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Published byJoy Williams Modified over 9 years ago
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DEFORMING
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Stress strain behavior of ductile materials σ ε Elastic-plastic with strain hardening Elastic-perfectly plastic Rigid perfectly plastic Rigid plastic with strain hardening
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Topics for today’s lecture Deformation processes ⊙ Deforming process characteristics ⊙ Deforming physics ⊙ Common deforming processes ⊙ DFM
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Process characteristics Material/continuum changes during processing ⊙ Machining = Local, concentrated ⊙ Deforming = Over large volume Force ⊙ Machining: ~10s - 100s of lbs ⊙ Stamping: ~10s - 100s of tons Materials - Virtually all ductile materials Shapes - Limited by strain/flow Size - Limited by force/equipment
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Advantages and disadvantages Advantages ⊙ Parallel process: rapid bulk formation ⊙ Overall material properties improved Disadvantages ⊙ Cost of equipment and dies ⊙ Limited flexibility in shapes and sizes (i.e. compared to machining ⊙ Accuracy ⊙ Repeatability
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Important physics Stress/strain ⊙ Affect CQFR ⊙ Affect deforming force -> equipment & energy requirements Friction ⊙ Affect on deforming force -> equipment & energy requirements ⊙ Why lubrication is needed and can help ⊙ Friction is not repeatable… quality….
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Stress strain behavior of ductile materials σ ε Elastic-plastic with strain hardening Elastic-perfectly plastic Rigid perfectly plastic Rigid plastic with strain hardening
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Example: 12L14 Steel in Duratec 12L14 Steel True Stress-Strain Behavior Intercept Tangent modulus 0.41 GPa [0.06 Mpsi] Young’s modulus 190 GPa [27.4 Mpsi] Strain, mm / mm Stress, MPa Stress, kpsi
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Forging force and friction Axisymmetric upsetting Purpose ⊙ Find F z (µ ) ⊙ Sensitivity Assumptions: ⊙ Tresca flow ⊙ Constant friction coefficient ⊙ Plastic deformation
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Forging force and friction Eqxn: A – Equilibrium in r direction dF inner arc dF friction top & bottom dF hoop dF outer arc Eqxn: B -Tresca Yield Criterion
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Forging force and friction Y=75000 psi h = ½ inch Affect of friction on contact pressure Distance from center line [inches] Contact pressure [psi]Increasing µ mu = 0 mu =.1 mu =.2 mu =.5
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Forging force and friction cont. Now use Taylor’s series expansion (3 terms) to approximate the exponential function Expand about 0, makes this approximation valid for small values of 2µ R/h
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Forging force and friction Affect of part size and friction on forging force Forging force [tons] Part size [inches] mu = 0 mu =.1 mu =.2 mu =.5 Increasing µ Y=75000 psi h = ½ inch
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Common processes Sheet metal Forging Extrusion Rolling
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Bending and shearing
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Forging Blank Edging Blocking Finishing Trimming
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Rolling and extrusion
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Affect of grain size Properties affected by grain size ⊙ Strength ⊙ Hardness ⊙ Ductility ⊙ For example (Ferrite) We desire smaller grains for better properties
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Recrystallization Recrystallization and Grain Growth in Brass Figure 7.21 Callister http://www.mmat.ubc.ca/other/courses/apsc278/lecture11.pdf 8s at 580 C: completc recrystallization 3s at 580 C: initial recrystallization 4s at 580 C: partial replacementCold- worked(33% CW) l5 min at 590 C: grain growth 10 min at 700 C: grain growth
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DFM for deforming processes Parting line and flash Draft angle Radii Lubrication
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Mechanics of spring back Q: Why do we see spring back? A: Elastic recover of material
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Example: Elastic spring back Example: Bending wire
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Quantifying elastic spring back Elastic recovery of material leads to spring back ⊙ Y = Yield stress E = Young’s Modulus t = thickness ⊙ ⊙ With increase in Ri / t or Y OR decrease in E spring back increases Titanium Steel Increasing
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