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3. Direct approach – truss analysis
Truss analysis
•Bar – a member in a truss structure• Forces in the bars are either tensile
or compressive – like a spring
3.1 Simple structure consisting of springs- a systematic solution
• Structure
• Element mesh
• Structure + mesh
• Elastic springs• External forces, (N)• Displacements, (m)
• ki spring stiffness, (N/m) • Elements• Nodal points
• Degrees of freedom (DOF)(displacements u1, u2, u3)
1. Element stiffness relation
• Definitions of one element
• Introduce element forces, P1 and P2
Normal force, N(positive in tension) du = u2 - u1
F=k du
P1 = -NP2 = N
, Eq. 1
, Eq. 2
Insert Eq.1 in Eq. 2: In matrix form:
1. Element stiffness relation
• Matrix form
or
where
Ke : element stiffness matrixae : nodal displacement vectorfe : element force vector
From the CALFEM-manual
From the CALFEM-manual
Analogous physical problems
2. Compatibility
Global definitions
Local definitions
Element 1:
Element 2:
Introduce global definitions,(compatibility):
Element 1:
Element 2:
Expanded element formulation:
3. Equilibrium conditions
• Forces acting on each nodal point
Cut the structure at nodes and insert section forces:
Force equilibrium: In matrix form:
4. Assembling
Force equilibrium in matrix form:
Expanded element form:
Element 1:
Element 2:
, Eq. 1
, Eq. 2
Insert Eq.2 in Eq. 1:
4. Assembling
or
where
K : global stiffness matrixa : global displacement vectorf : external force vector
Wich results in the system of linear equations:
5. Boundary conditions
No unique solution:
Introduce boundary conditions:Example: u1 = 0
0
=0
6. Solution
• Reduced system:
• Solution:
Direct assembling
Example element 4:Between dof 2 and 4
Direct assembling.From the CALFEM-manual
• Transformation of displacement vector
• Transformation of force vector
• where
• which gives
3.2 Truss analysis- transformation to global coordinates (see book for details)
1u
2u
3u
4u
x
1u
2u 3u
4u
x
y
Local system
Global system
eee faK
eeefaK
1u
2u1u2u
ILLT
From the CALFEM-manual
Steps in the FE method