'Hardness' refers to various properties of
matter in the
solid phase that give it high resistance to various kinds of shape change when
force is applied. 'Hard matter' is contrasted with
soft matter.
Macroscopic hardness is generally characterized by strong
intermolecular bonds. However, the behavior of solid materials under force is complex, resulting in several different scientific definitions of what might be called "hardness" in everyday usage.
In
materials science, there are three principal
operational definitions of hardness:
★ 'Scratch hardness' - Resistance to
fracture or plastic (permanent)
deformation due to friction from a sharp object
★
Indentation hardness - Resistance to plastic (permanent)
deformation due to impact from a sharp object
★ 'Rebound hardness' - Height of the bounce of an object dropped on the material, related to
elasticity.
In physics, hardness encompasses:
★
Elasticity,
plasticity,
viscosity, and
viscoelasticity
★
Strength and
strain
★
Brittleness/
ductility and
toughness
Materials science
In
materials science, 'hardness' is the characteristic of a
solid material expressing its resistance to permanent deformation. Hardness can be measured on the
Mohs scale or various other scales. Some of the other scales used for indentation hardness in engineering -
Rockwell,
Vickers, and
Brinell - can be compared using
practical conversion tables.
Scratch hardness
In
mineralogy, ''hardness'' commonly refers to a material's ability to penetrate softer materials. An object made of a ''hard'' material will scratch an object made of a ''softer'' material. Scratch hardness is usually measured on the
Mohs scale of mineral hardness. One tool to make this measurement is the
sclerometer.
Pure
diamond is the hardest known natural mineral substance and will scratch any other natural material. Diamond is therefore used to cut other diamonds; in particular, higher-grade diamonds are used to cut lower-grade diamonds.
The hardest substance known today is
aggregated diamond nanorods, with a hardness 1.11 times diamond. Estimates from proposed molecular structure indicate the hardness of
beta carbon nitride should also be greater than diamond (but less than
ultrahard fullerite). This material has not yet been successfully synthesized.
Indentation hardness

A Vickers hardness tester
Main articles: Indentation hardness
Primarily used in
engineering and
metallurgy, indentation hardness seeks to characterise a material's hardness; i.e. its resistance to permanent, and in particular
plastic, deformation. It is usually measured by loading an indenter of specified geometry onto the material and measuring the dimensions of the resulting indentation.
There are several alternative definitions of indentation hardness, the most common of which are
★
Brinell hardness test (HB);
★
Janka Wood Hardness Rating;
★
Knoop hardness test (HK) or microhardness test, for measurement over small areas;
★
Meyer hardness test;
★
Rockwell hardness test (HR), principally used in the
USA;
★
Shore durometer hardness, used for polymers;
★
Vickers hardness test (HV), has one of the widest scales;
★
Barcol hardness test, for composite materials, scale from 0 to 100.
There is, in general, no simple relationship between the results of different hardness tests. Though there are
practical conversion tables for hard steels, for example, some materials show qualitatively different behaviours under the various measurement methods.
Hardness increases with decreasing
particle size. This is known as the
Hall-Petch effect. However, below a critical grain-size, hardness decreases with decreasing grain size. This is known as the inverse Hall-Petch effect.
For measuring hardness of nanograined materials,
nanoindentation is used.
In the
December 4,
2005 issue of
The Jerusalem Post, Professors Eli Altus, Harold Basch and Shmaryahu Hoz, with doctoral student Lior Itzhaki
reported the discovery of a
polyyne that is 40 times harder than diamond. It is a "superhard" molecular rod, comprised of
acetylene units.
It is important to note that hardness of a material to deformation is dependent to its microdurability or small-scale
shear modulus in any direction, not to any rigidity or stiffness properties such as the
bulk modulus or
Young's modulus. Scientists and journalists often confuse stiffness for hardness
[1][2], and spuriously report materials that are not actually harder than diamond because the
anisotropy of their solid cells compromise hardness in other dimensions, resulting in a material prone to
spalling and flaking in squamose or acicular habits in that dimension. e.g.,
Osmium is stiffer than diamond but is as hard as
quartz. In other words, a claimed hard material should have similar hardness characteristics at any location on its surface.
Rebound hardness
Also known as ''dynamic hardness'', rebound hardness measures the height of the "bounce" of a diamond-tipped hammer dropped from a fixed height onto a material. The device used to take this measurement is known as a
scleroscope.
[3]
One scale that measures rebound hardness is the
Bennett Hardness Scale.
Physics
In
solid mechanics, solids generally have three responses to
force, depending on the amount of force and the type of material:
★ They exhibit
elasticity - 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
stiffness in the case of a given object, or a high
elastic modulus in the case of a material.
★ They exhibit
plasticity - the ability to permanently change shape in response to the force, but remain in one piece. The
yield strength 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
stress-strain curve. This response produces the observed properties of scratch and indentation hardness, as described and measured in materials science. Some materials exhibit both
elasticity and
viscosity when undergoing plastic deformation; this is called
viscoelasticity.
★ They
fracture - split into two or more pieces. The "ultimate strength" or
toughness of an object is the point at which fracture occurs.
Strength is a measure of the extent of a material's elastic range, or elastic and plastic ranges together. This is quantified as
compressive strength,
shear strength,
tensile strength depending on the direction of the forces involved.
Ultimate strength is measure of the maximum
strain a material can withstand.
Brittleness, in technical usage, is the tendency of a material to fracture with very little or no detectable 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 brittle materials, yield strength and ultimate strength are the same, because they do not experience detectable plastic deformation. The opposite of brittleness is
ductility.
The
toughness of a material is the maximum amount of
energy it can absorb before fracturing, which is different than the amount of
force that can be applied. Toughness tends to be small for brittle materials, because it is elastic and plastic deformations that allow materials to absorb large amounts of energy.
Materials whose properties are different in different directions (because of an asymmetrical
crystal structure) are referred to as
anisotropic.
Examples of hard matter
★
Ceramics
★
Composites
★
Metals
★
Semiconductors
External links
★
An introduction to materials hardness
References
1. "Diamonds are not forever": "The hardness of a material is measured by its isothermal bulk modulus." (2005).
2. "Hard as a Diamond?": "..bulk modulus would be surpassed only by diamond; and if combined with some impurity atoms to fill in the voids, it might be even harder than diamond." (1999).
3. [1]
Materials science:
★
Mechanical Metallurgy, , George E., Dieter,, McGraw-Hill Education, 1989,
★
Comment on hardness definitions, , J, Malzbender, Journal of the European Ceramics Society, 2003