Knowledge (XXG)

Hardness

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450:, in technical usage, is the tendency of a material to fracture with very little or no detectable plastic deformation beforehand. Thus in technical terms, a material can be both brittle and strong. In everyday usage "brittleness" usually refers to the tendency to fracture under a small amount of force, which exhibits both brittleness and a lack of strength (in the technical sense). For perfectly brittle materials, yield strength and ultimate strength are the same, because they do not experience detectable plastic deformation. The opposite of brittleness is 220:. This tool consists of a scale arm with graduated markings attached to a four-wheeled carriage. A scratch tool with a sharp rim is mounted at a predetermined angle to the testing surface. In order to use it a weight of known mass is added to the scale arm at one of the graduated markings, the tool is then drawn across the test surface. The use of the weight and markings allows a known pressure to be applied without the need for complicated machinery. 573:
dislocations creates an anchor point and does not allow the planes of atoms to continue to slip over one another A dislocation can also be anchored by the interaction with interstitial atoms. If a dislocation comes in contact with two or more interstitial atoms, the slip of the planes will again be disrupted. The interstitial atoms create anchor points, or pinning points, in the same manner as intersecting dislocations.
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deformation. Although hardness is defined in a similar way for most types of test – usually as the load divided by the contact area – the numbers obtained for a particular material are different for different types of test, and even for the same test with different applied loads. Attempts are sometimes made to identify simple analytical expressions that allow features of the stress-strain curve, particularly the
561: 516: 340: 164: 622:(UTS), to be obtained from a particular type of hardness number. However, these are all based on empirical correlations, often specific to particular types of alloy: even with such a limitation, the values obtained are often quite unreliable. The underlying problem is that metals with a range of combinations of yield stress and 527:, or the structure and arrangement of the atoms at the atomic level. In fact, most important metallic properties critical to the manufacturing of today’s goods are determined by the microstructure of a material. At the atomic level, the atoms in a metal are arranged in an orderly three-dimensional array called a 576:
By varying the presence of interstitial atoms and the density of dislocations, a particular metal's hardness can be controlled. Although seemingly counter-intuitive, as the density of dislocations increases, there are more intersections created and consequently more anchor points. Similarly, as more
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Dislocations provide a mechanism for planes of atoms to slip and thus a method for plastic or permanent deformation. Planes of atoms can flip from one side of the dislocation to the other effectively allowing the dislocation to traverse through the material and the material to deform permanently.
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There are two types of irregularities at the grain level of the microstructure that are responsible for the hardness of the material. These irregularities are point defects and line defects. A point defect is an irregularity located at a single lattice site inside of the overall three-dimensional
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The way to inhibit the movement of planes of atoms, and thus make them harder, involves the interaction of dislocations with each other and interstitial atoms. When a dislocation intersects with a second dislocation, it can no longer traverse through the crystal lattice. The intersection of
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technique, which involves iterative FEM modelling of an indentation test, does allow a stress-strain curve to be obtained via indentation, but this is outside the scope of conventional hardness testing.) A hardness number is just a semi-quantitative indicator of the resistance to plastic
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due to friction from a sharp object. The principle is that an object made of a harder material will scratch an object made of a softer material. When testing coatings, scratch hardness refers to the force necessary to cut through the film to the substrate. The most common test is
531:. In reality, however, a given specimen of a metal likely never contains a consistent single crystal lattice. A given sample of metal will contain many grains, with each grain having a fairly consistent array pattern. At an even smaller scale, each grain contains irregularities. 549:
are a type of line defect involving the misalignment of these planes. In the case of an edge dislocation, a half plane of atoms is wedged between two planes of atoms. In the case of a screw dislocation two planes of atoms are offset with a helical array running between them.
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and Bennett hardness scale. Ultrasonic Contact Impedance (UCI) method determines hardness by measuring the frequency of an oscillating rod. The rod consists of a metal shaft with vibrating element and a pyramid-shaped diamond mounted on one end.
