|
|
| (One intermediate revision by one other user not shown) |
| Line 1: |
Line 1: |
| {{Refimprove|date=August 2010}}
| | Last week I woke up and [http://lukebryantickets.omarfoundation.org vip luke bryan] realised - I have also been solitary for a while now and following much bullying from pals I today find myself registered for web dating. They promised me that there are a lot of entertaining, sweet and ordinary folks to fulfill, therefore here goes the pitch!<br>I endeavor to stay as physically fit as potential being at the gymnasium many times a week. I love my sports and strive to play or watch [http://www.cinemaudiosociety.org luke bryan presale tickets] because many a possible. Being wintertime I'll regularly at Hawthorn matches. Notice: I've [http://Browse.deviantart.com/?qh=§ion=&global=1&q=experienced experienced] the carnage of wrestling fits at stocktake revenue, Supposing that you considered shopping a hobby I really don't mind.<br>My household and pals are magnificent and spending time together at tavern gigabytes or meals is obviously a necessity. I have never been in to nightclubs as I realize you could do not get a significant dialog together with the sound. [http://www.google.co.uk/search?hl=en&gl=us&tbm=nws&q=I+additionally&gs_l=news I additionally] have 2 very adorable and unquestionably cheeky puppies who are invariably eager to meet fresh folks.<br><br> |
| [[Image:HoleForceLines.svg|thumb|right| Internal [[force lines]] are denser near the hole, a common [[stress concentration]]]] | |
|
| |
|
| '''Mechanics of materials''', also called '''strength of materials''', is a subject which deals with the behavior of solid objects subject to [[stress (physics)|stresses]] and [[strain (physics)|strains]]. The complete theory began with the consideration of the behavior of one and two dimensional members of structures, whose states of stress can be approximated as two dimensional, and was then generalized to three dimensions to develop a more complete theory of the elastic and plastic behavior of materials. An important founding pioneer in mechanics of materials was [[Stephen Timoshenko]].
| | My page :: luke bryan sold out - [http://lukebryantickets.hamedanshahr.com click the following web page], |
| | |
| The study of strength of materials often refers to various methods of calculating the stresses and strains in structural members, such as beams, columns, and shafts. The methods employed to predict the response of a structure under loading and its susceptibility to various failure modes takes into account the properties of the materials such as its [[yield strength]], [[ultimate strength]], [[Young's Modulus]], and [[Poisson's ratio]]; in addition the mechanical element's macroscopic properties (geometric properties), such as it length, width, thickness, boundary constraints and abrupt changes in geometry such as holes are considered.
| |
| | |
| ==Definition==
| |
| In materials science, the strength of a material is its ability to withstand an applied stress without failure.
| |
| The field of strength of materials deals with forces and deformations that result from their acting on a material.
| |
| A load applied to a mechanical member will induce internal forces within the member called stresses when those forces are expressed on a unit basis. The stresses acting on the material cause deformation of the material. Deformation of the material is called strain when those deformations too are placed on a unit basis.
| |
| The applied loads may be axial (tensile or compressive), or [[shear strength|shear]]. The stresses and strains that develop within a mechanical member must be calculated in order to assess the load capacity of that member. This requires a complete description of the geometry of the member, its constraints, the loads applied to the member and the properties of the material of which the member is composed. With a complete description of the loading and the geometry of the member, the state of stress and of state of strain at any point within the member can be calculated. Once the state of stress and strain within the member is known, the strength (load carrying capacity) of that member, its deformations (stiffness qualities), and its stability (ability to maintain its original configuration) can be calculated. The calculated stresses may then be compared to some measure of the strength of the member such as its material yield or ultimate strength. The calculated deflection of the member may be compared to a deflection criteria that is based on the member's use. The calculated buckling load of the member may be compared to the applied load. The calculated stiffness and mass distribution of the member may be used to calculate the member's dynamic response and then compared to the acoustic environment in which it will be used.
