BME 207 Introduction to Biomechanics Spring 2017

Similar documents
BME 207 Introduction to Biomechanics Spring Homework 9

Mechanical Design in Optical Engineering

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 3 Torsion

Structural Analysis I Chapter 4 - Torsion TORSION

Mechanics of Materials II. Chapter III. A review of the fundamental formulation of stress, strain, and deflection

MECHANICS OF MATERIALS

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Stress Strain Elasticity Modulus Young s Modulus Shear Modulus Bulk Modulus. Case study

ME Final Exam. PROBLEM NO. 4 Part A (2 points max.) M (x) y. z (neutral axis) beam cross-sec+on. 20 kip ft. 0.2 ft. 10 ft. 0.1 ft.

Solution: The strain in the bar is: ANS: E =6.37 GPa Poison s ration for the material is:

MAAE 2202 A. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work.

[7] Torsion. [7.1] Torsion. [7.2] Statically Indeterminate Torsion. [7] Torsion Page 1 of 21

PDDC 1 st Semester Civil Engineering Department Assignments of Mechanics of Solids [ ] Introduction, Fundamentals of Statics

Solid Mechanics Homework Answers

(48) CHAPTER 3: TORSION

Strength of Materials Prof S. K. Bhattacharya Department of Civil Engineering Indian Institute of Technology, Kharagpur Lecture - 18 Torsion - I

Chapter 5 Torsion STRUCTURAL MECHANICS: CE203. Notes are based on Mechanics of Materials: by R. C. Hibbeler, 7th Edition, Pearson

ME 176 Final Exam, Fall 1997

Mechanical Engineering Ph.D. Preliminary Qualifying Examination Solid Mechanics February 25, 2002

2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at A and supported at B by rod (1). What is the axial force in rod (1)?

M. Vable Mechanics of Materials: Chapter 5. Torsion of Shafts

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 2 Stress & Strain - Axial Loading

[5] Stress and Strain

MECHANICS OF MATERIALS

3.5 STRESS AND STRAIN IN PURE SHEAR. The next element is in a state of pure shear.

NAME: Given Formulae: Law of Cosines: Law of Sines:

Chapter 3. Load and Stress Analysis

CHAPTER 2 Failure/Fracture Criterion

Torsion of Shafts Learning objectives

QUESTION BANK SEMESTER: III SUBJECT NAME: MECHANICS OF SOLIDS

CIVL222 STRENGTH OF MATERIALS. Chapter 6. Torsion

QUESTION BANK DEPARTMENT: CIVIL SEMESTER: III SUBJECT CODE: CE2201 SUBJECT NAME: MECHANICS OF SOLIDS UNIT 1- STRESS AND STRAIN PART A

twenty one concrete construction: shear & deflection ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2014 lecture

The example of shafts; a) Rotating Machinery; Propeller shaft, Drive shaft b) Structural Systems; Landing gear strut, Flap drive mechanism

Structural Metals Lab 1.2. Torsion Testing of Structural Metals. Standards ASTM E143: Shear Modulus at Room Temperature

Chapter 5: Torsion. 1. Torsional Deformation of a Circular Shaft 2. The Torsion Formula 3. Power Transmission 4. Angle of Twist CHAPTER OBJECTIVES

5. What is the moment of inertia about the x - x axis of the rectangular beam shown?

Torsion of shafts with circular symmetry

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.

The problem of transmitting a torque or rotary motion from one plane to another is frequently encountered in machine design.

Torsion Stresses in Tubes and Rods

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE

ME311 Machine Design

High Tech High Top Hat Technicians. An Introduction to Solid Mechanics. Is that supposed to bend there?

UNIT-I STRESS, STRAIN. 1. A Member A B C D is subjected to loading as shown in fig determine the total elongation. Take E= 2 x10 5 N/mm 2

PERIYAR CENTENARY POLYTECHNIC COLLEGE PERIYAR NAGAR - VALLAM THANJAVUR. DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK

INTRODUCTION TO STRAIN

AERO 214. Lab II. Measurement of elastic moduli using bending of beams and torsion of bars

Solution: T, A1, A2, A3, L1, L2, L3, E1, E2, E3, P are known Five equations in five unknowns, F1, F2, F3, ua and va

IDE 110 Mechanics of Materials Spring 2006 Final Examination FOR GRADING ONLY

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Chapter 7. Highlights:

Sub. Code:

4. SHAFTS. A shaft is an element used to transmit power and torque, and it can support

Experiment: Torsion Test Expected Duration: 1.25 Hours

KINGS COLLEGE OF ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING QUESTION BANK. Subject code/name: ME2254/STRENGTH OF MATERIALS Year/Sem:II / IV