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Matyunin, VM; Marchenkov, AY; Agafonov, RY; Danilin, VV; Karimbekov, MA; Goryachkin, MV; Volkov, PV; Zhgut, DA (2021). "Correlation between the Ultimate Tensile Strength and the Brinell Hardness of Ferrous and Nonferrous Structural Materials".
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However, while a hardness number thus depends on the stress-strain relationship, inferring the latter from the former is far from simple and is not attempted in any rigorous way during conventional hardness testing. (In fact, the
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is formed. If there is a different type of atom at the lattice site that should normally be occupied by a metal atom, a substitutional defect is formed. If there exists an atom in a site where there should normally not be, an
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is formed. This is possible because space exists between atoms in a crystal lattice. While point defects are irregularities at a single site in the crystal lattice, line defects are irregularities on a plane of atoms.
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San-Miguel, A.; Blase, P.; Blase, X.; Mélinon, P.; Perez, A.; Itié, J.; Polian, A.; Reny, E.; et al. (1999-05-19). "High Pressure Behavior of Silicon Clathrates: A New Class of Low Compressibility Materials".
379:—the ability to temporarily change shape, but return to the original shape when the pressure is removed. "Hardness" in the elastic range—a small temporary change in shape for a given force—is known as 171:
There are three main types of hardness measurements: scratch, indentation, and rebound. Within each of these classes of measurement there are individual measurement scales. For practical reasons
247:. The tests work on the basic premise of measuring the critical dimensions of an indentation left by a specifically dimensioned and loaded indenter. Common indentation hardness scales are 601:
regime), which is the immediate outcome of a tensile test. This relationship can be used to describe how the material will respond to almost any loading situation, often by using the
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interstitial atoms are added, more pinning points that impede the movements of dislocations are formed. As a result, the more anchor points added, the harder the material will become.
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Careful note should be taken of the relationship between a hardness number and the stress-strain curve exhibited by the material. The latter, which is conventionally obtained via
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characteristics can exhibit the same hardness number. The use of hardness numbers for any quantitative purpose should, at best, be approached with considerable caution.
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measures the resistance of a sample to material deformation due to a constant compression load from a sharp object. Tests for indentation hardness are primarily used in
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that can be applied. Toughness tends to be small for brittle materials, because elastic and plastic deformations allow materials to absorb large amounts of energy.
1237: 402:. This response produces the observed properties of scratch and indentation hardness, as described and measured in materials science. Some materials exhibit both 398:
is the point at which elastic deformation gives way to plastic deformation. Deformation in the plastic range is non-linear, and is described by the
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In glasses, hardness seems to depend linearly on the number of topological constraints acting between the atoms of the network. Hence, the
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Smedskjaer, Morten M.; John C. Mauro; Yuanzheng Yue (2010). "Prediction of Glass Hardness Using Temperature-Dependent Constraint Theory".
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Busby, JT; Hash, MC; Was, GS (2005). "The relationship between hardness and yield stress in irradiated austenitic and ferritic steels".
503:. Stiffness is often confused for hardness. Some materials are stiffer than diamond (e.g. osmium) but are not harder, and are prone to 480:. However, below a critical grain-size, hardness decreases with decreasing grain size. This is known as the inverse Hall-Petch effect. 818: 1261: 1189: 589:, captures the full plasticity response of the material (which is in most cases a metal). It is in fact a dependence of the (true) 605:(FEM). This applies to the outcome of an indentation test (with a given size and shape of indenter, and a given applied load). 1246: 984: 92:, but the behavior of solid materials under force is complex; therefore, hardness can be measured in different ways, such as 862: 1286: 1234: 682: 672: 428:
is a measure of the extent of a material's elastic range, or elastic and plastic ranges together. This is quantified as
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Leslie, W. C. (1981). The physical metallurgy of steels. Washington: Hemisphere Pub. Corp., New York: McGraw-Hill,
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Tekkaya, AE (2001). "Improved relationship between Vickers hardness and yield stress for cold formed materials".
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Tiryakioglu, M (2015). "On the relationship between Vickers hardness and yield stress in Al-Zn-Mg-Cu Alloys".