| |
| | |
| Material strength refers to the point on the engineering stress-strain curve (yield stress) beyond which the material experiences deformations that will not be completely reversed upon removal of the loading and as a result the member will have a permanent deflection. The ultimate strength refers to the point on the engineering stress-strain curve corresponding to the stress that produces fracture.
| |
| | |
| ===Types of loadings===
| |
| * Transverse loading - Forces applied perpendicular to the longitudinal axis of a member. Transverse loading causes the member to bend and deflect from its original position, with internal tensile and compressive strains accompanying the change in curvature of the member.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 210}}</ref> Transverse loading also induces shear forces that cause shear deformation of the material and increase the transverse deflection of the member.
| |
| * Axial loading - The applied forces are collinear with the longitudinal axis of the member. The forces cause the member to either stretch or shorten.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 7}}</ref>
| |
| * Torsional loading - Twisting action caused by a pair of externally applied equal and oppositely directed force couples acting on parallel planes or by a single external couple applied to a member that has one end fixed against rotation.
| |
| | |
| ===Stress terms===
| |
| [[Image:Compressive tensile shear loading.svg|thumb|A material being loaded in a) compression, b) tension, c) shear.]]
| |
| | |
| Uniaxial stress is expressed by
| |
| :<math> | |
| \sigma=\frac{F}{A},
| |
| </math>
| |
| where ''F'' is the force [N] acting on an area ''A'' [m<sup>2</sup>].<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 5}}</ref> The area can be the undeformed area or the deformed area, depending on whether [[Engineering stress#Stress in one-dimensional bodies|engineering stress]] or true stress is of interest.
| |
| | |
| *''[[Compressive stress]]'' (or [[compression (physical)|compression]]) is the stress state caused by an applied load that acts to reduce the length of the material ([[compression member]]) along the axis of the applied load, it is in other words a stress state that causes a squeezing of the material. A simple case of compression is the uniaxial compression induced by the action of opposite, pushing forces. Compressive strength for materials is generally higher than their tensile strength. However, structures loaded in compression are subject to additional failure modes, such as [[buckling]], that are dependent on the member's geometry.
| |
| | |
| *''[[Tensile stress]]'' is the stress state caused by an applied load that tends to elongate the material along the axis of the applied load, in other words the stress caused by ''pulling'' the material. The strength of structures of equal cross sectional area loaded in tension is independent of shape of the cross section. Materials loaded in tension are susceptible to [[stress concentration]]s such as material defects or abrupt changes in geometry. However, materials exhibiting ductile behavior (most metals for example) can tolerate some defects while brittle materials (such as ceramics) can fail well below their ultimate material strength.
| |
| | |
| *''[[Shear stress]]'' is the stress state caused by the combined energy of a pair of opposing forces acting along parallel lines of action through the material, in other words the stress caused by faces of the material ''sliding'' relative to one another. An example is cutting paper with [[scissor]]s<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 9–10}}</ref> or stresses due to torsional loading.
| |
| | |
| ===Strength terms===
| |
| *''[[Yield (engineering)|Yield strength]]'' is the lowest stress that produces a permanent deformation in a material. In some materials, like [[aluminium alloy]]s, the point of yielding is difficult to identify, thus it is usually defined as the stress required to cause 0.2% plastic strain. This is called a 0.2% proof stress.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 52}}</ref>
| |
| | |
| *''[[Compressive strength]]'' is a limit state of [[compressive stress]] that leads to failure in a material in the manner of ductile failure (infinite theoretical yield) or brittle failure (rupture as the result of crack propagation, or sliding along a weak plane - see [[shear strength]]).
| |
| | |
| *''[[Tensile strength]]'' or ''ultimate tensile strength'' is a limit state of [[tensile stress]] that leads to tensile failure in the manner of ductile failure (yield as the first stage of that failure, some hardening in the second stage and breakage after a possible "neck" formation) or brittle failure (sudden breaking in two or more pieces at a low stress state). Tensile strength can be quoted as either true stress or engineering stress, but engineering stress is the most commonly used.