Bone Tissue Mechanics

3 Hours/100 Marks Seat No.

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Advanced Structural Analysis EGF Section Properties and Bending

(Refer Slide Time: 01:00 01:01)

Members Subjected to Torsional Loads

Solution: The moment of inertia for the cross-section is: ANS: ANS: Problem 15.6 The material of the beam in Problem

Class XI Chapter 9 Mechanical Properties of Solids Physics

ME 2570 MECHANICS OF MATERIALS

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

SRI CHANDRASEKHARENDRA SARASWATHI VISWA MAHAVIDHYALAYA

ME325 EXAM I (Sample)

Experiment Two (2) Torsional testing of Circular Shafts

WORCESTER POLYTECHNIC INSTITUTE

The science of elasticity

Only for Reference Page 1 of 18

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS

COURSE TITLE : APPLIED MECHANICS & STRENGTH OF MATERIALS COURSE CODE : 4017 COURSE CATEGORY : A PERIODS/WEEK : 6 PERIODS/ SEMESTER : 108 CREDITS : 5

2. Polar moment of inertia As stated above, the polar second moment of area, J is defined as. Sample copy

MECE 3321: MECHANICS OF SOLIDS CHAPTER 5

Chapter 13 ELASTIC PROPERTIES OF MATERIALS

MECHANICS OF MATERIALS REVIEW

Physics 8 Monday, November 20, 2017

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA SCIENCE FOR TECHNICIANS OUTCOME 1 - STATIC AND DYNAMIC FORCES TUTORIAL 3 STRESS AND STRAIN

Chapter 4 Deflection and Stiffness

Stress Transformation Equations: u = +135 (Fig. a) s x = 80 MPa s y = 0 t xy = 45 MPa. we obtain, cos u + t xy sin 2u. s x = s x + s y.

6.4 A cylindrical specimen of a titanium alloy having an elastic modulus of 107 GPa ( psi) and

Downloaded from Downloaded from / 1

Module 5: Theories of Failure

FINAL EXAMINATION. (CE130-2 Mechanics of Materials)

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 4 Pure Bending Homework Answers

Question 1. Ignore bottom surface. Solution: Design variables: X = (R, H) Objective function: maximize volume, πr 2 H OR Minimize, f(x) = πr 2 H

2012 MECHANICS OF SOLIDS

COURSE TITLE : THEORY OF STRUCTURES -I COURSE CODE : 3013 COURSE CATEGORY : B PERIODS/WEEK : 6 PERIODS/SEMESTER: 90 CREDITS : 6

MECE 3321 MECHANICS OF SOLIDS CHAPTER 1

GATE SOLUTIONS E N G I N E E R I N G

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS

Chapter 8 Structural Design and Analysis. Strength and stiffness 5 types of load: Tension Compression Shear Bending Torsion

CHAPTER THREE SYMMETRIC BENDING OF CIRCLE PLATES

EMA 3702 Mechanics & Materials Science (Mechanics of Materials) Chapter 10 Columns

Transcription:

April 7, 2017 UNIVERSITY OF RHODE ISAND Department of Electrical, Computer and Biomedical Engineering BE 207 Introduction to Biomechanics Spring 2017 Homework 7 Problem 14.3 in the textbook. In addition to parts a-d, at r = 1 cm compute the e) shear stress τ and f) shear strain γ. Answers e) τ = 119.37 Pa f) γ = 0.683 Problem 2 A circular tube subjected to pure torsion by moments has an outer radius equal to twice the inner radius r i. A. If the maximum shear strain is measured as 400 10 6 rad, what is the shear strain γ min at the inner surface? B. If the maximum allowable rate of twist is 0.45 /m, and the maximum shear strain is to be kept at 400 10 6 rad by adjusting the moment, what is the minimum required outer radius? r i = 2r i Answers A. γ min = 200 10 6 rad B. minimum = 50.93 mm Problem 3 A circular tube of length = 0.90 m is loaded in torsion by moments. A. If the inner radius is r i = 40 mm and the measured angle of twist between the ends is 0.5, what is the shear strain γ min at the inner surface? B. If the maximum allowable shear strain is 0.0005 rad and the angle of twist is kept at 0.5 by adjusting the moment, what is the maximum permissible outer radius? r i Answers A. γ min = 387.9 10 6 rad B. maximum = 51.6 mm - 1 -