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Wredenberg, Fredrik; PL Larsson (2009). "Scratch testing of metals and polymers: Experiments and numerics".
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of a diamond-tipped hammer dropped from a fixed height onto a material. This type of hardness is related to
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lattice of the grain. There are three main point defects. If there is an atom missing from the array, a
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is an engineering measure of the maximum load a part of a specific material and geometry can withstand.
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Haasen, P. (1978). Physical metallurgy. Cambridge  ; New York: Cambridge University Press.
1185: 980: 962: 441: 56:, such as an indentation (over an area) or a scratch (linear), induced mechanically either by 38: 1204: 1131: 1095: 1068: 1041: 1006: 954: 894: 776: 594: 437: 348: 184: 93: 64:. In general, different materials differ in their hardness; for example hard metals such as 1266: 1241: 800: 734: 714: 586: 528: 411: 384: 364: 128: 569:
The movement allowed by these dislocations causes a decrease in the material's hardness.
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Hardness of a material to deformation is dependent on its microdurability or small-scale
1127: 1037: 950: 890: 597:, but this is readily obtained from a nominal stress – nominal strain curve (in the pre- 724: 687: 623: 536: 524: 433: 316: 248: 1208: 1255: 1143: 523:
The key to understanding the mechanism behind hardness is understanding the metallic
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Hashemi, SH (2011). "Strength-hardness statistical correlation in API X65 steel".
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it can absorb before fracturing, which is different from the amount of
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has allowed predicting hardness values with respect to composition.
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A representation of the crystal lattice showing the planes of atoms
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Measure of a material's resistance to localized plastic deformation
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Chinn, R. L. (2009). "Hardness, bearings, and the Rockwells".
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SI Metric Adaptation. Maidenhead, UK: McGraw-Hill Education.
371:, depending on the amount of force and the type of material: 634: 88:. Macroscopic hardness is generally characterized by strong 1215:
Revankar, G. (2003). "Introduction to hardness testing."
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Malzbender, J (2003). "Comment on hardness definitions".
288:. The device used to take this measurement is known as a 581:
Relation between hardness number and stress-strain curve
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Surface hardening of steels: Understanding the basics.
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when undergoing plastic deformation; this is called
292:. Two scales that measures rebound hardness are the 440:depending on the direction of the forces involved. 175:are used to convert between one scale and another. 815:"A guide to rebound hardness and scleroscope test" 100:, and rebound hardness. Hardness is dependent on 925:Introduction to materials science course manual 192:is the measure of how resistant a sample is to 26:"Softness" redirects here. For other uses, see 216:Another tool used to make these tests is the 8: 564:Planes of atoms split by an edge dislocation 507:and flaking in squamose or acicular habits. 367:, solids generally have three responses to 209:. One tool to make this measurement is the 383:in the case of a given object, or a high 910: 908: 1197:Journal of the European Ceramic Society 759: 461:of a material is the maximum amount of 1177:Materials Park, OH: ASM International. 