Design of an Aerospace Component

Slides:



Advertisements
Similar presentations
LECTURER5 Fracture Brittle Fracture Ductile Fracture Fatigue Fracture
Advertisements

3 – Fracture of Materials
ME 240: Introduction to Engineering Materials Chapter 8. Failure 8.1 CHAPTER 8.
Crack Nucleation and Propagation
CHE 333 Class 20 Fracture continued.
MSM Lab . ( Graduate Student )
Design of Machine Elements
Engineering materials lecture #14
PRINCIPLES OF PRODUCTION ENGINEERING
CHE 333 Class 14 Plastic Deformation of Metals and Recrystallization.
Component Testing Test Setup TapLok Insert Shear Key Copper Threads Friction Tests Collar Shear Tests NSTX TF FLAG JOINT REVIEW 8/7/03 Michael Kalish.
Crystalline Arrangement of atoms. Chapter 4 IMPERFECTIONS IN SOLIDS The atomic arrangements in a crystalline lattice is almost always not perfect. The.
Dislocations and Strengthening
Chapter 5 – Design for Different Types of Loading
Home Work #4 Due Date: 18 Mar, 2010 (Turn in your assignment at the mail box of S581 outside the ME general office) The solutions must be written on A4.
THEORIES OF FAILURE THEORIES OF FAILURE FOR DUCTILE MATERIALS
Chapter 6 Fatigue Failure Theories
ENGR 225 Section
Mechanical Properties of Metals
Thermal Strains and Element of the Theory of Plasticity
Effect of finite size of component The SIF derived earlier is for cracks in an infinite body. However the finite size, geometry of the component, loading.
Solidification and Heat Treatment
DISLOCATION MOVEMENT.
WEEK 2 STRUCTURE OF MATERIALS MATERIALS SCIENCE AND MANUFACTURING PROCESSES.
The Structures of Metals
Fatigue Fatigue is the lowering of strength or the failure of a material due to repetitive stress, which may be above or below the yield strength. Many.
Fracture Mechanic Dr.Behzad Heidar shenas. Course Outline -An overview on the materials characteristics: 1.Types of crystal structures 2. Defects 3.Stress-Strain.
5/6/2002, Monday Summary: What we learned from this course?
Copyright Prentice-Hall Behavior and Manufacturing Properties of Part I Q1.1 (25): What is the difference between a material’s mechanical property and.
Design Stress & Fatigue
DESIGN FOR FATIGUE STRENGTH
FATIGUE Fatigue of Materials (Cambridge Solid State Science Series) S. Suresh Cambridge University Press, Cambridge (1998)
Mechanical Behavior, Testing and Manufacturing Properties of Materials
Week 4 Fracture, Toughness, Fatigue, and Creep
Chapter 8: Failure of Metals
Fracture, Toughness, Fatigue, and Creep
Registered Electrical & Mechanical Engineer
Mechanics of Materials II UET, Taxila Lecture No. (4&5)
Dislocation And Strengthening Mechanisms Plastic deformation through dislocation: Slip Ideal shear stress d a   ~ G d/a ~ 10 6 psi (calc.) ~ 10~10 3.
Strengthening of Metals.
Mechanical & Aerospace Engineering West Virginia University Statistics of Brittle Fracture.
Deformation of Axially Loaded Members - Single Member
Example 1: The lattice constant “a” of BCC iron is 2.86 Å. Determine the specific gravity. Atomic mass of Fe = g/mole. Å 2.86 Å # of atoms/cell =
Problems 1. A large plate is fabricated from a steel alloy that has a plane strain fracture toughness of 82.4MPa√m. If, during service use, the plate is.
Week 4 Fracture, Toughness, Fatigue, and Creep
Materials Science Chapter 4 Disorder in solid Phases.
Problems H.P. : 신재혁.
Plastic deformation Extension of solid under stress becomes
A = 122 mm2 Establish that Schmid’s law is obeyed.
Materials Science Chapter 8 Deformation and Fracture.
Hasmukh Goswami College Of Engineering
Methods to Maximize Design Life
Engineering materials lecture #12
Chapter 3 Mechanical Properties of Materials
CHE 333 Class 20 Fracture continued.
Atomic Structure and Bonding
Determination of Fracture Toughness
Materials: engineering, science, processing and design, 2nd edition Copyright (c)2010 Michael Ashby, Hugh Shercliff, David Cebon.
1/18/2019 6:28 AM C h a p t e r 8 Failure Dr. Mohammad Abuhaiba, PE.
Mechanical Properties: 2
Surface Technology Part 1 Introduction
Plastic Deformation of Metals and Recrystallization
FATIGUE FATIGUE Dr. Mohammed Abdulrazzaq
Plastic Deformation of Metals and Recrystallization
Simple Stresses & Strain
Lab8: Fatigue Testing Machine
Lab8: Fatigue Testing Machine
Mechanical Properties Of Metals - I
Mechanical Failure(파괴)
Presentation transcript:

Design of an Aerospace Component Question 1 Design of an Aerospace Component Because Mg is a low-density material (r = 1.738 g/cm3) with a low melting temperature (670 oC) and boiling point, it has been considered for use in an aerospace vehicle intended to enter the outer space environment. Is this a good material design? In space, the pressure is low. Even at relatively low temperatures, solid magnesium can begin to change to a vapor, causing metal loss that could damage a space vehicle. In addition, solar radiation could cause the vehicle to heat, increasing the rate of magnesium loss. A low density material with higher boiling point (lower vapor pressure) would be better. Al boils at 2494 oC and is a good alternative.

