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

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

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

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

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

Torsion of Shafts Learning objectives

MECE 3321: MECHANICS OF SOLIDS CHAPTER 5

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

PROBLEM #1.1 (4 + 4 points, no partial credit)

Chapter Objectives. Copyright 2011 Pearson Education South Asia Pte Ltd

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

Aluminum shell. Brass core. 40 in

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

MECHANICS OF MATERIALS

Free Body Diagram: Solution: The maximum load which can be safely supported by EACH of the support members is: ANS: A =0.217 in 2

Mechanical Design in Optical Engineering

MECHANICS OF MATERIALS Sample Problem 4.2

Structural Analysis I Chapter 4 - Torsion TORSION

Mechanics of Materials MENG 270 Fall 2003 Exam 3 Time allowed: 90min. Q.1(a) Q.1 (b) Q.2 Q.3 Q.4 Total

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

[5] Stress and Strain

If the solution does not follow a logical thought process, it will be assumed in error.

MECHANICS OF MATERIALS

σ = Eα(T T C PROBLEM #1.1 (4 + 4 points, no partial credit)

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

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

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

CIVL222 STRENGTH OF MATERIALS. Chapter 6. Torsion

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

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

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.

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

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)?

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

Stress and Strain ( , 3.14) MAE 316 Strength of Mechanical Components NC State University Department of Mechanical & Aerospace Engineering

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.

Problem d d d B C E D. 0.8d. Additional lecturebook examples 29 ME 323

(48) CHAPTER 3: TORSION

Symmetric Bending of Beams

The science of elasticity

Outline. Organization. Stresses in Beams

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

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

Solution ME 323 EXAM #2 FALL SEMESTER :00 PM 9:30 PM Nov. 2, 2010

Solid Mechanics Homework Answers

BME 207 Introduction to Biomechanics Spring 2017

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

Name (Print) ME Mechanics of Materials Exam # 1 Date: October 5, 2016 Time: 8:00 10:00 PM

INTRODUCTION TO STRAIN

Stress-Strain Behavior

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

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

Comb Resonator Design (2)

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

Advanced Structural Analysis EGF Section Properties and Bending

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

ME311 Machine Design

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

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

WORCESTER POLYTECHNIC INSTITUTE

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

Mechanics of Materials

CHAPTER 4: BENDING OF BEAMS

ME 323 MIDTERM # 1: SOLUTION FALL SEMESTER Time allowed: 1hour

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

Strength of Material. Shear Strain. Dr. Attaullah Shah

Sample Question Paper

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

Mechanical Properties of Materials

The University of Melbourne Engineering Mechanics

MINISTRY OF EDUCATION AND SCIENCE OF UKRAINE. National aerospace university Kharkiv Aviation Institute. Department of aircraft strength

STANDARD SAMPLE. Reduced section " Diameter. Diameter. 2" Gauge length. Radius

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

and F NAME: ME rd Sample Final Exam PROBLEM 1 (25 points) Prob. 1 questions are all or nothing. PROBLEM 1A. (5 points)

Solid Mechanics Chapter 1: Tension, Compression and Shear

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

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

Comb resonator design (2)

Spherical Pressure Vessels

Fig Example 8-4. Rotor shaft of a helicopter (combined torsion and axial force).

University of Pretoria Department of Mechanical & Aeronautical Engineering MOW 227, 2 nd Semester 2014

External Work. When a force F undergoes a displacement dx in the same direction i as the force, the work done is

Unified Quiz M4 May 7, 2008 M - PORTION

Sub. Code:

Torsion of shafts with circular symmetry

PES Institute of Technology

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

= 50 ksi. The maximum beam deflection Δ max is not = R B. = 30 kips. Notes for Strength of Materials, ET 200

ME325 EXAM I (Sample)

Torsion Stresses in Tubes and Rods

MECHANICS LAB AM 317 EXP 4 TORSION OF CIRCULAR RODS

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.

Lecture 5: Pure bending of beams

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 6

MECHANICS OF MATERIALS REVIEW

Stresses in Curved Beam

CHAPTER 2 Failure/Fracture Criterion

Purpose of this Guide: To thoroughly prepare students for the exact types of problems that will be on Exam 3.