1230:An introduction to materials hardness 135:. Common examples of hard matter are 7: 311:There are five hardening processes: 72:are harder than soft metals such as 49:) is a measure of the resistance to 472:Hardness increases with decreasing 347:, showing the relationship between 1163:Advanced Materials & Processes 351:(force applied per unit area) and 14: 1217:Mechanical testing and evaluation 853:Jeandron, Michelle (2005-08-25). 865:from the original on 2009-02-15. 699:Hardness scales, tools and tests 794:Hoffman Scratch Hardness Tester 421:—split into two or more pieces. 151:, which can be contrasted with 1247:Testing the Hardness of Metals 1235:Guidelines to hardness testing 959:10.1103/PhysRevLett.105.115503 667:Other strengthening mechanisms 1: 1209:10.1016/S0955-2219(02)00354-0 1046:10.1016/j.jnucmat.2004.09.024 487:in any direction, not to any 280:, measures the height of the 1173:Davis, J. R. (Ed.). (2002). 813:Allen, Robert (2006-12-10). 683:Solid solution strengthening 673:Grain boundary strengthening 321:solid solution strengthening 899:10.1103/PhysRevLett.83.5290 1303: 1180:Dieter, George E. (1989). 1100:10.1016/j.msea.2015.02.073 1073:10.1016/j.msea.2010.10.089 855:"Diamonds are not forever" 781:10.1016/j.wear.2008.05.014 705:Leeb rebound hardness test 387:in the case of a material. 329:martensitic transformation 304: 294:Leeb rebound hardness test 227: 182: 25: 18: 1136:10.1134/s0036029521130164 167:A Vickers hardness tester 1262:Condensed matter physics 591:von Mises plastic strain 313:Hall-Petch strengthening 19:Not to be confused with 710:Tablet hardness testing 678:Precipitation hardening 620:Ultimate Tensile Stress 611:Indentation Plastometry 495:properties such as its 478:Hall-Petch relationship 476:. This is known as the 325:precipitation hardening 1182:Mechanical Metallurgy. 1011:10.1002/srin.200100122 565: 520: 360: 307:Hardening (metallurgy) 218:pocket hardness tester 168: 603:Finite Element Method 563: 518: 511:Mechanisms and theory 342: 166: 32:Hard (disambiguation) 28:Soft (disambiguation) 1219:, ASM Online Vol. 8. 740:Barcol hardness test 720:Roll hardness tester 656:Hardness of ceramics 430:compressive strength 236:Indentation hardness 230:Indentation hardness 224:Indentation hardness 98:indentation hardness 90:intermolecular bonds 1287:Physical properties 1128:2021RuMet2021.1719M 1038:2005JNuM..336..267B 951:2010PhRvL.105k5503S 923:Samuel, J. (2009). 891:1999PhRvL..83.5290S 730:Janka hardness test 651:Hardness comparison 542:interstitial defect 400:stress-strain curve 345:stress-strain curve 205:, which is used in 198:plastic deformation 149:superhard materials 54:plastic deformation 1240:2021-02-25 at the 1116:Russian Metallurgy 1088:Mater. Sci. Eng. A 1061:Mater. Sci. Eng. A 799:2014-03-23 at the 640:Related properties 566: 521: 361: 359:of a ductile metal 335:In solid mechanics 263:, amongst others. 169: 1277:Materials science 1122:(13): 1719–1724. 750: 749: 442:Ultimate strength 267:Rebound hardness 173:conversion tables 39:materials science 1294: 1212: 1170: 1148: 1147: 1110: 1104: 1103: 1083: 1077: 1076: 1067:(3): 1648–1655. 1056: 1050: 1049: 1032:(2–3): 267–278. 1021: 1015: 1014: 994: 988: 977: 971: 970: 934: 928: 921: 915: 912: 903: 902: 873: 867: 866: 850: 844: 843: 836: 830: 829: 827: 826: 817:. Archived from 810: 804: 791: 785: 784: 764: 635: 595:von Mises stress 438:tensile strength 277:dynamic hardness 274:, also known as 272:Rebound hardness 190:Scratch hardness 185:Scratch hardness 179:Scratch hardness 94:scratch hardness 1302: 1301: 1297: 1296: 1295: 1293: 1292: 1291: 1272:Solid mechanics 1252: 1251: 1242:Wayback Machine 1226: 1194: 1160: 1157: 1155:Further reading 1152: 1151: 1112: 1111: 1107: 1085: 1084: 1080: 1058: 1057: 1053: 1023: 1022: 1018: 996: 995: 991: 978: 974: 939:Phys. Rev. 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Index

Hardiness
Soft (disambiguation)
Hard (disambiguation)
materials science
plastic deformation
pressing
abrasion
titanium
beryllium
sodium
tin
wood
plastics
intermolecular bonds
scratch hardness
indentation hardness
ductility
elastic
stiffness
plasticity
strain
strength
toughness
viscoelasticity
viscosity
ceramics
concrete
metals
superhard materials
soft matter

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