materials selection for mechanical design 1 breaking down

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Materials selection for mechanical design 1 Breaking down a design problem Identifying function, objectives, constraints Optimizing performance Ashby plots

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Page 1: Materials selection for mechanical design 1 Breaking down

Materials selection for mechanical design 1

• Breaking down a design problem • Identifying function, objectives, constraints • Optimizing performance • Ashby plots

Page 2: Materials selection for mechanical design 1 Breaking down

• Mechanical response: how does a material respond to loads? • Elastic deformation

• strain: unitless change in dimension • stress: force per area • elastic deformation is reversible upon release of applied forces

• Plastic deformation • permanent deformation is what’s left over • response depends on material history (microstructure)

• Fracture • preexisting cracks/flaws in material, propagate under applied stress • catastrophic failure of material

• Creep • time-dependent permanent deformation to time-independent load • thermally activated response

• Fatigue • fracture response to time-dependent cyclic loading • cycling promotes crack nucleation and growth; catastrophic failure

Mechanical response of materials 2

Page 3: Materials selection for mechanical design 1 Breaking down

• Uniaxial tension test: • Stress: what we do to the material • Strain: how the material responds

• Quantify: • Initial gauge length L0 and area A0; instantaneous length L and area A

Stress-strain diagram 3

Engineering stress

�E =P

A0

�T =PA

True stress

Engineering strain

✏E =�L0=

L � L0

L0

True strain

✏T = lnLL0= ln

A0

A= ln(1 + ✏E)

schematic steel stress-strain curve (not to scale)

Page 4: Materials selection for mechanical design 1 Breaking down

• Engineering vs. true quantities • Engineering: loads and deformation from initial geometry • True: what the material experiences (stress), accumulated/additive

dimension change (strain: 10% true + 10% true = 20% true) • Yield strength: highest stress that the material can withstand without

undergoing significant plastic (irreversible) deformation • May be defined by a yield point (rapid drop in stress at yield) • May be defined as 0.2% offset (stress to get 0.2% plastic strain)

• Ultimate strength: is the maximum value of stress (engineering stress) that the material can withstand

• Fracture stress: the value of stress at fracture • Stiffness: ratio of stress to strain, primarily of interest in the elastic

region. (elastic moduli) • Ductility: Materials that undergo large strain before fracture are classified

as ductile materials. Necks before failure • Percent elongation: 100(Lf−L0)/L0 • Percent reduction in area: 100(A0−Af)/A0

4Stress-strain diagram: features

Page 5: Materials selection for mechanical design 1 Breaking down

! Rupture occurs along a cone-shaped surface that forms an angle of approximately 45° with the original surface of the specimen (“cup-cone” shape)

! Shear is primarily responsible for failure in ductile materials

! Axial loading: maximum shear stress occurs at 45o

Necking Rupture

5Stress-strain diagram: ductile materials

Page 6: Materials selection for mechanical design 1 Breaking down

Ashby plots

Materials selection for mechanical

design:

choose best material among

competing properties

Our goal: understanding mechanisms

responsible for behavior

M. Ashby “Materials Selection in Mechanical Design”

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Page 7: Materials selection for mechanical design 1 Breaking down

PM(M)PG(G)

Materials selectionDesign concerns

function - what a component does constraints - what must/must not occur objective - what is maximized/minimized

M. Ashby, “Materials Selection in Mechanical Design”

function constraint objective

Example: tie-rod stretches to carry load, must not yield, and be lightweight

Rank different designs performance as a function P(F, G, M): functional needs (F) geometry (G) material properties (M)

We assume a separable form: P(F, G, M) = PF(F) PG(G) PM(M) so that material choice can be optimized independent of design specifics, with flexibility

The goal: optimize performance

pmax =2↵⇡r·0BBBB@

K2Ic

�YS

1CCCCA

Ex: maximum pressure in cylindrical vessel to leak, but not fracture:

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Page 8: Materials selection for mechanical design 1 Breaking down

Materials propertiesMaterial properties

mechanical: modulus, yield stress, fracture toughness, ... transport/thermal: heat capacity, thermal expansion, resistivity economic: density, cost/mass

price includes: cost to extract, cost/energy to process, cost/energy to form, cost of disposal, regulation cost

M. Ashby, “Materials Selection in Mechanical Design”

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Page 9: Materials selection for mechanical design 1 Breaking down

Relative material cost/mass

Based on Callister, 6th ed.

