Rajalakshmi Engineering College - Ph19141 – Physics of Materials – Study Material

Total Page:16

File Type:pdf, Size:1020Kb

Rajalakshmi Engineering College - Ph19141 – Physics of Materials – Study Material RAJALAKSHMI ENGIN EERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL 1 PH19141 - PHYSICS OF MATERIALS LTPC 3 0 2 4 Common to I sem. B.E. - Aero, Auto, Civil, Mech& MCT OBJECTIVES • To enhance the fundamental knowledge in Physics and its applications relevant to mechanical engineering streams. • To familiarize students in various experimental setups and instruments that are used to study / determine the various properties of materials. UNIT I - MECHANICS & PROPERTIES OF MATTER 9 Basic definitions - Newton’s laws – forces -solving Newton’s equations - constraints and friction - cylindrical and spherical coordinates - potential energy function - conservative and non-conservative forces - central forces - conservation of angular momentum - non-inertial frames of reference - rotating coordinate system - centripetal and coriolis accelerations – Elasticity - stress-strain diagram - bending of beams - cantilever depression - Young’s modulus determination - I-shape girders. UNIT II - CRYSTAL PHYSICS 9 Basis – lattices - symmetry operations and crystal systems -Bravaislattics - atomic radius and packing fraction - SC, BCC, FCC, HCP lattices - Miller indices - diffraction by crystals - reciprocal lattice - interpreting diffraction patterns - crystal growth techniques-Czochralski and Bridgmann, crystal defects. UNIT III - PHYSICS OF MATERIALS 9 Solid solutions - Hume-Rothery’s rules –Gibb’s phase rule - binary phase diagrams -isomporhpus systems - tie-line and lever rule - eutectic, eutectoid, peritectic, peritectoid, monotectic and syntectic systems - formation of microstructures - homogeneous and non-homogenous cooling – nucleation - iron-carbon phase diagram - eutectoid steel - hypo and hypereutectoid steel – diffusion - Fick’s laws – T-T-T diagrams. UNIT IV - ENGINEERING MATERIALS & TESTING 9 Metallic glasses – preparation and properties - Ceramics – types, manufacturing methods and properties - Composites – types and properties - Shape memory alloys – properties and applications - Nano-materials – top down and bottom up approaches – properties - Tensile strength – Hardness – Fatigue - Impact strength – Creep - Fracture – types of fracture. UNIT V - QUANTUM PHYSICS 9 Blackbody problem -Planck’s radiation law - duality of light -De Broglie hypothesis - properties of matter waves - wave packets –Schrodinger’s equations (time dependent and time independent) - Born interpretation (physical significance of wave function) - probability current - operator formalism (qualitative) - expectation values - uncertainty principle - particle in a box -eigen function and eigen values -Dirac notation (qualitative). TEXT BOOKS: 1. Bhattacharya, D.K. & Poonam, T. “Engineering Physics”. Oxford University Press, 2018. 2. Gaur, R.K. & Gupta, S.L. “Engineering Physics”. DhanpatRai Publishers, 2018. 3. Raghavan, V. “Physical Metallurgy: Principles and Practice” . PHI Learning, 2019. RAJALAKSHMI ENGINEERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL RAJALAKSHMI ENGIN EERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL 2 REFERENCES 1. Balasubramaniam, R. “Callister's Materials Science and Engineering”. Wiley India Pvt. Ltd., 2017. 2. Raghavan, V. “Materials Science and Engineering : A First course” . PHI Learning, 2019. 3. Resnick, R., Halliday, D., & Walker, J. “Principles of Physics ”, Wiley India Pvt., 2018. LIST OF EXPERIMENTS: PHYSICS LABORATORY (Any 10 experiments) 30 1. Determination of Laser characteristics (wavelength and angular spread). 2. Determination of Young’s modulus by non-uniform bending method 3. Determination of thermal conductivity of a bad conductor – Lee’s Disc method. 4. Determination of velocity of sound and compressibility of liquid – Ultrasonic interferometer 5. Coupled oscillators - Two compound pendulums; 6. Experiment on moment of inertia measurement- Torsional pendulum by resonance, 7. LC circuit, LCR circuit and Resonance phenomena in LCR circuits; 8. Experiments on electromagnetic induction – BH-Curve experiment 9. Determination of thickness of a thin wire – Air wedge method 10. Determination of solar cell characteristics. 11. Measurement of hysteresis loss:B -H curve. 