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2.092/2.093 — Finite Element Analysis of Solids & Fluids I Fall ‘09 
Lecture 3 -Analysis of Solids/Structures and Fluids 
Prof. K. J. Bathe MIT OpenCourseWare 
The fundamental conditions to be satisfied are: 
I. Equilibrium: in solids, F = ma; in fluids, conservation of momentum 
II. Compatibility: continuity and boundary conditions 
III. Constitutive relations: Stress/strain law Each joint and each element must be in equilibrium. From last lecture: 
We want to solve KU = R for this system. We know that 
⎤⎡ 
R = 
⎢⎢⎢⎢⎣ 
0 
−P 
0 
0 0 
⎥⎥⎥⎥⎦ 
To solve for K, assume u5 = 1, u1 = u2 = u3 = u4 = 0. Then, the left hand side becomes 
⎤⎡ ⎢⎢⎢⎢⎣ 
k15 k25 k35 
k45 k55 
⎥⎥⎥⎥⎦ 
= R 
where R are the external applied forces corresponding to the imposed displacement. 
Example 
Consider a simple bar: 
1
Lecture 3 Analysis of Solids/Structures and Fluids 2.092/2.093, Fall ‘09 
EA EA 
F = L × [ Displacement u ] → K˜ = L 
Truss bars can only resist axial forces. Note that the length of bar 3 does not change in infinitesimal 
displacement analysis! L0 cos θ = a 
We use the approximations cos θ = 1, sin θ = θ because the displacements are small, and we are performing an infinitesimal displacement analysis. So, L0 = a. 
L1 = L2 ΔL = √12 
AE 
AE 
AE 
AE 
k55 = 2√ 2a + 
a 
; 
k15 = − 2√ 2a 
; 
k25 = − 2√ 2a 
2
Lecture 3 Analysis of Solids/Structures and Fluids 2.092/2.093, Fall ‘09 
⎤ 
⎡ 
K = 
AE 
a 
⎢⎢⎢⎢⎢⎢⎢⎢⎣ 
1 
.... 
− 2√ 2 
1 
.... 
− 2√ 2 
.... 
0 
.... 0 
1 
.... 2√ 2 +1 
⎥⎥⎥⎥⎥⎥⎥⎥⎦ 
Using this method, we can construct the whole stiffness matrix with the displacement boundary conditions removed. Our KU = R becomes 
⎤⎡⎤⎡ 
⎤ 
⎡ 
Kaa Kab 
Ra 
⎢⎣ ⎥⎦ 
ua 
5×55×3 
⎦ = 
Kba Kbb ub Rb 
3×53×3 
⎣ 
⎣⎦ 
⎤⎡ 
⎤⎡ 
R1u1 
⎤⎡ 
u6 
⎤⎡ 
R6 
⎢⎢⎢⎢⎢⎢⎣ ⎥⎥⎥⎥⎥⎥⎦ 
and 
ub 
= ; Ra = 
⎢⎢⎢⎢⎢⎢⎣ ⎥⎥⎥⎥⎥⎥⎦ 
R2 
R3 
R4 u2 
u3 
u4 
⎢⎣ ⎥⎦ ⎢⎣ ⎥⎦ 
and Rb = 
R7 
= 
ua 
u7 R8u8 
u5 R5 
Now we have the simplified equation KaaUa = Ra. Solve for Ua, and then the reactions are Rb = KbaUa. Also note: “Linear analysis” means that for any constants α, β, 
KU1 = R1, KU2 = R2 → K (αU1 + βU2)= αR1 + βR2 To see why the solutions in linear analysis are unique, please see p. 239 in the textbook: Bathe, K.J. Finite Element Procedures. Cambridge, MA: Klaus-J¨ 
urgen Bathe, 2007. ISBN: 978-0979004902. 
3
MIT OpenCourseWare 
http://ocw.mit.edu 
2.092 / 2.093 Finite Element Analysis of Solids and Fluids I 
Fall 2009 
For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.

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Mit2 092 f09_lec03

  • 1. 2.092/2.093 — Finite Element Analysis of Solids & Fluids I Fall ‘09 Lecture 3 -Analysis of Solids/Structures and Fluids Prof. K. J. Bathe MIT OpenCourseWare The fundamental conditions to be satisfied are: I. Equilibrium: in solids, F = ma; in fluids, conservation of momentum II. Compatibility: continuity and boundary conditions III. Constitutive relations: Stress/strain law Each joint and each element must be in equilibrium. From last lecture: We want to solve KU = R for this system. We know that ⎤⎡ R = ⎢⎢⎢⎢⎣ 0 −P 0 0 0 ⎥⎥⎥⎥⎦ To solve for K, assume u5 = 1, u1 = u2 = u3 = u4 = 0. Then, the left hand side becomes ⎤⎡ ⎢⎢⎢⎢⎣ k15 k25 k35 k45 k55 ⎥⎥⎥⎥⎦ = R where R are the external applied forces corresponding to the imposed displacement. Example Consider a simple bar: 1
  • 2. Lecture 3 Analysis of Solids/Structures and Fluids 2.092/2.093, Fall ‘09 EA EA F = L × [ Displacement u ] → K˜ = L Truss bars can only resist axial forces. Note that the length of bar 3 does not change in infinitesimal displacement analysis! L0 cos θ = a We use the approximations cos θ = 1, sin θ = θ because the displacements are small, and we are performing an infinitesimal displacement analysis. So, L0 = a. L1 = L2 ΔL = √12 AE AE AE AE k55 = 2√ 2a + a ; k15 = − 2√ 2a ; k25 = − 2√ 2a 2
  • 3. Lecture 3 Analysis of Solids/Structures and Fluids 2.092/2.093, Fall ‘09 ⎤ ⎡ K = AE a ⎢⎢⎢⎢⎢⎢⎢⎢⎣ 1 .... − 2√ 2 1 .... − 2√ 2 .... 0 .... 0 1 .... 2√ 2 +1 ⎥⎥⎥⎥⎥⎥⎥⎥⎦ Using this method, we can construct the whole stiffness matrix with the displacement boundary conditions removed. Our KU = R becomes ⎤⎡⎤⎡ ⎤ ⎡ Kaa Kab Ra ⎢⎣ ⎥⎦ ua 5×55×3 ⎦ = Kba Kbb ub Rb 3×53×3 ⎣ ⎣⎦ ⎤⎡ ⎤⎡ R1u1 ⎤⎡ u6 ⎤⎡ R6 ⎢⎢⎢⎢⎢⎢⎣ ⎥⎥⎥⎥⎥⎥⎦ and ub = ; Ra = ⎢⎢⎢⎢⎢⎢⎣ ⎥⎥⎥⎥⎥⎥⎦ R2 R3 R4 u2 u3 u4 ⎢⎣ ⎥⎦ ⎢⎣ ⎥⎦ and Rb = R7 = ua u7 R8u8 u5 R5 Now we have the simplified equation KaaUa = Ra. Solve for Ua, and then the reactions are Rb = KbaUa. Also note: “Linear analysis” means that for any constants α, β, KU1 = R1, KU2 = R2 → K (αU1 + βU2)= αR1 + βR2 To see why the solutions in linear analysis are unique, please see p. 239 in the textbook: Bathe, K.J. Finite Element Procedures. Cambridge, MA: Klaus-J¨ urgen Bathe, 2007. ISBN: 978-0979004902. 3
  • 4. MIT OpenCourseWare http://ocw.mit.edu 2.092 / 2.093 Finite Element Analysis of Solids and Fluids I Fall 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.