BE 207 - Homework 7 April 7, 2017 Problem 4 A circular tube is loaded in torsion by moments. The tube is 30 cm long with inside and outside diameters of 6 and 8 cm, respectively. When the moment is 5800 N-m, the measured twist angle is 3.63. Compute the maximum shear strain γ max, the shear modulus of elasticity G, and the maximum shear stress τ max. 6 cm 30 cm 8 cm Answers γ max = 8.45 10 3 rad G = 10.0 GPa τ max = 84.4 Pa Problem 5 A solid steel baf circular cross section has a diameter d = 1.5 inches, length = 4.5 feet, and shear modulus of elasticity G = 11.5 10 6 psi. The bar is subjected to moments at the ends. A. If the moments have magnitude = 250 lb-ft, what is the maximum shear stress in the bar? What is the angle of twist at the ends? B. If the allowable shear stress is 6000 psi and the allowable angle of twist is 2.5, what is the maximum allowable moment? d Answers A. τ max = 4527.1 psi θ = 1.62 B. max = 331.4 lb-ft Problem 6 Determine the minimum required diametef a solid circular bar given the design requirements: i. maximum allowable shear stress is 70 Pa; ii. twist angle between two points located 2.5 m apart must not exceed 3 ; iii. applied moment is 1400 N-m; iv. shear modulus G = 11 GPa. Answers minimum diameter is 88.7 mm - 2 -

BE 207 - Homework 7 April 7, 2017 Problem 7 Our textbook defines torsional stiffness k T as the ratio of the applied torque to the resultant angular deformation (the angle of twist). Using Equation 14.29 we can show: θ = k T = GJ where G is the shear modulus of elasticity, J is the polar moment of inertia, and is the length of the rod. A. For the rod shown with dimensions = 1.2 m, = 15 mm and shear modulus of elasticity G = 28 GPa: i. compute the torsional stiffness; ii. compute the maximum shear strain, maximum shear stress, and the applied moment (torque) if the angle of twist is 4 degrees; iii. compute the shear strain and shear stress at r = 6 mm. iv. Sketch the shear stress and shear strain versus the distance from the centef the rod. B. The centef the rod is now drilled out to create a hollow tube with inner diameter r i = 12 mm. i. Derive the polar moment of inertia for the hollow tube: J = π 2 ( r 4 o r 4 i ) (This is the equation above Equation 14.27 in our book.) ii. Compute the torsional stiffness for the hollow tube. iii. Compute the maximum and minimum shear strain, the maximum and minimum shear stress, and the twist angle if the applied moment is same as in part A.ii above. iv. Compute the shear strain and shear stress at r = 14 mm. v. Sketch the shear stress and shear strain versus the distance from the centef the hollow tube. Answers A. k T = 1855.5 N-m; γ max = 8.73 10 4, τ max = 24.4 Pa, = 129.5 N-m; at r = 6 mm: γ = 3.49 10 4, τ = 9.77 Pa B. k T = 1095.5 N-m; γ max = 14.8 10 4, γ min = 11.8 10 4, τ max = 41.4 Pa, τ min = 33.1 Pa, θ = 6.78 ; at r = 14 mm: γ = 1.38 10 3, τ = 38.6 Pa - 3 -

BE 207 - Homework 7 April 7, 2017 Problem 8 A solid shaft and a hollow tube are constructed of the same material (with shear modulus G and density ρ) and have the same length and outer radius. The hollow tube inner radius is 0.6. A. Assuming the shaft and tube are subjected to the same moment, compare their maximum shear stresses τ max, angles of twist θ, and weights W. B. Calculate the ratio (tube/shaft) for τ max, θ, and W. r i = 0.6 Answers A. τ shaft = 2 πr 3 o θ shaft = 2 πgr 4 o W shaft = ρπr 2 o B. τ tube /τ shaft = 1.15 θ tube /θ shaft = 1.15 W tube /W shaft = 0.64 Problem 9 As the premier biomedical engineer at your company, you have been chosen to design the artificial tibia for a new prosthetic leg. This artificial bone will be a circular shaft that must support a torque of 1200 N-m without exceeding a maximum shear stress of 40 Pa. The shear modulus of the shaft material is 78 GPa. The shaft can be either a solid bar a hollow tube; both have a circular cross section. A. Compute the required diameter d o of the solid bar. B. Compute the required outer diametef the hollow tube if the thickness of the tube is one-eighth of the outer radius. C. Determine the outer diameter ratio and weight ratio of the hollow tube to the solid bar. D. Compute the maximum and minimum shear stress and shear strain in each shaft. E. Compute the torsional stiffness ratio of the tube to the bar. F. Compute the rate of twist in each shaft when a moment of 160 N-m is applied. G. Given these results, which is stronger, the solid bar hollow tube? If maximal strength and minimal weight are design criteria, should the prosthetic be a solid bar tube? What does this imply for the geometric structure of long bones? Answers A. solid bar: d o = 5.35 cm B. hollow tube: d o = 7.17 cm C. tube/bar diameter ratio = 1.342, weight ratio = 0.422 D. bar: τ max = 40 Pa, τ min = 0, γ max = 0.513 10 3, γ min = 0 tube: τ max = 40 Pa, τ min = 35 Pa, γ max = 0.513 10 3, γ min = 0.449 10 3 E. tube/bar k T ratio = 1.342 F. tube: 0.109 /m, bar: 0.147 /m - 4 -