| |
| | |
| *''[[Fatigue (material)|Fatigue strength]]'' is a measure of the strength of a material or a component under cyclic loading,<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 60}}</ref> and is usually more difficult to assess than the static strength measures. Fatigue strength is quoted as stress amplitude or stress range (<math>\Delta\sigma= \sigma_\mathrm{max} - \sigma_\mathrm{min}</math>), usually at zero mean stress, along with the number of cycles to failure under that condition of stress.
| |
| | |
| *''[[Impact resistance|Impact strength]]'', is the capability of the material to withstand a suddenly applied load and is expressed in terms of energy. Often measured with the [[Izod impact strength test]] or [[Charpy impact test]], both of which measure the impact energy required to fracture a sample. Volume, modulus of [[Elasticity (physics)|elasticity]], distribution of forces, and yield strength affect the impact strength of a material. In order for a material or object to have a high impact strength the stresses must be distributed evenly throughout the object. It also must have a large volume with a low modulus of elasticity and a high material yield strength.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 693–696}}</ref>
| |
| | |
| ===Strain (deformation) terms===
| |
| *''[[Deformation (engineering)|Deformation]]'' of the material is the change in geometry created when stress is applied (as a result of applied forces, gravitational fields, accelerations, thermal expansion, etc.). Deformation is expressed by the displacement field of the material.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 47}}</ref>
| |
| *''[[Strain (materials science)|Strain]]'' or ''reduced deformation'' is a mathematical term that expresses the trend of the deformation change among the material field. Strain is the deformation per unit length.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 49}}</ref> In the case of uniaxial loading the displacements of a specimen (for example a bar element)lead to a calculation of strain expressed as the quotient of the displacement and the original length of the specimen. For 3D displacement fields it is expressed as derivatives of displacement functions in terms of a second order [[tensor]] (with 6 independent elements).
| |
| *''[[Deflection (engineering)|Deflection]]'' is a term to describe the magnitude to which a structural element is displaced when subject to an applied load.<ref>{{cite book
| |
| | title = Structural Analysis
| |
| | author = R. C. Hibbeler
| |
| | publisher = Pearson Prentice Hall
| |
| | year = 2009
| |
| | edition = 7
| |
| | isbn = 978-0-13-602060-8
| |
| | pages = 305}}</ref>
| |
| | |
| ===Stress-strain relations===
| |
| [[File:Tension test.svg|thumb|300px|Basic static response of a specimen under tension]]
| |
| *''[[Elasticity (physics)|Elasticity]]'' is the ability of a material to return to its previous shape after stress is released. In many materials, the relation between applied stress is directly proportional to the resulting strain (up to a certain limit), and a graph representing those two quantities is a straight line.
| |
| The slope of this line is known as [[Young's Modulus]], or the "Modulus of Elasticity." The Modulus of Elasticity can be used to determine the stress-strain relationship in the linear-elastic portion of the stress-strain curve. The linear-elastic region is either below the yield point, or if a yield point is not easily identified on the stress-strain plot it is defined to be between 0 and 0.2% strain, and is defined as the region of strain in which no yielding (permanent deformation) occurs.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 53–56}}</ref>
| |
| | |
| *''[[Plasticity (physics)|Plasticity]]'' or plastic deformation is the opposite of elastic deformation and is defined as unrecoverable strain. Plastic deformation is retained after the release of the applied stress. Most materials in the linear-elastic category are usually capable of plastic deformation. Brittle materials, like ceramics, do not experience any plastic deformation and will fracture under relatively low stress. Materials such as metals usually experience a small amount of plastic deformation before failure while ductile metals such as copper and lead or polymers will plasticly deform much more.
| |
| | |
| Consider the difference between a carrot and chewed bubble gum. The carrot will stretch very little before breaking. The chewed bubble gum, on the other hand, will plastically deform enormously before finally breaking.