By Dr. Mohammed Ramidh

Russell C. Hibbeler. Chapter 1: Stress

Transcription:

Problem 10.4 A prismatic bar with length L 6m and a circular cross section with diameter D 0.0 m is subjected to 0-kN compressive forces at its ends. The length and diameter of the deformed bar are measured and determined to be L 5.940 m and D 0.0006 m. What are the modulus of elasticity and Poisson s ration of the material? The strain in the bar is: ε L L L 5.94 m 6.0 m 6.0 m 0.01 The compressive stress in the bar is: σ P 0, 000 N 63.7 MPa A π(0.01 m) The modulus of elasticity for the material is: E σ 63.7 MPa ε 0.01 E 6.37 GPa Poison s ration for the material is: υ ε LAT ε υ 0.3 (D D)/D ε (0.0006 m 0.0 m)/0.0 m 0.01 Problem 10.5 The bar has modulus of elasticity E 30 10 6 psi and Poisson s ration ν 0.3. It has a circular cross section with diameter D 0.75 in. What compressive force would have to be eerted on the right end of the bar to increase its diameter to 0.75 in? From the definition of Poisson s ratio: (0.75 in 0.75 in)/0.75 in 0.3 ε The strain which will be produced by the applied load is: ε σ ( )( E P π(0.375 in) 1 30 10 6 lb/in Substituting the above epression for the strain into the epression for Poisson s ratio: (0.75 in 0.75 in)/0.75 in 0.3 ( (P/(π(0.375 in) )) P 110.4 kip ) 1 30 10 6 lb/in )

Problem 11.1 A cube of material is subjected to a pure shear stress τ 9 MPa. The angle β is measured ad determined to be 89.98. What is the shear modulus G of the material? Diagram: Converting the shear strain angle into radians: γ (90 89.98 ) 180 π 3.49 10 4 radians Using the definition of the shear modulus: G τ γ 9 106 N/m 3.49 10 4 G 5.8 GPa Problem 11. If the cube in Problem 11.1 consists of material with shear modulus G 4.6 10 6 psi and the shear stress τ 8000 psi, what is the angle β in degrees? The shear strain will be: γ τ G The angle β is: 8, 000 lb/in 4.6 10 6 lb/in 1.739 10 3 radians 0.0996 β 89.9 β 90 γ 90 0.0996 Problem 11.3 If the cube in Problem 11.1 consists of aluminum alloy that will safely support a pure stress of 70 MPa and G 6.3 GPa, what is the largest shear strain to which the cube can safely be subjected? The shear strain will be: γ 0.0103 γ τ G 70 106 N/m 6.3 10 9 N/m 0.01066

Problem 11.13 The bar has a circular cross section with 15-mm diameter and the shear modulus of the material is G 6GPa. If the torque T 10N m, determine (a) the magnitude of the maimum shear stress in the bar; (b) the angle of twist of the end of the bar in degrees. J π c4 π (0.0075m)4 J 4.97 10 9 m 4 Maimum shear stress in the bar is: τ MAX Tρ J (10 N m) (0.0075 m) 4.97 10 9 (a) τ MAX 15.1 10 6 N/m The angle of twist for the bar is: φ LT JG (0.8m)(10 N m) (4.97 10 9 m 4 )(6 10 9 N/m ) φ 0.0619 rad 3.547 Problem 11.14 If the bar in Problem 11.13 is subjected to a torque T that causes the end of the bar to rotate 4, what is the magnitude of the maimum shear stress in the bar? The polar moment of inertia for the cross section is: J π c4 π (0.0075)4 4.97 10 9 Using the angle of rotation at the end of the bar to determine the applied torque: ( 4 ) 180 (π) rad TL JG (0.8 m)(t ) (4.97 10 9 m 4 )(6 10 9 N/m ) T 11.7 N m Maimum shear stress in the cross section is: τ MAX Tc J τ MAX 17.01 MPa (11.7 N m)(0.0075 m) 4.97 10 9 m 4

Problem 11.17 Consider the solid circular shaft in Problem 11.16. The shear modulus of the material is G 80GPa. What angle of twist per unit meter of length is caused by the -MN-m torque? J π c4 π (0.4 m)4 0.040 m 4 The angle of twist per meter of length is: φ L T JG 10 6 N m (0.040 m 4 )(80 10 9 N/m ) φ 0.0006 rad/m 0.0356 degrees/m L Problem 11.18 If the shaft in Problem 11.16 has a hollow circular cross section with 0.5-m outer radius and 0.3-m inner radius, what is the maimum shear stress? The polar moment of inertia for the hollow shaft is: J π (ro r i) π [(0.5 m) 4 (0.3 m) 4] J 0.0855 m 4 Maimum shear stress in the shaft is: τ MAX Tρ ( 10 6 J N m ) (0.5 m) 0.0855 m 4 τ MAX 11.7 MPa