12. Determination of creep characteristics of a metallic wire. TOTAL PERIODS 75 OUTCOMES: On completion of the course students will be able to • Understand foundational mechanics and elastic nature of materials and determine the elastic moduli of materials. • Apply the basic knowledge of crystallography in materials preparation and treatments. • Create binary phase diagrams and TTT charts and use them to analyse and measure the properties of alloys. • Understand various engineering materials, test or measure their properties and use them in suitable applications. • Understand the concepts of quantum theory and the nature of light and determine the characteristics of a given laser source. *** RAJALAKSHMI ENGINEERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL RAJALAKSHMI ENGIN EERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL 3 UNIT I – Mechanics and Properties of Matter Particle: Dimensions of an object are considered to be negligible and small compared to the coordinates describing its motion. System of particles: An object represented by two or more particles and is dealt with together is called system of particles. Rigid body : The distance between any two given points on a rigid body is invariant in time regardless of external forces exerted on it.A rigid body is usually considered as a continuous distribution of mass. Deformable body: Anybody that changes its shape and/or volume while being acted upon by any kind of external force. A force is a push or a pull exerted on one object by another object. The units of force is newton. Newton’s first law: A body continuous a state of rest or uniform motion unless an external force acts on it. Newton's first law says that if the net force on an object is zero ( ΣF=0), then that object will have zero acceleration. That doesn't necessarily mean the object is at rest, but it means that the velocity is constant. The property of a body to remain at rest or to remain in motion with constant velocity is called inertia . Newton’s first law is often called the law of inertia. The inertia of an object is measured by its mass. Mass can be determined by measuring how difficult an object is to accelerate. The more mass an object has, the harder it is to accelerate. Newton’s second law:Acceleration of an object produced by a net force is directly proportional to the magnitude of the net force, in the same direction as the net force, and inversely proportional to the mass of the object. Newton’s third law: All forces between two objects exist in equal magnitude and opposite direction. Newton’s first law of motion from Newton’s second law of motion Newton's first law states that a body stays at rest if it is at rest and moves with a constant velocity if already moving, until a net force is applied to it. In other words, the state of motion of a body changes only on application of a net non-zero force.Newton's second law states that the net force applied on a body is equal to the rate of change in its momentum. Mathematically, ͤ⃗͘ ̀⃗ = Where, F is the net force, and p is the momentum.ͨ͘ Now, we can write the same as, ͤ⃗͘ ͘ʚͪ⃗͡ʛ ͘͡ ʚͪ⃗ʛ ̀⃗ = ⇒ ̀⃗ = = ͨ͘ ͨ͘ ͨ͘ RAJALAKSHMI ENGINEERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL RAJALAKSHMI ENGIN EERING COLLEGE - PH19141 – PHYSICS OF MATERIALS – STUDY MATERIAL 4 So, if the net force, F is zero, change in the value of v is be zero i.e., a body at rest will be at rest and a body moving with constant velocity will continue with the same velocity, until a net force is applied. This conclusion is similar to the Newton’s first law of motion. Thus, we can derive Newton’s first law of motion using Newton’s second law of motion. Newton’s third law of motion from Newton’s second law of motion Consider an isolated system of two bodies A & B mutually interacting with each other, provided there is no external force acting on the system. Let F AB , be the force exerted on body B by body A and F BA be the force exerted by body B on A.Suppose that due to these forces F AB and F BA , dp 1/dt and dp 2/dt be the rate of the change of momentum of these bodies respectively. Then, F BA = dp 1/dt ---------- (i) FAB = dp 2/dt ---------- (ii) Adding equations (i) and (ii), we get, FBA + F AB = dp 1/dt + dp 2/dt F + F = d(p + p )/dt ⇒ BA AB 1 2 If no external force acts on the system, then d(p 1 + p 2)/dt = 0 F + F = 0 ⇒ BA AB F = - F --------- (iii) ⇒ BA AB the above equation (iii) represents the Newton's third law of motion (i.e., for every action there is equal and opposite reaction). Constrained Motion: In some cases a particle is forced to move along a curve or surface. This curve or surface is referred to as a constraint, and the resulting motion is called constrained motion. The particle exerts a force on the constraint, and by Newton’s third law the constraint exerts a force on the particle. This