triaxial compression deformations. The Poisson's ratio first decreases and then increases with increasing compression strain. A minimum in Poisson's ratio of approximately 0.7 for all initial densities was achieved with an appropriate permanent compression strain, compared with 0.6 at similar density determined earlier via optical methods. Foams with higher values of initial density attained minima in Poisson's ratio at lower permanent volumetric compression. The shear modulus increased with increasing volumetric compression ratio, and showed a small hump near the point corresponding to Poisson's ratio minimum. get pdf
D. Li, L. Dong and Lakes, R. S., The resonant ultrasound spectroscopy method for determining the Poisson's ratio of spheres over the full range, Materials Letters, 143 3134 (2015).
The method for determining the Poisson's ratio of isotropic spheres was studied via resonant ultrasound spectroscopy (RUS). To that end, the mode structure maps for freely vibrating isotropic spheres were obtained via finite element method over the full range of Poisson's ratio (1 to +0.5). RUS measurements for spherical samples (indium, steel, SiO2, 13.5 wt% InSn, and copper foam) were compared with the numerical results and the Poisson's ratios were determined as +0.4, +0.3, +0.2, 0.08, and 0.3, respectively. The effects of slight shape imperfection upon the first 12 modes were analyzed for various Poisson's ratios, and were found to be negligible in interpretation of the experimental results.
Journal link
Negative Poisson's ratio in deformed
chicken wire. Positive Poisson's ratio, as one might expect, in normal chicken wire.
The effect of geometry on Poisson's ratio can also be explored using models based on LEGO blocks:
MRSEC LEGO education book pdf.
The second international workshop on auxetic ( negative Poisson's ratio ) materials and related systems was held near Poznan, Poland in August 2005.
Link 2005;
group
image courtesy Professor Peel. I am second from the right.
2007, Malta 4th International Workshop on Auxetics and Related Systems & 4th Annual AuxetNet Young Researchers Forum
Link 2007
2009, 6th International Workshop on Auxetics and Related Systems, Bolton UK
Link 2009
2011, 8th International Workshop on Auxetics and Related Systems, Poznan, Poland
Link 2011
2012, 4th International Conference and 9th International Workshop on Auxetics and Related Systems, Bolton, UK
Link 2012
2014, 5th International Conference and 10th International Workshop on Auxetics and Related Systems, Poznan, Poland
Link 2014
imechanica blog node on auxetic materials
A special issue of Composites Science and Technology, 70, issue 7, 2010, was devoted to Chiral Smart Materials. The originating concept is the honeycomb of Prall and Lakes (1996), provided above
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