Thermography detection on the fatigue damage of the specimen alloy Essay

Thermography espial on the fatigue damage of the specimen alloy - Essay ExampleFatigue occurs when a substantial is subjected to periodic nisus which is below its tensile breaking or yield vehemence but which is tolerable to cause permanent damage. The formal definition of fatigue as given by Wikipedia (n.d.1) isFatigue is the progressive, localized, and permanent structural damage that occurs when a material is subjected to cyclic or fluctuating strains at nominal stresses that have uttermost values less than (often much less than) the static yield strength of the material.It is because fatigue happens so quiet and insidiously that makes it very dangerous even resulting in loss of life. Sadananda et al (2003) assert that Fatigue is the important cause of premature failure of engineering components.Many structures such as aeroplanes, oil rigs and bridges, to name plainly a few, are exposed to fluctuating stresses. The engineering approach falls into two broad categories of traffic with stress induced fatigue. The first part is prediction of the lifetime of a material under stress. This amaze will provide recommendations on how frequently materials have to be replaced. The second approach is to predict how farther a crack tummy grow before failure happens. Detection and prediction of failure of cracks can mean the difference between life and death of users of these facilities.The basic method o S-N CurvesThe basic method of presenting engineering fatigue data is by means of the S-N curve, a plot of stress S against the tot of cycles to failure N. ( Key to Steel, n.d.) The S-N curves enable prediction of how long a material will last in terms of cycles of payload. Figure 1. A S-N Plot for an aluminum alloy (Kelly, 1997)Kelly (1997) explains that cracks go through lead stages of formation, reference and failure.Stress Intensity factor KStress Intensity, K, is a parameter that amplifies the magnitude of the applied stress that includes the geometr ical parameter Y (load type) (Wikepedia, n.d.2). This factor measures the degree to which stress is magnified around a crack. The loading around a crack falls into three modes I, II and III.Figure 2. Three loading modes (Key to Steel, n.d.) The three modes are path 1 opening or tensile mode (the crack faces are pulled apart) Mode 2 sliding or in-plane shear (the crack surfaces slide over each other) Mode 3 tearing or anti-plane shear (the crack surfaces move parallel to the leading edge of the crack and copulation to each other)(Key to Steel, n.d.)The most common mode is mode I and this is what is used in most calculations. The bulk factor, K, determines the rate at which a crack will propagate and hence the lifetime of the material. The mathematical kind is defined by Callister (1994, cited by Kelly(1997)) asThis compare relates the rate of growth of a crack to the transport in intensity factor K. In this equation A and m are dependent on the materials and da is the change in crack length while dN is the change in number of stress cycles. The change in K is defined byWhere Kmax and Kmin are the maximum and minimum intensity factors respectively, Y is a constant dependent geometry of the material and is the applied stress on the material. When this equation is re-arranged and integrated it becomesThis equation gives Nf, the estimated number of cycles before