Problem 11.19 The propeller of the wind generator is supported by a hollow circular shaft with 0.4-m outer radius and 0.3-m inner radius. The shear modulus of the material is G 80GPa. If the propeller eerts an 840- kn-m torque on the shaft, what is the resulting maimum shear stress? J [(0.4 π m) 4 (0.3 m) 4] J 0.075 m 4 Maimum shear stress in the shaft is: τ MAX Tc J τ MAX 1. MPa (840, 000 N m) (0.4 m) 0.075 m 4 Problem 11.0 In Problem 11.19, what is the angle of twist of the propeller shaft per meter of length? J [(0.4 π m) 4 (0.3 m) 4] J 0.075 m 4 Angle of twist for the shaft is: φ LT JG (1 m) (840, 000 N m) (0.075 m 4 ) (80 10 9 N/m ) φ 0.00038 rad 0.019

Problem 11.1 In designing a new shaft for the wind generator in Problem 11.19, the engineer wants to limit the maimum shear stress in the shaft to 10 MPa, but design constraints require retaining the 0.4-m outer radius. What new inner radius should she use? J [(0.4 π m) 4 (r i ) 4] J 0.040 1.571ri 4 Maimum shear stress in the shaft is: τ MAX Tc J (840, 000 N m) (0.4 m) (0.040 1.571r 4 i ) 10 10 6 N/m r i 0.546 m Problem 11. The bar has a circular cross section with 1-in. diameter and the shear modulus of the material is G 5.8 10 6 psi. If the torque T 1000 in lb, determine (a) the magnitude of the maimum shear stress in the bar; (b) the magnitude of the angle of twist of the right end of the bar relative to the wall in degrees. Maimum torque in the shaft is 1,000 in-lb. J π (0.5 in)4 J 0.098 in 4 (a) Maimum shear stress in the shaft is: τ MAX TC J τ MAX 509.958 lb/in (1, 000 in lb) (0.5 in) 0.098 in 4 (b) The angle of twist in the 8-inch section of the bar is: φ 8in (8 in)(500 in lb)) (0.098 in 4 )(5.8 10 6 in 4 ) φ 8in 0.0070 rad 0.40 The angle of twist in the 6-inch section of the bar is: φ 6in (6 in)(1,000 in lb) (0.098 in 4 )(5.8 10 6 lb/in ) φ 6in 0.0105 rad 0.604 Total angle of twist for the bar is: φ φ 8in + φ 6in 0.40 +0.604 φ 1.006

Problem 11.3 For the bar in Problem 11., what value of the torque T would cause the angle of twist of the end of the bar to be zero? The torque in the 8-inch section of the bar is (T 500 in lb). The torque in the 6-inch section of the bar is T. The equation for total angle of twist for the bar is: 0 L 8inT 8in JG + L 6inT 6in JG Solving the equation for T : T 86 in lb (8 in) (T 500 in lb) (6 in) T + JG JG Problem 11.4 Part A of the bar has a solid circular cross section and Part B has a hollow circular cross section. The shear modulus of the material is G 3.8 10 6 psi. Determine the magnitudes of the maimum shear stresses in parts A and B of the bar. The torque in the solid section of the bar is 50,000 in-lb. The torque in the hollow section of the bar is 100,000 in-lb. Polar moment of inertia for the solid section of the bar is: J S π ( in)4 5.13 in 4 Polar moment of inertia for the hollow section of the shaft is: J H π [ ( in) 4 (1 in) 4] 3.56 in 4 Maimum shear stress in the solid section of the bar is: (τ MAX ) S T Sc S J S (50, 000 in lb) ( in) 5.13 in lb (τ MAX ) S 19, 896.54 lb/in 19.89 ksi Maimum shear stress in the hollow section of the bar is: (τ MAX ) H T Hc H J H (100, 000 in lb) ( in) 3.56 in 4 (τ MAX ) H 8, 488.96 lb/in 8.49 ksi

