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Mechanical Properties of Metals


The mechanical properties of metals determine the range of usefulness of the metal and establish the service that can be expected. Mechanical properties are also used to help specify and identify metals. The most common properties considered are strength, hardness, ductility, and impact resistance.

The mechanical properties of metals determine the range of usefulness of the metal and establish the service that can be expected. Mechanical properties are also used to help specify and identify metals. The most common properties considered are strength, hardness, ductility, and impact resistance.


The strength of a metal is its ability to withstand the action of external forces without breaking. Tensile strength, also called ultimate strength, is the maximum strength developed in a metal in a tension test. The tension test is a method for determining the behavior of a metal under an actual stretch loading. This test provides the elastic limit, elongation, yield point, yield strength, tensile strength, and the reduction in area. Tensile tests are normally taken at standardized room temperatures but may also be made at elevated temperatures.

Many tensile testing machines are equipped to plot a curve which shows the load or stress and the strain or movement that occurs during the test operation. In the testing operation the load is increased gradually and the specimen will stretch or elongate in proportion to the tensile load.

The specimen will elongate in direct proportion to the load during the elastic portion of the curve to point A. At this point, the specimen will continue to elongate but without an increase in the load. This is known as the yield point of the steel and is the end of the elastic portion. At any point up to point A if the load is eliminated, the specimen will come back to its original dimension.

Yielding occurs from point A to point B and this is the area of plastic deformation. If the load were eliminated at point B the specimen would not go back to its original dimension but instead take a permanent set. Beyond point B the load will have to be increased to further stretch the specimen.

The load will increase to point C, which is the ultimate strength of the material. At point C the specimen will break and the load is no longer carried. The ultimate tensile strength of the material is obtained by dividing the ultimate load by the cross-sectional area of the original specimen. This provides the ultimate tensile strength in Newtons per square millimeter (Mega Pascals, MPa) or pounds per square inch.

The yield stress or yield point is obtained by dividing the load at yield or at point A by the original area. This provides a figure in pounds per square inch or MPa. Extremely ductile metals do not have a yield point. They stretch or yield at low loads. For these metals the yield point is determined by the change in elongation. Two tenths of one percent elongation is arbitrarily set as the yield point. The yield point is the limit upon which designs are calculated.


The ductility of a metal is the property that allows it to be stretched or otherwise changed in shape without breaking and to retain the changed shape after the load has been removed.

The ductility of a metal can be determined from the tensile test. This is done by determining the percent of elongation. Gauge marks are made two inches apart across the point where fracture will occur. The increase in gauge length related to the original length times 100 is the percentage of elongation. This is done by making center punch marks two inches apart at the reduced section of the test coupon, testing the coupon, tightly holding the two pieces together and re-measuring the distance between the center punch marks. The original two inches is subtracted from the measured length and the difference is divided by two and multiplied by 100 to obtain percentage of elongation.

Reduction of Area

Reduction of area is another measure of ductility and is obtained from the tensile test by measuring the original cross-sectional area of the specimen and relating it to the cross-sectional area after failure.

For a round specimen the diameter is measured and the cross-sectional area is calculated. After the test bar is broken the diameter is measured at the smallest point. The cross-sectional area is again calculated. The difference in area is divided by the original area and multiplied by 100 to give the percentage reduction of area. This figure is of less importance than the elongation but is usually reported when the mechanical properties of a metal are given.

The tensile test specimen also provides another property of metal known as its modulus of elasticity, also called Young`s modulus. This is the ratio of the stress to the elastic strain. It relates to the slope of the curve to the yield point. The modulus of elasticity is important to the designers and is incorporated in many design formulas.


The hardness of a metal is defined as the resistance of a metal to local penetration by harder substance. The hardness of metals is measured by forcing a hardened steel ball or diamond into the surface of the specimen, under a definite weight, in a hardness testing machine.

The Brinell is one of the more popular types of machines for measuring hardness. It provides a Brinell hardness number (BHN), which is in kilograms per square millimeter based on the load applied to the hardened ball in kilograms and divided by the area of the impression left by the ball in square millimeters.

There is several other hardness measuring systems. A popular machine is the Rockwell hardness tester, which utilizes a diamond that is forced into the surface of the specimen. Different loads are used to provide different scaled. Smaller loads are used for softer materials. Another method is by means of the Vickers hardness machine, which reads directly, as a diamond is pressed into the surface of the metal. Another way is the Shore scleroscope, which utilizes a small dropped weight which will bounce from the surface of the metal providing a hardness measure.

Impact Resistance

Resistance of a metal to impacts is evaluated in terms of impact strength. A metal may possess satisfactory ductility under static loads but may fail under dynamic loads or impact.

Impact strength is most often determined by the Charpy test. It is sometimes measured by the Izode test. Both types of tests use the same type of pendulum-testing machine. The Charpy test specimen is a beam supported at both ends and contains a notch in the center. The specimen is placed on supports and struck with a pendulum on the side opposite the notch. The accuracy and location of the notch is of extreme importance. There are several types of Charpy specimens; the V-notch type is the most popular.

The impact strength of a metal is determined by measuring the energy absorbed in the fracture. This is equal to the weight of the pendulum times the height at which the pendulum is released and the height to which the pendulum swings after it has struck the specimen. In standard metric practice, impact resistance is measured two ways. One, in Joules based on energy absorbed and, two, in Joules per square centimeter of the area of the fractured surface or the cross-sectional area under the notch. In Anglo-Saxon terms the impact strength is the foot pounds of energy absorbed.

Total Materia has mechanical properties inserted for many thousands of materials and accessing them is just a click of a button away.

Covering a wide variety of property information, it is easy to find yield stress, tensile stress and elongation data for a huge number of materials within the database.

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The mechanical properties data will be displayed for all available conditions and treatments.

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