| |
| | |
| ==Design terms==
| |
| Ultimate strength is an attribute related to a material, rather than just a specific specimen made of the material, and as such it is quoted as the force per unit of cross section area (N/m<sup>2</sup>). The ultimate strength is the maximum stress that a material can withstand before it breaks or weakens.<ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 27–28}}</ref> For example, the ultimate tensile strength (UTS) of AISI 1018 Steel is 440 [[meganewton|MN]]/m<sup>2</sup>. In general, the SI unit of stress is the [[pascal (unit)|pascal]], where 1 Pa = 1 N/m<sup>2</sup>. In Imperial units, the unit of stress is given as lbf/in² or [[pounds-force per square inch]]. This unit is often abbreviated as '''psi'''. One thousand psi is abbreviated '''ksi'''.
| |
| | |
| A [[Factor of safety]] is a design criteria that an engineered component or structure must achieve. <math>FS = UTS/R</math>, where FS: the factor of safety, R: The applied stress, and UTS: ultimate stress (psi or N/m<sup>2</sup>) <ref>{{cite book
| |
| | title = Mechanics of Materials
| |
| | author = Beer & Johnston
| |
| | publisher = McGraw Hill
| |
| | year = 2006
| |
| | edition = 5th
| |
| | isbn = 978-0-07-352938-7
| |
| | pages = 28}}</ref>
| |
| | |
| Margin of Safety is also sometimes used to as design criteria. It is defined MS = Failure Load/(Factor of Safety * Predicted Load) - 1
| |
| | |
| For example to achieve a factor of safety of 4, the allowable stress in an AISI 1018 steel component can be calculated to be <math>R = UTS/FS</math> = 440/4 = 110 MPa, or <math>R</math> = 110×10<sup>6</sup> N/m<sup>2</sup>. Such allowable stresses are also known as "design stresses" or "working stresses."
| |
| | |
| Design stresses that have been determined from the ultimate or yield point values of the materials give safe and reliable results only for the case of static loading. Many machine parts fail when subjected to a non steady and continuously varying loads even though the developed stresses are below the yield point. Such failures are called fatigue failure. The failure is by a fracture that appears to be brittle with little or no visible evidence of yielding. However, when the stress is kept below "fatigue stress" or "endurance limit stress", the part will endure indefinitely. A purely reversing or cyclic stress is one that alternates between equal positive and negative peak stresses during each cycle of operation. In a purely cyclic stress, the average stress is zero. When a part is subjected to a cyclic stress, also known as stress range (Sr), it has been observed that the failure of the part occurs after a number of stress reversals (N) even if the magnitude of the stress range is below the material’s yield strength. Generally, higher the range stress, the fewer the number of reversals needed for failure.
| |
| | |
| ===Failure theories===
| |
| | |
| There are four important failure theories: maximum shear stress theory, maximum normal stress theory, maximum strain energy theory, and maximum distortion energy theory. Out of these four theories of failure, the maximum normal stress theory is only applicable for brittle materials, and the remaining three theories are applicable for ductile materials.
| |
| Of the latter three, the distortion energy theory provides most accurate results in majority of the stress conditions. The strain energy theory needs the value of Poisson’s ratio of the part material, which is often not readily available. The maximum shear stress theory is conservative. For simple unidirectional normal stresses all theories are equivalent, which means all theories will give the same result.
| |
| | |
| *Maximum Shear stress Theory- This theory postulates that failure will occur if the magnitude of the maximum shear stress in the part exceeds the shear strength of the material determined from uniaxial testing.
| |
| | |
| *Maximum normal stress theory - This theory postulates that failure will occur if the maximum normal stress in the part exceeds the ultimate tensile stress of the material as determined from uniaxial testing. This theory deals with brittle materials only. The maximum tensile stress should be less than or equal to ultimate tensile stress divided by factor of safety. The magnitude of the maximum compressive stress should be less than ultimate compressive stress divided by factor of safety.