Problem 11.5 For the bar in Problem 11.4, determine the magnitude of the angle of twist of the end of the bar in degrees. The torque in the solid section of the bar is 50,000 in-lb. The torque in the hollow section of the bar is 100,000 in-lb. Polar moment of inertia for the solid section of the bar is: J S π ( in)4 5.13 in 4 Polar moment of inertia for the hollow section of the shaft is: J H π [ ( in) 4 (1 in) 4] 3.56 in 4 The angle of twist for the solid section of the shaft is: φ L ST S (7 in) (50, 000 in lb) ( J S G S 5.13 in 4 )( 3.8 10 6 lb/in ) φ S 0.0183 rad 1.05 The angle of twist for the hollow section of the shaft is: φ L HT H (14 in) (100, 000 in lb) ( J H G H 3.56 in 4 )( 3.8 10 6 lb/in ) φ H 0.0156 rad 0.896 Total angle of twist for the shaft is: φ 1.95 φ t φ S + φ H 1.05 +0.896 Problem 11.6 For the bar in Problem 11.4, determine the magnitude of the maimum shear stresses in parts A and B of the bar and the magnitude of the angle of twist of the end of the bar in degrees if the 150 in-kip couple acts in the opposite direction. Polar moments of inertia for the two sections of the bar are: J A π (in)4 5.13 in 4 J B π [ (in) 4 (1in) 4] 3.56 in 4 From the FBD we see that the torque in the sections of the bar is: T A 50, 000 in lb T B 100, 000 in lb Maimum shear stresses in the sections of the bar are: (50, 000 in lb)( in) (100, 000 in lb)( in) (τ A ) MAX 5.13 in 4 (τ B ) MAX 3.56 in 4 (τ A ) MAX 3, 980 lb/in (τ B ) MAX 8, 488.96 lb/in 8.49 ksi The angles of twist in each of the sections of the bar are: (50, 000 in lb)(7 in) (100, 000 in lb)(14 in) φ A (5.13 in 4 )(3.8 10 6 lb/in φ B ) (3.56 in 4 )(3.8 10 6 lb/in ) φ A 0.00367 radians Total angle of twist is: φ B 0.01564 radians φ φ A + φ B 0.00367 rad + 0.01564 rad φ 0.01197 rad 0.686

Problem 7.6 Determine the y coordinate of the centroid of the area in Problem 7.5. Let y in Equation (7.7) be the height of the midpoint of a vertical strip: R 1 [ ] yda A y h (R ) 1/ (R ) 1/ d. da da A The upper integral is R 1 h (R ) d 1 ] R [R 3 3 h 1 ( R 3 A 3 R h + h3 3 ). y h y ½(R ) ½ d From the solution of Problem 7.5, [ A da R ) 1/ ( ) πr (1 ] A h h h R R arcsin. R ( ) The centroid is y 1 R 3 R A 3 h + h3 3 Determine the coordinates of the cen- Problem 7.7 troids. y Let us solve this by parts. 40 mm A 1 A h b 60 mm l 40 mm h 40 mm 60 mm 40 mm b l b 60mm l 40mm h 40mm y A 1 1 bh 1 (60)(40) 100 mm 40 mm A lh (40)(40) 1600 mm A 1 + A 800 mm From the tables and inspection 60 mm 40 mm 1 3 b b + l/z y 1 1 3 h y 1 h 1 40mm 80mm y 1 13.33 mm y 0mm For the composite, substituting, 1A 1 + A A 1 + A y y 1A 1 + y A A 1 + A 6.9 mm 17.1 mm

Determine the coordinates of the cen- Problem 7.8 troids. y 0 mm 60 mm 30 mm 70 mm Let us solve this problem by using symmetry and by breaking the composite shape into parts. l 1 0 mm y A 1 h 1 0 mm 60 mm A h l 1 70 mm h 1 70 mm l 70 mm h 70 mm 60 mm l 30 mm l 1 70mm 70 mm h 1 0mm l 30mm h 60mm A 1 l 1 h 1 1400 mm A l h 1800 mm By symmetry, 1 0 0 y 1 70mm y 30mm For the composite, 1A 1 + A 0+0 A 1 + A 30 mm 0 y y 1A 1 + y A A 1 + A (70)(1400) + (30)(1800) y 300 y 47.5mm 0 15000 300