Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of...

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Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics of Materials: An Introductory Course with Integration of Theory, Analysis, Verification and Design Hartley T. Grandin, Jr. Worcester Polytechnic Institute Joseph J. Rencis University of Arkansas
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Page 1: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

Mechanical Engineering Session March 18, 2006

2006 New England Section American Society of Engineering Education Conference

A New Approach to Mechanics of Materials: An Introductory Course with Integration of

Theory, Analysis, Verification and DesignHartley T. Grandin, Jr.

Worcester Polytechnic InstituteJoseph J. Rencis

University of Arkansas

Page 2: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Outline

1. Theory

2. Analysis

3. Verification

4. Design

5. Examples

6. Conclusion

Page 3: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Theory

• Typical of a One Semester Course• Topics

1. Planar Equilibrium Analysis of a Rigid Body2. Stress3. Strain4. Material Properties and Hooke’s Law5. Centric Axial Tension and Compression6. Torsion7. Bending8. Combined Analysis9. Static Failure Theories10. Columns

• Commonly Found in Textbooks

Page 4: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Analysis

• Structured Problem Solving Format1. Model

2. Free-Body Diagrams

3. Equilibrium Equations

4. Material Law Formulas

5. Compatibility and Boundary Conditions

6. Complementary and Supporting Formulas

7. Solve

8. Verification

• Textbooks• Headings to Solve Problem Commonly Used• Craig – Closest to us! But does not use structured format.

Blue Steps for Statics

Page 5: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Analysis ‘Continued’

7. Solve

a) Traditional – w/ Values and/or

– Symbolic

b) Ours– Do Not Isolate Known and Unknown Variables– No Algebraic Manipulation – Reduces Errors!– Engineering Tool – Student Choice

c) No Textbook Does This!

CBAx PPRF =+=∑ ;0

KnownsUnknown

PPR BCA

=−=

CBA PPR =+

Page 6: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Verification

• Question and Test to Verify the “Answers”

• Suggested Questions– A Hand Calculation?– Comparison w/ a Known Problem Solution?– Examination of Limiting Cases w/ Known Solutions?– Examination of Obvious Known Solutions?– Your Best Judgment?– Comparison w/ Experimentation? – Not done in course.

X

w(0)

w(L)

x

AB

L

+ =

Page 7: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Verification ‘Continued’

• Important Educational Elements– Reflex Suspicion of Program Results

– Check Results with Alternative Methods

• Expected of Professionals

• Expect Student to be Professional

• Textbook by Craig

– Intuitive Discussion for One Solution

– No Numerical Testing

– We Do Both Since We Use Engineering Tools! Allows for Multiple Calculations Easily.

Page 8: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Design

• Design is Where you Search for Optimum Solution– Interchanging Role of Known & Unknown Variables

• ABET Criteria 3c & Criteria 4 (now in 3c)

• Textbooks – Homework & Computer– Traditional

• Typically Single Solution for a Single Set of Specific Requirements

– Ours• Multiple Solution for Any Set of Requirements

• Easily Change Known & Unknown Variables

Page 9: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Example 1: Statically DeterminateAxially Loaded Bar

Determine the displacement at B and C.

Solve using the given specifications:• PB = - 18.0 kN• L1 = 0.508 m • d1 = 40 mm• E1 = 207 GPa: Steel

• PC = 6.0 kN• L2 = 0.635 m• d2 = 30 mm• E2 = 69 GPa: Aluminum

X

L L1 2

P P

A B CB C(1) (2)

y

d2d1

x

Page 10: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

1. Model

• Problem Defined & Figure Labeled Symbolically

• Identify Loading Model– Axial, Torsion and/or Transverse

• State Assumptions• Define Coordinate Set

X

L L1 2

P P

A B CB C(1) (2)

y

d2d1

Page 11: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

2. Free-Body Diagrams

• Complete and/or Parts of Structure• Symbolic Variables – Even Knowns!

R

F

L L1 2

uu

P P

P

A B C

BC

A

B C

C

PB

A BFBD I

B CFBD II

Very Thin IMAGINARY sliceshown for clarity of solution only.

(1) (2)

FB(1)

(2)

Assumed Deformation

(a)

(b)

(c)

(d)

x

x

y

B

(1)

(1)

FB

(1)

Page 12: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

3. Equilibrium Equations

• Symbolic Equations• Check Dimensional Homogeneity• Do Not Isolate Unknowns

– Reduces Algebraic Error!

)2(:

)1(:)1(

)1(

CBB

AB

PPFIIFBD

RFIFBD

+==

R

F

L L1 2

uu

P P

P

A B C

BC

A

B C

C

PB

A BFBD I

B CFBD II

Very Thin IMAGINARY sliceshown for clarity of solution only.