force is called the reaction force, and is described by giving its components normal to the motion, denoted N, and parallel to the motion, denoted f . Constrained motion results when an object is forced to move in a restricted way. For example, it may have to move along a curved track, to slide on a table that may accelerate upwards, to stay in contact with an accelerating wedge, etc. Constraint Forces adjust themselves according to Newton's Second Law so that the acceleration of an object is just the right value for the object to follow the motion required by the particular constrained. Friction: In the constrained motion of a particle a common force parallel to the motion of the particle is friction, which typically acts in the direction opposite to that of the motion (i.e., it acts in such a way as to slow the motion of the particle). Experimentally, it is found that the magnitude of the frictional force is proportional to the magnitude of the normal force, i.e., f = µN, where the proportionality constant, µ is referred to as the coefficient of friction.
Recommended publications
  • Periodic Table of Crystal Structures
    Periodic Table Of Crystal Structures JeffreyJean-ChristopheLoneliest entitled Prent sosometimes aping fretfully almost that interjects third,Batholomew thoughany oscillogram canalizesPietro impedes offsaddleher loquaciousness? his loungingly.alkalescences Felon apprenticed. and downbeat Which This article serves to illustrate how conventional bonding concepts can be adapted to the understanding of the structures and structural transformations at high pressure with examples drawn mainly on the experience of the author. Another way to describe the bonding in metals is nondirectional. What is the Periodic Table Showing? To receive a free trial, but how those elements are stacked together is also very important to know. Full potential LMTO total energy and force calculations in: electronic structure and physical properties of solids. Let us examine some of the more common alloy systems with respect to the metallurgy of the material and its purpose in bearing design. The CCDC license is managed by the Chemistry Dept. The microcrystals are deformed in metalworking. Working with lattices and crystals produces rather quickly the need to describe certain directions and planes in a simple and unambigous way. It can cause damage to mucous membranes and respiratory tissues in animals. It is formed by combining crystal systems which have space groups assigned to a common lattice system. Please check the captcha form. Is more than one arrangement of coordination polyhedra possible? Polishing and etching such a specimen discloses no microcrystalline structure. This is reflected in their properties: anisotropic and discontinuous. Even metals are composed of crystals at the microscopic level. It is a noble metal and a member of the platinum group.
    [Show full text]
  • Review of Metallic Structure
    Phase Diagrams—Understanding the Basics Copyright © 2012 ASM International® F.C. Campbell, editor All rights reserved www.asminternational.org APPENDIX A Review of Metallic Structure THE WORD METAL, derived from the Greek metallon, is believed to have originated as a verb meaning to seek, search after, or inquire about. Today, a metal is defined as any element that tends to lose electrons from the outer shells of its atoms. The resulting positive ions are held together in crystalline structure by the cloud of these free electrons in what is known as the metallic bond. The metallic bond yields three physical characteris- tics typical of solid metals: (1) metals are good conductors of electricity, (2) metals are good conductors of heat, and (3) metals have a lustrous appearance. In addition, most metals are malleable, ductile, and generally denser than other elemental substances. Those elements that do not display the characteristics of the metallic elements are called nonmetals. However, there are some elements that behave as metals under some circumstances and as nonmetals under different circumstances. These are now called semimetals, but have also been called metalloids, meaning like metals. The boundaries separating the regions in the periodic table covered by the different classes of elements are not distinct, except that nonmetals never form positive ions. A simplified periodic table is shown in Fig. A.1, high- lighting the elements that are currently considered to be metals. A.1 Periodic Table In the periodic table, it is the number of electrons in the outer shell that affects the properties of the elements the most.