| |
| | |
| *Maximum strain energy theory - This theory postulates that failure will occur when the strain energy per unit volume due to the applied stresses in a part equals the strain energy per unit volume at the yield point in uniaxial testing.
| |
| | |
| *Maximum distortion energy theory - This theory is also known as shear energy theory or [[Von Mises yield criterion|von Mises-Hencky theory]]. This theory postulates that failure will occur when the distortion energy per unit volume due to the applied stresses in a part equals the distortion energy per unit volume at the yield point in uniaxial testing. The total elastic energy due to strain can be divided into two parts: one part causes change in volume, and the other part causes change in shape. Distortion energy is the amount of energy that is needed to change the shape.
| |
| | |
| *Fracture mechanics was established by Alan Arnold Griffith and George Rankine Irwin. This important theory is also known as numeric conversion of toughness of material in the case of crack existence.
| |
| | |
| * Fractology was proposed by Takeo Yokobori because each fracure laws including creep rupture criterion must be combined nonlinially.
| |
| | |
| ==Microstructure==
| |
| | |
| A material's strength is dependent on its [[microstructure]]. The engineering processes to which a material is subjected can alter this microstructure. The variety of [[strengthening mechanisms of materials|strengthening mechanisms]] that alter the strength of a material includes [[work hardening]], [[solid solution strengthening]], [[precipitation hardening]] and [[grain boundary strengthening]] and can be quantitatively and qualitatively explained. Strengthening mechanisms are accompanied by the caveat that some other mechanical properties of the material may degenerate in an attempt to make the material stronger. For example, in grain boundary strengthening, although [[yield strength]] is maximized with decreasing grain size, ultimately, very small grain sizes make the material brittle. In general, the yield strength of a material is an adequate indicator of the material's mechanical strength. Considered in tandem with the fact that the yield strength is the parameter that predicts [[plastic deformation]] in the material, one can make informed decisions on how to increase the strength of a material depending its microstructural properties and the desired end effect. Strength is expressed in terms of the limiting values of the [[compressive stress]], [[tensile stress]], and [[shear stress]]es that would cause failure. The effects of dynamic loading are probably the most important practical consideration of the strength of materials, especially the problem of [[fatigue (material)|fatigue]]. Repeated loading often initiates [[brittle]] cracks, which grow until failure occurs. The cracks always start at [[stress concentration]]s, especially changes in cross-section of the product, near holes and corners at nominal stress levels far lower than those quoted for the strength of the material.
| |
| | |
| ==See also==
| |
| {{colbegin|3}}
| |
| * [[Creep of materials]]
| |
| * [[Deformation-mechanism maps]]
| |
| * [[Diffusion in materials]]
| |
| * [[Dynamics (mechanics)|Dynamics]]
| |
| * [[Fatigue of materials]]
| |
| * [[Forensic engineering]]
| |
| * [[Fracture mechanics]]
| |
| * [[Fracture toughness]]
| |
| * [[Material selection]]
| |
| * [[Specific strength]]
| |
| * [[Statics]]
| |
| *[[Universal testing machine]]
| |
| {{colend}}
| |
| | |
| ==References==
| |
| {{Reflist}}
| |
| | |
| ==Further reading==
| |
| {{colbegin}}
| |
| *Fa-Hwa Cheng, Initials. (1997). Strength of material. Ohio: McGraw-Hill
| |
| * Mechanics of Materials, E.J. Hearn
| |
| * Alfirević, Ivo. ''Strength of Materials I''. Tehnička knjiga, 1995. ISBN 953-172-010-X.
| |
| * Alfirević, Ivo. ''Strength of Materials II''. Tehnička knjiga, 1999. ISBN 953-6168-85-5.
| |
| * [[M. F. Ashby|Ashby, M.F.]] ''Materials Selection in Design''. Pergamon, 1992.