(1) (2)

FB(1)

(2)

Assumed Deformation

(a)

(b)

(c)

(d)

x

x

y

B

(1)

(1)

FB

(1)

Page 13: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

4. Compatibility and Boundary Conditions

• Symbolic Equations• Do Not Isolate Unknowns

– Reduces Algebraic Error!• Done for Statically

– Determinate (Not Common) and– Indeterminate Problems

• Done for Both Problems in Textbooks by– Craig– Crandall, Dahl, Lardner– Shames

Treat Both Problems the Same Way!

Page 14: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

4. Compatibility and Boundary Conditions ‘Continued’

• Compatibility– Displacement at Identical Points of Segment Equal

• Boundary Condition– uA = 0 for Rigid Support

R

F

L L1 2

uu

P P

P

A B C

BC

A

B C

C

PB

A BFBD I

B CFBD II

Very Thin IMAGINARY sliceshown for clarity of solution only.

(1) (2)

FB(1)

(2)

Assumed Deformation

(a)

(b)

(c)

(d)

x

x

y

B

(1)

(1)

Page 15: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

5. Material Law Formulas• Symbolic Equations• Do Not Isolate Unknowns – Reduces Error!• Check Dimensional Homogeneity

F

u

y

uL

F x

u(x)

ba

a

b

a b

A, E Constant

AE

LFuu b

ab +=

)3(:)1(11

1)1(

EA

LFuuSegment B

AB +=

)4(:)2(22

2

EA

LPuuSegment C

BC +=

R

F

L L1 2

uu

P P

P

A B C

BC

A

B C

C

PB

A BFBD I

B CFBD II

Very Thin IMAGINARY sliceshown for clarity of solution only.

(1) (2)

FB(1)

(2)

Assumed Deformation

(a)

(b)

(c)

(d)

x

x

y

B

(1)

(1)F

B

(1)

Page 16: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

6. Complementary and Supporting Formulas

• Complementary Formulas– Stress, Strain, Stiffness, etc.

• Supporting Formulas– Cross-sectional Area– Polar Moment of Inertia– Centroid Location– Moment of Inertia, etc.

)(4

21

1 id

= )(4

22

2 iid

=

Page 17: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

7. Solve

• # Independent Equations = 4• # Unknowns = 4

– RA, , uB and uC

• Solution by– Hand – Requires Algebraic Manipulation

• Coupled Equations – Indeterminate

• Nonlinear Equations

– Engineering Tool• ABET Criteria 3k

• Not Found in Textbooks

)1(BF

)2(:

)1(:)1(

)1(

CBB

AB

PPFIIFBD

RFIFBD

+==

)3(:)1(11

1)1(

EA

LFuuSegment B

AB +=

)4(:)2(22

2

EA

LPuuSegment C

BC +=

Page 18: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

8. Verification

• Comments– May not Yield Absolute Proof

– Does Improve the Level of Confidence

• Step 7. Solves Problem Once• Step 8. Solves Problem Multiple Times

– Need Engineering Tool!

• Compare to– Hand Solution

– Similar Problems in other Texts

Page 19: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

8. Verification ‘Continued’

X

L L1 2

P P

A B CB C(1) (2)

• Uniform, Homogenous w/ PB = 0

• Uniform, Homogenous w/ PC = 0

• E1 ∞ Yields– uB = 0

• E2 ∞ Yields uB = uC=

• E1 ∞ and E2 ∞ Yields uB = uC = 0

• PB = - PC Yields uB = 0 &

AELLPu CC )( 21 +=

111 EALPuu BBC ==

222 )( EALPu CC =

111))(( EALPP CB +

x

y

222 )( EALPu CC =

Page 20: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Example 2: Statically IndeterminateAxially Loaded Bar

• All Equations the Same as Example 1

• Determinate Problem – Example 1– PC = Known

– uC = Unknown

• Indeterminate Problem – Example 2– PC = Unknown

– uC = Known = 0

– Only Requires Changing Known and Unknown

L L1 2

A B C

y

xPB(2)(1)

X

L L1 2

P P

A B CB C(1) (2) x

Page 21: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Example 3: Design Application of Example 2

• Find d2 to limit uB to -20 μm

• Solution Alternative 1– Iterate Input d2

– Solve uB

• Solution Alternative 2– Plot d2 versus uB

• Solution Alternative 3– uB = - 20 μm (Known)

– d2 = Unknown

L L1 2

A B C

y

xPB(2)(1)

Commonly Found in Textbooks

• Coupled • Non-linear Solution

• No Intermediate Analyses

d2=?

Page 22: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

Conclusion

• Integrated Approach– Theory– Analysis

• Structured Problem Solving Format• Symbolic Equations• Solution by Engineering Tool

– Verification• Hand Solution• Known Solution• Limiting Cases

– Design• Change Known and Unknown Variables

Page 23: Mechanical Engineering Session March 18, 2006 2006 New England Section American Society of Engineering Education Conference A New Approach to Mechanics.

2006 ASEE NE Section Conference

What do you think?

Joe Rencis

Department of Mechanical Engineering

University of Arkansas

V-mail: 479-575-3153

FAX: 479-575-6982

E-mail: [email protected]