    [Show full text]
  • CHAPTER 3: Crystal Structures and Properties
    CHAPTER 3: Crystal structures and properties ISSUES TO ADDRESS... • How do atoms assemble into solid structures? (for now, focus on metals) • How does the density of a material depend on its structure? • When do material properties vary with the sample (i.e., part) orientation? 1 Energy and packing • Non dense, random packing Energy typical neighbor bond length typical neighbor r bond energy •Dense, regular packing Energy typical neighbor bond length typical neighbor r bond energy Dense, regular-packed structures tend to have lower energy. 2 Materials and packing Crystalline materials... • atoms pack in periodic, 3D arrays • typical of: -metals -many ceramics -some polymers crystalline SiO2 Adapted from Fig. 3.18(a), Callister 6e. Si Oxygen Noncrystalline materials... • atoms have no periodic packing • occurs for: -complex structures -rapid cooling "Amorphous" = Noncrystalline noncrystalline SiO2 Adapted from Fig. 3.18(b), Callister 6e. 3 Metallic crystals • tend to be densely packed. • have several reasons for dense packing: -Typically, only one element is present, so all atomic radii are the same. -Metallic bonding is not directional. -Nearest neighbor distances tend to be small in order to lower bond energy. • have the simplest crystal structures. We will look at three such structures... 4 Simple Cubic (SC) structure • Rare due to poor packing (only Po has this structure) • Close-packed directions are cube edges. • Coordination # = 6 (# nearest neighbors) (Courtesy P.M. Anderson) 5 Atomic Packing Factor (APF) Volume of atoms in unit cell* APF = Volume of unit cell *assume hard spheres • APF for a simple cubic structure = 0.52 volume atoms 4 atom a unit cell 1 π (0.5a) 3 3 R=0.5a APF = a 3 volume close-packed directions unit cell contains 8 x 1/8 = 1 atom/unit cell Adapted from Fig.
    [Show full text]
  • The Structure of Crystalline Solids
    THE STRUCTURE OF CRYSTALLINE SOLIDS Subject: Material Science - Lecture #5 مدرسة المادة : الدكتورة روژه برهان الدين عبدالرحمن Kirkuk University - College of Science Physics Department – 3rd grade مدرسة المادة : الدكتورة روژه برهان الدين عبدالرحمن Subject: Material Science Lecture # 5 WHY STUDY The Structure of Crystalline Solids? • The properties of some materials are directly related to their crystal structures. For example, pure and undeformed magnesium and beryllium, having one crystal structure, are much more brittle (i.e., fracture at lower degrees of deformation) than are pure and undeformed metals such as gold and silver that have yet another crystal structure • Furthermore, significant property differences exist between crystalline and noncrystalline materials having the same composition. For example, noncrystalline ceramics and polymers normally are optically transparent; the same materials in crystalline (or semicrystalline) form tend to be opaque or, at best, translucent. 2 Kirkuk University - College of Science - Physics Department - 3rd grade مدرسة المادة : الدكتورة روژه برهان الدين عبدالرحمن Subject: Material Science Lecture # 5 Learning Objectives After studying this chapter, you should be able to do the following: 1. Describe the difference in atomic/molecular structure between crystalline and noncrystalline materials. 2. Draw unit cells for face-centered cubic, body-centered cubic, and hexagonal close-packed crystal structures. 3. Derive the relationships between unit cell edge length and atomic radius for face-centered cubic and body-centered cubic crystal structures. 4. Compute the densities for metals having face-centered cubic and body-centered cubic crystal structures given their unit cell dimensions. 3 Kirkuk University - College of Science - Physics Department - 3rd grade مدرسة المادة : الدكتورة روژه برهان الدين عبدالرحمن Subject: Material Science Lecture # 5 5.
    [Show full text]