BE 207 - Homework 7 April 7, 2017 Problem 10 The picture shows midshaft cross sections of femurs from a woman in her thirties (left) and from a woman in her nineties (right) [RB artin, DB Burr, NA Sharkey; Skeletal Tissue echanics (Springer 1998)]. Osteoporosis has greatly reduced the cross sectional area of the older specimen. For this analysis the femur will be modeled as a hollow cylindrical tube with an outer diametef 6 cm and ultimate stress of 130 Pa. A moment is applied to the femur so the load is pure torsion. A. Assume the healthy femur has an inner diametef 3 cm. Compute the applied moment required to break the healthy femur. B. Due to osteoporosis the cortical thickness of the older femur is reduced by 50%. Compute the moment required to break the older femur. C. Sketch the shear stress versus the distance from the centef the long axis for both femurs. D. Sketch the shear strain versus the radius for both femurs. Assume G = 3.3 GPa. E. In light of the above results, why do older people suffer more bone fractures? Answers A. = 5169 N-m B. = 3769 N-m C. younger: τ min = 65 Pa, older: τ min = 97.5 Pa both: τ max = 130 Pa - 5 -

BE 207 - Homework 7 April 7, 2017 Problem 11 While out jogging, a clumsy professor misjudges a curb and begins to fall. Due to his stride, the body weight generates a compressive axial force of 1725 N on the femur. During the fall, a twisting torque of 900 N-m is applied to the femur. The bone has inner and outer diameters of 4.4 cm and 5.0 cm, respectively. For the following analysis consider a typical material element on the anterior surface of the femur. A. Compute the axial stress σ Y caused by the body weight. B. Compute the torsional shear stress τ S caused by the twisting torque of the fall. (When discussing principal stresses we ve been calling this τ max, but part D will show this isn t the maximum shear stress.) C. Compute the principal stresses that arise from the combined load of the axial force and the twisting torque. Also compute the orientation of the principal plane. D. Compute the maximum shear stress, the associated normal stresses, and orientation of the maximum shear plane. E. Experimental data from the human femur give the ultimate stress values below. Since the combined load is rapidly applied, the ultimate stress approximates the failure stress. Given these data, how does the bone fracture? Sketch the crack path on the shaft of the femur. load type σ U (Pa) tension 78.8 144 compression 170 209 y σ Y τ XY σ X x Answers A. σ Y = 3.89 Pa B. τ S = 91.60 Pa C. σ 1 = 89.7 Pa, σ 2 = 93.6 Pa, θ P = 44.4 D. τ max = 91.62 Pa, σ avg = 1.95 Pa, θ S = 89.4 This combined loading problem demonstrates the superposition of the individual loads. In most analyses superposition is justified as long as we considenly linear elasticity. Since the stresses here are rather high, and the loads are applied rapidly, we are actually in the realm of nonlinear elasticity so superposition really doesn t hold. But it s a fun problem to think about even if the assumptions are a bit of a stretch... - 6 -

BE 207 - Homework 7 April 7, 2017 Problem 12 Suppose you are designing an artificial femur, and you need to increase its torsional stiffness compared to an older model. From Problem 7 and the textbook s Equation 14.29 we know the torsional stiffness is k T = θ = GJ where is the applied moment, θ is the twist angle, G is the shear modulus of elasticity, J is the polar moment of inertia, and is the length of the femur. Your new prosthetic femur will replace a solid circular cylinder with a polar moment of inertia J old ; your new femur must have J new = 2J old. The material will not change. Since you know hollow tubes are more stiff than solid cylinders, you decide to use a circular tube with inner radius r i and outer radius. The cross-sectional area of your new femur must be same as that of the old femur, which has radius r. A. Determine r i and in terms of r. B. What is the weight ratio of the two femurs? Given the data = 7.6 N-m r = 6 mm = 45.7 cm G = 28 GPA for both femurs compute: C. twist angles and the maximum and minimum shear stresses D. torsional stiffness k T Answers A. r i = r / 2 0.707 r = 3/2 r 1.255 r C. old: θ = 3.5 τ max = 22.4 Pa τ min = 0 Pa new: θ = 1.75 τ max = 13.7 Pa τ min = 7.92 Pa D. old: k T = 125 N-m new: k T = 250 N-m - 7 -