| |
| * Beer, F.P., E.R. Johnston, et al. ''Mechanics of Materials'', 3rd edition. McGraw-Hill, 2001. ISBN 0-07-248673-2
| |
| * Cottrell, A.H. ''Mechanical Properties of Matter''. Wiley, New York, 1964.
| |
| * Den Hartog, Jacob P. ''Strength of Materials''. Dover Publications, Inc., 1961, ISBN 0-486-60755-0.
| |
| * Drucker, D.C. ''Introduction to Mechanics of Deformable Solids''. McGraw-Hill, 1967.
| |
| * [[J.E. Gordon|Gordon, J.E.]] ''The New Science of Strong Materials''. Princeton, 1984.
| |
| * Groover, Mikell P. ''Fundamentals of Modern Manufacturing'', 2nd edition. John Wiley & Sons,Inc., 2002. ISBN 0-471-40051-3.
| |
| * Hashemi, Javad and William F. Smith. ''Foundations of Materials Science and Engineering'', 4th edition. McGraw-Hill, 2006. ISBN 0-07-125690-3.
| |
| * Hibbeler, R.C. ''Statics and Mechanics of Materials'', SI Edition. Prentice-Hall, 2004. ISBN 0-13-129011-8.
| |
| * Lebedev, Leonid P. and Michael J. Cloud. ''Approximating Perfection: A Mathematician's Journey into the World of Mechanics''. Princeton University Press, 2004. ISBN 0-691-11726-8.
| |
| *[http://dx.doi.org/10.1016/B978-0-12-394584-6.00010-8 Chapter 10 – Strength of Elastomers], A.N. Gent, W.V. Mars, In: James E. Mark, Burak Erman and Mike Roland, Editor(s), The Science and Technology of Rubber (Fourth Edition), Academic Press, Boston, 2013, Pages 473-516, ISBN 9780123945846, 10.1016/B978-0-12-394584-6.00010-8
| |
| * Mott, Robert L. ''Applied Strength of Materials'', 4th edition. Prentice-Hall, 2002. ISBN 0-13-088578-9.
| |
| * Popov, Egor P. ''Engineering Mechanics of Solids''. Prentice Hall, Englewood Cliffs, N. J., 1990. ISBN 0-13-279258-3.
| |
| * Ramamrutham, S. ''Strength of Materials''.
| |
| * Shames, I.H. and F.A. Cozzarelli. ''Elastic and inelastic stress analysis''. Prentice-Hall, 1991. ISBN 1-56032-686-7.
| |
| * [[Stephen Timoshenko|Timoshenko S.]] ''Strength of Materials'', 3rd edition. Krieger Publishing Company, 1976, ISBN 0-88275-420-3.
| |
| * Timoshenko, S.P. and D.H. Young. ''Elements of Strength of Materials'', 5th edition. (MKS System)
| |
| *Davidge, R.W., Mechanical Behavior of Ceramics, Cambridge Solid State Science Series, (1979)
| |
| *Lawn, B.R., Fracture of Brittle Solids, Cambridge Solid State Science Series, 2nd Edn. (1993)
| |
| *Green, D., An Introduction to the Mechanical Properties of Ceramics, Cambridge Solid State Science Series, Eds. Clarke, D.R., Suresh, S., Ward, I.M.Babu Tom.K (1998)
| |
| {{colend}}
| |
| | |
| ==External links==
| |
| *[http://www.mech.uwa.edu.au/DANotes/SSS/failure/theories.html Failure theories]
| |
| *[http://materials.open.ac.uk/mem/index.htm case studies in structural failure]
| |
| | |
| {{Use dmy dates|date=January 2011}}
| |
| | |
| {{DEFAULTSORT:Strength Of Materials}}
| |
| [[Category:Solid mechanics]]
| |
| [[Category:Materials science]]
| |
| [[Category:Building engineering]]
| |
| [[Category:Deformation]]
| |
| | |
| [[ca:Resistència dels materials]]
| |
| [[uk:Опір матеріалів]]
| |
| [[vi:Độ bền vật liệu]]
| |