Reference material: rolled A36 carbon steel

Relative costs fluctuate less than actual costs over time.

Cost includes both extraction and processing, but not production.

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Page 10: Materials selection for mechanical design 1 Breaking down

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Nucleosynthesis (stellar fusion processes) determines what “raw” materials we have available.

10

Page 11: Materials selection for mechanical design 1 Breaking down

Materials properties and selectionMaterial properties

mechanical: modulus, yield stress, fracture toughness, ... transport/thermal: heat capacity, thermal expansion, resistivity economic: density, cost/mass

price includes: cost to extract, cost/energy to process, cost/energy to form, cost of disposal, regulation cost

Materials selection involves 1. determining combination of properties to maximize (function,

constraint, and objective) 2. selecting material/material class to fill that need

M. Ashby, “Materials Selection in Mechanical Design”

We do selection via an “Ashby plot”: log-log plot of two material properties

PM(M) =M↵11 ·M

↵22 · · ·

log PM(M) = ↵1 log M1 + ↵2 log M2 + · · ·

Why log-log?

Constant (equal) performance is a straight line on an Ashby plot

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Page 12: Materials selection for mechanical design 1 Breaking down

Light, strong tie-rod 12

A tie-rod carries load along its length. We want it to carry the load without yielding, and if it’s in a vehicle, we want a low mass. First: what is the function? A. low mass B. low area C. carry load D. long length E. not yield

Page 13: Materials selection for mechanical design 1 Breaking down

Light, strong tie-rod 13

A tie-rod carries load along its length. We want it to carry the load without yielding, and if it’s in a vehicle, we want a low mass. Next: what is the objective? A. low mass B. low area C. carry load D. long length E. not yield

Page 14: Materials selection for mechanical design 1 Breaking down

Light, strong tie-rod 14

A tie-rod carries load along its length. We want it to carry the load without yielding, and if it’s in a vehicle, we want a low mass. Finally: what is the constraint? A. low mass B. low area C. carry load D. long length E. not yield

Page 15: Materials selection for mechanical design 1 Breaking down

Light, strong tie-rod 15

A tie-rod carries load along its length: • Functional needs: carry load F • Geometry: length L, area A • Constants? F, L • Variables? area A, material • Constraint? stress below yield stress • Performance? mass m

Page 16: Materials selection for mechanical design 1 Breaking down

Light, strong tie-rod 16

A tie-rod carries load along its length: • Functional needs: carry load F • Geometry: length L, area A • Constants? F, L • Variables? area A, material • Constraint? stress below yield stress • Performance? mass m

m = SLFρ

σYS

Page 17: Materials selection for mechanical design 1 Breaking down

Yield strength vs. density

M. Ashby, “Materials Selection in Mechanical Design”

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Page 18: Materials selection for mechanical design 1 Breaking down

Yield strength vs. density

M. Ashby, “Materials Selection in Mechanical Design”

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lines of constant performance?

A B

Page 19: Materials selection for mechanical design 1 Breaking down

Yield strength vs. density

M. Ashby, “Materials Selection in Mechanical Design”

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Page 20: Materials selection for mechanical design 1 Breaking down

Yield strength vs. density

M. Ashby, “Materials Selection in Mechanical Design”

increasing YS/density

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Page 21: Materials selection for mechanical design 1 Breaking down

Light, stiff tie-rod 21

A tie-rod carries load along its length. We want it to carry the load without extending more than length δ, and if it’s in a vehicle, we want a low mass. • Functional needs: carry load F • Geometry: length L, area A • Constants? F, L • Variables? area A, material • Constraint? extension below δ • Performance? mass m

Page 22: Materials selection for mechanical design 1 Breaking down

Light, stiff tie-rod 22

A tie-rod carries load along its length. We want it to carry the load without extending more than length δ, and if it’s in a vehicle, we want a low mass. • Functional needs: carry load F • Geometry: length L, area A • Constants? F, L • Variables? area A, material • Constraint? extension below δ • Performance? mass m

m =SFL2

δρE

Page 23: Materials selection for mechanical design 1 Breaking down

Young’s modulus vs. density

M. Ashby, “Materials Selection in Mechanical Design”

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Page 24: Materials selection for mechanical design 1 Breaking down