Question 2

Question 3 Calculate the theoretical density of Si. Assume a diamond cubic structure and the radius to be 1.176 Angstroms.

Question 4 Calculate the theoretical density of GaAs, which is a compound semiconductor having the zinc blende structure, given that the atomic mass of Ga is 69.723 g/mole and As is 74.921 g/mole and that the radius of the Ga ion is 0.62 A and the radius of the As ion is 2.22 A. (2)

Question 5 The coefficient for linear thermal expansion for Al is 23.6x10exp(-6) /oC. If a 200 mm long, 100 mm diameter rod is heated from 20 oC to 100 oC, what are the dimensions (length and diameter) of the rod at 100 oC? Is there a stress on the rod? (2)

Question 6 If an application requires materials to support loads at 250 degrees C, determine whether gold, copper, iron and titanium will likely creep. The design temperature is 250 + 273 = 523 K. Both Au and Cu will likely creep since T/Tm is 0.39 and 0.38, respectively, and they are pure elements that have no creep strengthening. The melting temperatures Fe (2447 oC) and Ti (1668 oC) are too high for creep at 250 C.

Question 7 D: 0,1,1/2 – 100 = -1,1,1/2 =

Question 8

Question 9

Question 10

Question 11 What are the indices of the four directions of the form <111> that lie in the plane of a cubic cell? (2)

Question 12 Calculate the length of the dislocation Burgers vector in BCC iron (low temperature), FCC iron, aluminum, and germanium.

Question 13 Calculate the length of the dislocation Burgers vector for Silicon given that its (111) has width of 3.135 Angstroms.

Question 14 A slight misalignment of an optoelectronic device during fabrication leaves a grain boundary passing through the optically active region having a width of 20 nm. If the two grains approach each other at an angle of 10 degrees, how many dislocations, N, could exist to short out the device?

Question 15 A single crystal of an BCC metal is oriented so that the [001] direction is parallel to an applied stress. If the critical resolved shear stress is 12,000 psi, calculate the magnitude of the applied stress required to cause slip to begin in the direction in the , , and slip planes.

Question 16 The strength of titanium is found to be 65,000 psi when the grain size is 17 x 10-6 m and 82,000 psi when the grain size is 0.8 x 10-6 m. Determine the constants in the Hall-Petch equation and the strength of the titanium when the grain size is reduced to 0.2 x 10-6 m.

Question 17

Question 18

Question 19 f

Question 20 – Part 1 The acrylic polymer from which the figure below was obtained is subjected to an alternating stress between 15 MPa and 0 MPa. The largest surface cracks initially detected by non-destructive testing are 0.001 mm in length. From the graph calculate the constants C and n for the steady state fatigue equation. If the critical fracture toughness of the polymer is 2 MPa sqrt(in), calculate the critical flaw size, ac and the number of cycles, N, required before failure occurs, which is given by the equation below. Let f = 1.0.

Question 20 – Part 2 The acrylic polymer from which the figure below was obtained is subjected to an alternating stress between 15 MPa and 0 MPa. The largest surface cracks initially detected by non-destructive testing are 0.001 mm in length. From the graph calculate the constants C and n for the steady state fatigue equation. If the critical fracture toughness of the polymer is 2 MPa sqrt(in), calculate the critical flaw size, ac and the number of cycles, N, required before failure occurs, which is given by the equation below. Let f = 1.0. From:

Question 21 In a fatigue test, the maximum stress applied in tension is 80,000 psi and the minimum stress in compression is 20,000 psi. Determine the stress range, stress amplitude, mean stress and stress ratio, R Smax = 80,000 psi; Smin = -20,000 psi Stress range, Sr = 80,000 – (-20,000) = 100,000 psi Stress amplitude = Sr/2 = 50,000 psi Mean stress = (80,000 + (-20,000))/2 = 30,000 psi Stress ratio = Smax/ Smin = -20,000/80,000 = -0.25

Question 22 Calculate the fatigue limit of a steel that has an ultimate tensile strength of 160 psi when the stress ratio, R = 0 and a 50 per cent probability of enduring the stress for the life of the component. Use a safety factor of 2. Determine the diameter of the rod to be used to carry a fluctuating load of 20,000 lb-force. The 50% probability of survival for the life of the component corresponds to the fatigue limit of the steel. Thus, Fatigue Limit = 0.5 UTS = 80 psi With a safety factor of 2, cycle stress = 80,000/2 = 40,000 psi For a cyclic load of 20,000 lb-force, the conservative diameter of the steel will be in push-pull mode and

Question 23 The activation energy for self-diffusion in copper is 49,300 cal/mol. A copper specimen creeps at 0.002 in/in –h when a stress of 15,000 psi is applied at 600 oC. If the creep rate is dependent on self-diffusion, determine the creep rate if the temperature is 800 oC.

Question 24