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Thermal Stresses Jake Blanchard Spring 2008

Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

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Page 1: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Thermal StressesJake BlanchardSpring 2008

Page 2: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Temp. Dependent PropertiesFor most materials, k is a function of

temperatureThis makes conduction equation nonlinearANSYS can handle this with little input from usExamples:

◦Copper: k=420.75-0.068493*T (W/m-K; T in K)◦Stainless Steel: k=9.01+0.015298*T◦Plot these vs. Temperature from 300 K to 1000 K

◦Try:◦MP,KXX,1,420.75,-0.068493

Page 3: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Incorporating into ANSYSInput polynomial coefficients into

Material TableSet nonlinearity parametersEverything else is the same

Page 4: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

In-Class Problems

Material 1 is CuMaterial 2 is SS

21

10 cm

1 cm

q=104 W/m2

h=1000 W/m2-KTb=50 C

Page 5: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Thermal StressesThermal stresses occur when

there is differential expansion in a structure◦Two materials connected, uniform

temperature change (different thermal expansion coefficients lead to differential expansion)

◦Temperature gradient in single material (differential expansion is from temperature variation)

Page 6: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Treating Thermal Stress in ANSYSTwo options

1. Treat temperature distributions as inputs (useful for uniform temperature changes) – must input thermal expansion coefficient

2. Let ANSYS calculate temperatures, then read them into an elastic/structural analysis

Page 7: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Prescribing temperaturesUse: Preprocessor/Loads/Define

Loads/Apply/Structural/Temperature/On Areas (for example)

Page 8: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Sample

1=2*10-6 /KE1=200 GPa1=0.32=5*10-6 /KE2=100 GPa2=0.28Increase T by 200 CInner radius=10 cmCoating thickness=1 cm

2

1

Page 9: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Calculating both temp and stress

Set jobname to ThermTest (File/Change Jobname…)Main Menu/Preferences/Structural&Thermal&h-

methodInput structural and thermal propertiesCreate geometry and meshInput thermal loads and BCsSolve and save .db fileDelete all load data and switch element type to

struct.Edit element options if necessaryApply BCsLoads/Define Loads/Apply/Temperature/from

thermal anal./ThermTest.rthSolve

Page 10: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

Sample

1=2*10-6 /KE1=200 Gpak1=10 W/m-K1=0.32=5*10-6 /KE2=100 Gpak2=20 W/m-K2=0.28Set outside T to 0 CSet heating in 2 to 106 W/m3

Inner radius=10 cmCoating thickness=1 cm

2

1

Page 11: Thermal Stresses Jake Blanchard Spring 2008. Temp. Dependent Properties For most materials, k is a function of temperature This makes conduction equation

In-Class Problems

Channels are 3 cm in diameter

k=20 W/m-KE=200 Gpa=0.3= 10-5 /K

10 cmq=104 W/m2

15 cm

2 cm

h=1000 W/m2-KTb=50 C