• Determination Of The Characteristic Strength Properties Of Mild Steel Reinforcement
    [A CASE STUDY OF ILORIN METROPOLIS]

  • CHAPTER TWO -- [Total Page(s) 10]

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    • 2.7.2 CREEP
      At elevated temperatures a metal in tension will continue to elongate under a constant stress which may be much less than the ultimate tensile stress. This phenomenon is called ‘creep’ and is measured by the rate of strain per hour under a certain stress at a given temperature.
      If a ‘short time’ tensile test is carried out on a metal specimen at a specific temperature a fairly definite ultimate stress is obtained. The material may be made to fail by creep under a lower stress, however, provided sufficient time is allowed the rate of creep depending on the stress. At any temperature there is a limiting stress below which creep will not take place, i.e. the metal will not fractures if the stress is applied for an indefinite period.
      This limiting creep stress may frequently be less than half the ultimate stress obtained in a normal test at that temperature. in designing any part which is stressed at high temperatures it is clearly necessary to base the working stress on the limiting creep stress.
      2.7.3 COMPRESSION TEST
      Specimens for compression tests on metals are usually circular, and for concrete square, in section. To prevent failure by buckling, the length should be of about the same order as the minimum width.
      For a ductile material such as mild steel or copper later distortion takes place, and due to the restraining influences of friction at the load faces, the cross section becomes greatest at the centre, the test piece taking up a barrel shape failure finally occurs by cracks Brittle materials such as cast iron and cement usually frail by wearing along planes inclined  between 50^0 and 700 to the longititudinal axis appearing on the surface and Spreading inwards.
       2.7.4 FATIGUE
      Many machine parts are subjected to fluctuating stresses, taking at relatively high frequencies and under these conditions failure is or occur at stress values much lower than would apply for static loading. This phenomenon is known as ‘fatigue’ failure.
      Fluctuating stresses occur in practice under three main types of loading.
          Direct stresses (tension and compression).
          Bending stresses.
           Torsional stresses
      Experiments show that, for a given means stress, there is a limiting rage of stress below which fracture will not take place for an indefinite number of cycles. This range is known as the endurance or fatigue limit and may be quoted as a maximum and minimum stress or as a range about a certain mean. The fatigue limit in reversed bending is found to be about 25% higher than in reversed tension and compression, probably due to the stress gradient. In reversed torsion the fatigue limit for sear stress is about 0.55 times the tensile fatigue limit.
      In order to determine the fatigue limit at a given mean stress, it is necessary to carry out a series of tests on specimens subjected to a gradually decreasing range of stress. It will then be found that the number of cycles of stress required to fracture each specimen increases and as the fatigue limit is approached some hundreds of millions of reversals may be understood.
      Factors of design which affect the fatigue strength are
      a.     Surface treatment.
      b.     Surface finish.
      c.     The frequency of stress reversals.
      d.     Stress concentrations caused by sudden changes in cross-sectional features such as screw threads and key ways.
      2.8     EFFECT OF CARBON CONTENT
      The variation of mechanical properties in plain carbon steel in the annealed condition is shown below.
      It will be seen that the ultimate strength and hardness values increases together with the increased carbon content, the elastic limit (and similarly the yield point) increasing at a reduced rate. At ,the same time there is a marked falling off in ductility in indicated by the decrease in value for elongation and reduction in area, steel containing more than about 0.6% carbon exhibiting a “brittle” type of fracture.
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    • ABSRACT - [ Total Page(s): 1 ]ABSTRACT WILL BE HERE SOON ... Continue reading---

         

      APPENDIX A - [ Total Page(s): 6 ] ... Continue reading---

         

      TABLE OF CONTENTS - [ Total Page(s): 1 ]TABLE OF CONTENTS CHAPTER ONE 1.0    Introduction  1.2    Statement of the Problem   1.3     Aim and Objectives of the Study  1.4    Justification of the Study       1.5    Scope of the Study   1.6    Proposed Methodology   CHAPTER TWO2.0 Literature Review  2.1 Nigerian Steel Industry (Historical Development)  2.2 Engineering Materials and Properties  2.2.1 Cement and Concrete   2.2.2 Aggregates and Sand  2.2.3 Timber and Plywood   2.3 Strength of Materials ... Continue reading---

         

      CHAPTER ONE - [ Total Page(s): 2 ]CHAPTER ONE 1.0    INTRODUCTION     Steel is a man-made material containing 95% of iron. The remaining constituent are small amount of element derived from the raw-material use in the making of the steel, as well as other element added to improve certain characteristics or properties of the product (Marcus, 1964).    Steel reinforcement are used generally in the form of bars of circular cross-section in concrete structure. They are like a skeleton in human body. Plain concrete without s ... Continue reading---

         

      CHAPTER THREE - [ Total Page(s): 3 ]3.3.2 Principle of OperationWith every 2 revolutions made on the hand or motor driven gear box of high mechanical advantage, a force of 20kN (2000kgf) is applied to a test piece held in the chuck pins. The force deflects the spring beam and this deflection operates a level acting on a piston in a cylinder containing mercury. It should be noted that the mercury inside the sleeve must be at zero point before the drive is made, and this can be alone using the mercury adjuster. The recording graph i ... Continue reading---

         

      CHAPTER FOUR - [ Total Page(s): 8 ]vii.    ELASTIC MODULUSThis is the slope of the straight line portion of each curveSpecimen 1 =(change in stress)/(change in strain) =  295/0.012  = 24583 N/〖mm〗^2Specimen 2 =   240/(0.018 )   = 13333N/〖mm〗^2Specimen 3 = 220/0.012  = 20000N/〖mm〗^2Therefore:Average elastic modulus =   (24583+13333+20000 )/3 = 19305N/〖mm〗^24.1.4 ANALYSIS FOR 16mm MILD STEEL SPECIMENSi. ULTIMATE STRENGTH OR TENSILE STRENGTHSpecimen 1 = 489.48N/ã ... Continue reading---

         

      CHAPTER FIVE - [ Total Page(s): 1 ]CHAPTER FIVE5.0 CONCLUSION AND RECOMMENDATION From the test carried out and the results obtained, the average yield strength for specimens diameter of 8mm, 10mm, 12mm, 16mm, 2Omm and 25mm were 79N/mm2, 225 N/mm2, 261 N/mm2, 277 N/mm2, 295 N/mm2 and 297 N/mm2 respectively. It was therefore observed that specimen of 8mm and 10m do not meet the BS8110 specification of 250 N/mm2 for mild steel.However, the analysis shows that the average ultimate strength obtained for the specimens of 8mm, 10mm 12mm ... Continue reading---

         

      REFRENCES - [ Total Page(s): 1 ]REFERENCESAlbert, G.G., (1960), ‘Elements of Physical Metallurgy’, 2 Edition, Addison Wesley Publishing Co. Inc., London, pp337-340Arthur, H.N., et aL, (2004), ‘Design of Concrete Structures’, 13th Edition, Tata McGraw Hill Companies, India, pp38-50Bakare, O.S., (2006), Thesis on Determination of Ultimate Tensile Strength of High Tensile Steel Specimens, Civil Engineering Department, University of Ilorin, Nigeria.Kenneth. L -. Dionisio. B.. (1997), ‘Reinforced con ... Continue reading---