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THE NATURE OF MATERIALS

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Presentation on theme: "THE NATURE OF MATERIALS"— Presentation transcript:

1 THE NATURE OF MATERIALS
Atomic Structure and the Elements Bonding between Atoms and Molecules Crystalline Structures Noncrystalline (Amorphous) Structures Engineering Materials John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

2 Periodic Table of Elements
Transition Zone contains metalloids or semi‑metals John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

3 Primary Bonds Ionic Bonding Metallic Bonding Covalent Bonding
John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

4 Two Examples of Covalent Bonding
John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

5 Body-Centred Cubic (BCC) Crystal Structure
Unit cell Atoms indicated as point locations in 3d axis system Unit cell model Closely packed atoms sometimes called hard-ball model Repeated pattern of the BCC structure John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

6 Three Crystal Structures in Metals
Body-centered cubic Face-centered cubic Hexagonal close-packed Chromium Iron Molybdenum Tungsten Aluminum Copper Gold Lead Silver Nickel Magnesium Titanium Zinc

7 Point Defects in Crystal Structures
Displaced ion Interstitialcy – lattice distortion produced by an extra atom in structure John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

8 Line Defects in Crystal Structures
Edge of an extra plane of atoms that exists in the lattice Spiral within the lattice structure wrapped around an imperfection line John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

9 Deformation of Crystal Structures
Original Lattice Elastic Deformation Plastic Deformation Elastic strain - no permanent change in positions of atoms Plastic strain - atoms in the lattice are forced to move to new “homes” John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

10 Effect of Dislocations on Strain
John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

11 Crystalline versus Noncrystalline
Crystalline structure Noncrystalline structure Volume changes for a pure metal (a crystalline structure) Versus Volumetric changes in glass (a noncrystalline structure) John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

12 MECHANICAL PROPERTIES OF MATERIALS
Stress‑Strain Relationships Tensile - tend to stretch the material Compressive - tend to squeeze it Shear - tend to cause adjacent portions of material to slide against each other John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

13 Tensile Stress-Strain Relationship
Setup Tensile Test Typical Test Specimen John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

14 Tensile Test Sequence (1) beginning of test, no load
(2) uniform elongation and reduction of cross‑sectional area (3) continued elongation, maximum load reached (4) necking begins, load begins to decrease (5) fracture (6) final length measured with pieces put back together John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

15 Stress-Strain Relationship
s = engineering stress F = applied force Ao = original area of test specimen e = engineering strain L = length at any point during elongation Lo = original gage length John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

16 Typical Engineering Stress-Strain Plot of Metal
Tensile Strength Yield point S Hooke's Law: s = E e E = modulus of elasticity John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

17 Ductility Measure – Elongation EL
EL = elongation Lf = specimen length at fracture Lo = original specimen length AR = area reduction Af = area of cross section at point of fracture Ao = original cross-sectional area Strain hardening - means that the metal is becoming stronger as strain increases John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

18 In-class example A tensile test uses a test specimen that has a gage length of 50 mm and an area = 200 mm2. During the test the specimen yields under a load of 98,000 N. The corresponding gage length = mm. This is the 0.2 percent yield point. The maximum load = 168,000 N is reached at a gage length = 64.2 mm. Determine (a) yield strength, (b) modulus of elasticity, and (c) tensile strength. Fracture occurs at a gage length of 67.3 mm. Determine (d) the percent elongation. (e) If the specimen necked to an area = 92 mm2, determine the percent reduction in area. John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing

19 ASSIGNMENT – STUDENT MUST SHOW SOLUTION TO PROFESSOR DURING LAB PERIOD
A test specimen in a tensile test has a gage length of 2.0 in and an area = 0.5 in2. During the test the specimen yields under a load of 32,000 lb. The corresponding gage length = in. This is the 0.2 percent yield point. The maximum load = 60,000 lb is reached at a gage length = 2.60 in. Determine (a) yield strength, (b) modulus of elasticity, and (c) tensile strength. Fracture occurs at a gage length of 2.92 in. Determine (d) the percent elongation. (e) If the specimen necked to an area = 0.25 in2, determine the percent reduction in area. John Wiley & Sons, Inc. M P Groover, Fundamentals of Modern Manufacturing


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