Knowledge (XXG)

Hardness

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461:, 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 231:. 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. 584:
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
572: 527: 351: 175: 633:(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 538:, 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 587:
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
542:. 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. 560:
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".
390:—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 182:
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
258:. 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 612:
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.
1248: 413:. This response produces the observed properties of scratch and indentation hardness, as described and measured in materials science. Some materials exhibit both 409:
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".
514:. Stiffness is often confused for hardness. Some materials are stiffer than diamond (e.g. osmium) but are not harder, and are prone to 491:. However, below a critical grain-size, hardness decreases with decreasing grain size. This is known as the inverse Hall-Petch effect. 829: 1272: 1200: 600:, captures the full plasticity response of the material (which is in most cases a metal). It is in fact a dependence of the (true) 616:(FEM). This applies to the outcome of an indentation test (with a given size and shape of indenter, and a given applied load). 1257: 995: 103:, but the behavior of solid materials under force is complex; therefore, hardness can be measured in different ways, such as 873: 1297: 1245: 693: 683: 439:
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.
1196: 991: 973: 452: 67:, such as an indentation (over an area) or a scratch (linear), induced mechanically either by 49: 1215: 1142: 1106: 1079: 1052: 1017: 965: 905: 787: 605: 448: 359: 195: 104: 75:. In general, different materials differ in their hardness; for example hard metals such as 1277: 1252: 811: 745: 725: 597: 539: 422: 395: 375: 139: 580:
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
1138: 1048: 961: 901: 608:, but this is readily obtained from a nominal stress – nominal strain curve (in the pre- 735: 698: 634: 547: 535: 444: 327: 259: 1219: 1266: 1154: 534:
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.
382:, depending on the amount of force and the type of material: 645: 99:. Macroscopic hardness is generally characterized by strong 1226:
Revankar, G. (2003). "Introduction to hardness testing."
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Malzbender, J (2003). "Comment on hardness definitions".
299:. The device used to take this measurement is known as a 592:
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
303:. Two scales that measures rebound hardness are the 451:depending on the direction of the forces involved. 186:are used to convert between one scale and another. 826:"A guide to rebound hardness and scleroscope test" 111:, and rebound hardness. Hardness is dependent on 936:Introduction to materials science course manual 203:is the measure of how resistant a sample is to 37:"Softness" redirects here. For other uses, see 227:Another tool used to make these tests is the 8: 575:Planes of atoms split by an edge dislocation 518:and flaking in squamose or acicular habits. 378:, solids generally have three responses to 220:. One tool to make this measurement is the 394:in the case of a given object, or a high 921: 919: 1208:Journal of the European Ceramic Society 770: 472:of a material is the maximum amount of 1188:Materials Park, OH: ASM International. 1241:An introduction to materials hardness 146:. Common examples of hard matter are 7: 322:There are five hardening processes: 83:are harder than soft metals such as 60:) is a measure of the resistance to 483:Hardness increases with decreasing 358:, showing the relationship between 1174:Advanced Materials & Processes 362:(force applied per unit area) and 25: 1228:Mechanical testing and evaluation 864:Jeandron, Michelle (2005-08-25). 876:from the original on 2009-02-15. 710:Hardness scales, tools and tests 805:Hoffman Scratch Hardness Tester 432:—split into two or more pieces. 162:, which can be contrasted with 1258:Testing the Hardness of Metals 1246:Guidelines to hardness testing 970:10.1103/PhysRevLett.105.115503 678:Other strengthening mechanisms 1: 1220:10.1016/S0955-2219(02)00354-0 1057:10.1016/j.jnucmat.2004.09.024 498:in any direction, not to any 291:, measures the height of the 1184:Davis, J. R. (Ed.). (2002). 824:Allen, Robert (2006-12-10). 694:Solid solution strengthening 684:Grain boundary strengthening 332:solid solution strengthening 910:10.1103/PhysRevLett.83.5290 1314: 1191:Dieter, George E. (1989). 1111:10.1016/j.msea.2015.02.073 1084:10.1016/j.msea.2010.10.089 866:"Diamonds are not forever" 792:10.1016/j.wear.2008.05.014 716:Leeb rebound hardness test 398:in the case of a material. 340:martensitic transformation 315: 305:Leeb rebound hardness test 238: 193: 36: 29: 1147:10.1134/s0036029521130164 178:A Vickers hardness tester 1273:Condensed matter physics 602:von Mises plastic strain 324:Hall-Petch strengthening 30:Not to be confused with 721:Tablet hardness testing 689:Precipitation hardening 631:Ultimate Tensile Stress 622:Indentation Plastometry 506:properties such as its 489:Hall-Petch relationship 487:. This is known as the 336:precipitation hardening 1193:Mechanical Metallurgy. 1022:10.1002/srin.200100122 576: 531: 371: 318:Hardening (metallurgy) 229:pocket hardness tester 179: 614:Finite Element Method 574: 529: 522:Mechanisms and theory 353: 177: 43:Hard (disambiguation) 39:Soft (disambiguation) 1230:, ASM Online Vol. 8. 751:Barcol hardness test 731:Roll hardness tester 667:Hardness of ceramics 441:compressive strength 247:Indentation hardness 241:Indentation hardness 235:Indentation hardness 109:indentation hardness 101:intermolecular bonds 1298:Physical properties 1139:2021RuMet2021.1719M 1049:2005JNuM..336..267B 962:2010PhRvL.105k5503S 934:Samuel, J. (2009). 902:1999PhRvL..83.5290S 741:Janka hardness test 662:Hardness comparison 553:interstitial defect 411:stress-strain curve 356:stress-strain curve 216:, which is used in 209:plastic deformation 160:superhard materials 65:plastic deformation 1251:2021-02-25 at the 1127:Russian Metallurgy 1099:Mater. Sci. Eng. A 1072:Mater. Sci. Eng. A 810:2014-03-23 at the 651:Related properties 577: 532: 372: 370:of a ductile metal 346:In solid mechanics 274:, amongst others. 180: 1288:Materials science 1133:(13): 1719–1724. 761: 760: 453:Ultimate strength 278:Rebound hardness 184:conversion tables 50:materials science 16:(Redirected from 1305: 1223: 1181: 1159: 1158: 1121: 1115: 1114: 1094: 1088: 1087: 1078:(3): 1648–1655. 1067: 1061: 1060: 1043:(2–3): 267–278. 1032: 1026: 1025: 1005: 999: 988: 982: 981: 945: 939: 932: 926: 923: 914: 913: 884: 878: 877: 861: 855: 854: 847: 841: 840: 838: 837: 828:. Archived from 821: 815: 802: 796: 795: 775: 646: 606:von Mises stress 449:tensile strength 288:dynamic hardness 285:, also known as 283:Rebound hardness 201:Scratch hardness 196:Scratch hardness 190:Scratch hardness 105:scratch hardness 21: 18:Hardness testing 1313: 1312: 1308: 1307: 1306: 1304: 1303: 1302: 1283:Solid mechanics 1263: 1262: 1253:Wayback Machine 1237: 1205: 1171: 1168: 1166:Further reading 1163: 1162: 1123: 1122: 1118: 1096: 1095: 1091: 1069: 1068: 1064: 1034: 1033: 1029: 1007: 1006: 1002: 989: 985: 950:Phys. Rev. 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Index

Hardness testing
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

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