Young’s modulus vs. density

increasing E/density

M. Ashby, “Materials Selection in Mechanical Design”

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Page 25: Materials selection for mechanical design 1 Breaking down

Light, strong cantilever 25

A cantilever is fixed at one end, and carries load perpendicular to its length. We want it to carry the load without yielding, we want a low mass. • Functional needs: carry load W • Geometry: length L, diameter d • Constants? W, L • Variables? diameter d, material • Constraint? stress below yield • Performance? mass m

Page 26: Materials selection for mechanical design 1 Breaking down

Light, strong cantilever 26

A cantilever is fixed at one end, and carries load perpendicular to its length. We want it to carry the load without yielding, we want a low mass. • Functional needs: carry load W • Geometry: length L, diameter d • Constants? W, L • Variables? diameter d, material • Constraint? stress below yield • Performance? mass m

m ∝ρ

σ2/3YS

Page 27: Materials selection for mechanical design 1 Breaking down

Yield strength vs. density

M. Ashby, “Materials Selection in Mechanical Design”

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Page 28: Materials selection for mechanical design 1 Breaking down

Yield strength vs. density

increasing YS2/3/density

M. Ashby, “Materials Selection in Mechanical Design”

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Page 29: Materials selection for mechanical design 1 Breaking down

What about cost?Material properties

mechanical: modulus, yield stress, fracture toughness, ... transport/thermal: heat capacity, thermal expansion, resistivity economic: density, cost/mass

price includes: cost to extract, cost/energy to process, cost/energy to form, cost of disposal, regulation cost

M. Ashby, “Materials Selection in Mechanical Design”

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Page 30: Materials selection for mechanical design 1 Breaking down

Young’s modulus vs. cost

increasing E/cost

M. Ashby, “Materials Selection in Mechanical Design”

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Page 31: Materials selection for mechanical design 1 Breaking down

Young’s modulus vs. cost

increasing E1/2/cost

M. Ashby, “Materials Selection in Mechanical Design”

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Page 32: Materials selection for mechanical design 1 Breaking down

• External load does work on a body: change in internal energy • Work = integral of force × distance

• Force = (stress) × (area) • Distance = (strain) × (length)

• stress × strain → energy/volume • If the deformation is recoverable

then so is the energy.

Strain energy density 32

W =Z

F · dr

=

Z(�A0)(L0 d✏)

= V0

Z� d✏

Elastic energy storage density: modulus of resilience

Total strain energy density from fracture: modulus of toughness

ur =12�pl✏pl

=12

�2pl

E

Page 33: Materials selection for mechanical design 1 Breaking down

Young’s modulus vs. yield strength

M. Ashby, “Materials Selection in Mechanical Design”

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Page 34: Materials selection for mechanical design 1 Breaking down

Young’s modulus vs. yield strength

increasing YS2/E

M. Ashby, “Materials Selection in Mechanical Design”

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Page 35: Materials selection for mechanical design 1 Breaking down

Pressure tanks 35

A pressure tank holds a fluid at pressure, and carries load perpendicular to its thickness. We want it to carry the load to yield before fracture, and so that the critical flaw size is larger than the thickness (leak before fracture). • Functional needs: hold pressure p • Geometry: wall thickness t, diameter d • Constants? d • Variables? thickness t, material • Constraint? stress below yield, flaw size above t • Performance? pressure p

Page 36: Materials selection for mechanical design 1 Breaking down

Fracture toughness vs. yield strength

increasing KIc/YS

increasing YS

M. Ashby, “Materials Selection in Mechanical Design”

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Page 37: Materials selection for mechanical design 1 Breaking down

Fracture toughness vs. yield strength

M. Ashby, “Materials Selection in Mechanical Design”

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Page 38: Materials selection for mechanical design 1 Breaking down

• Beginning of design and materials selection • Breaking down a design problem • Identifying function, objectives, constraints • Optimizing performance • Ashby plots

Summary 38