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FINITE ELEMENT ANALYSIS
OF TRUSS
BY-
Ms. JAPE ANUJA S.
ASSISTANT PROFESSOR,
CIVIL ENGINEERING DEPARTMENT,
SRES, SANJIVANI COLLEGE OF ENGINEERING,
KOPARGAON-423603.
MAID ID: anujajape@gmail.com
japeanujacivil@sanjivani.org.in
FINITE ELEMENT ANALYSIS OF TRUSS
• Truss may be determinate or indeterminate truss
• Joint displacements are Unknown variables.
• Formulation of stiffness matrix of truss:
• The nodal displacement vector for the bar element is
• The stiffness matrix of a bar element is
1 2
AE, L
 
'
' 1
'
2
e
u
x
u
 
  
 
'
' 1
'
2
1 1
1 1
uAE
K
L u
 
       
' '
1 2u u
Transformation matrix for the truss:
• x' y'= Local coordinate systems
• x, y = global coordinate system
u1' , u2' = Displacements in local
coordinate system
• u1, u2, u3, u4= Displacements in
global coordinate system
• Ɵ=Angle measured in
anticlockwise sense w.r.t. positive
x-axis
Since axial directions of all members of truss are not same, hence in global coordinate
system (x-y) there are two displacement components at every node. Hence the nodal
displacement vector for typical truss element is
 
1
1
2
2
e
u
v
x
u
v
 
 
 
  
 
  
At Node1 At Node 2
Therefore, in matrix form above relation are
Where =vector of local unknowns
=vector of global unknowns
=Transformation matrix
where
'
1 1 1cos sinu u v   '
2 2 2cos sinu u v  
    
1
'
11
'
22
2
'
cos sin 0 0
0 0 cos sin
ee
u
vu
uu
v
x L x
 
 
 
      
    
    
  

 '
e
x
 e
x
 L
 
0 0
0 0
l m
L
l m
 
  
 
2 1
2 1
cos
sin
x x
l
L
y y
m
L



 

 
Stiffness matrix of truss element in global coordinate system:
     
 
 
'
0
0 1 1 0 0
0 1 1 0 0
0
0
0
0
0
T
K L K L
l
m l mAE
K
l l mL
m
l
m l m l mAE
K
l l m l mL
m
   
 
               
 
 
 
           
 
 
 
2 2
2 2
2 2
2 2
l lm l lm
lm m lm mAE
K
L l lm l lm
lm m lm m
  
 
  
  
 
  
THANK YOU

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Truss Analysis using Finite Element method ppt

  • 1. FINITE ELEMENT ANALYSIS OF TRUSS BY- Ms. JAPE ANUJA S. ASSISTANT PROFESSOR, CIVIL ENGINEERING DEPARTMENT, SRES, SANJIVANI COLLEGE OF ENGINEERING, KOPARGAON-423603. MAID ID: anujajape@gmail.com japeanujacivil@sanjivani.org.in
  • 2. FINITE ELEMENT ANALYSIS OF TRUSS • Truss may be determinate or indeterminate truss • Joint displacements are Unknown variables. • Formulation of stiffness matrix of truss: • The nodal displacement vector for the bar element is • The stiffness matrix of a bar element is 1 2 AE, L   ' ' 1 ' 2 e u x u        ' ' 1 ' 2 1 1 1 1 uAE K L u           ' ' 1 2u u
  • 3. Transformation matrix for the truss: • x' y'= Local coordinate systems • x, y = global coordinate system u1' , u2' = Displacements in local coordinate system • u1, u2, u3, u4= Displacements in global coordinate system • Ɵ=Angle measured in anticlockwise sense w.r.t. positive x-axis Since axial directions of all members of truss are not same, hence in global coordinate system (x-y) there are two displacement components at every node. Hence the nodal displacement vector for typical truss element is   1 1 2 2 e u v x u v              
  • 4. At Node1 At Node 2 Therefore, in matrix form above relation are Where =vector of local unknowns =vector of global unknowns =Transformation matrix where ' 1 1 1cos sinu u v   ' 2 2 2cos sinu u v        1 ' 11 ' 22 2 ' cos sin 0 0 0 0 cos sin ee u vu uu v x L x                             ' e x  e x  L   0 0 0 0 l m L l m        2 1 2 1 cos sin x x l L y y m L        
  • 5. Stiffness matrix of truss element in global coordinate system:           ' 0 0 1 1 0 0 0 1 1 0 0 0 0 0 0 0 T K L K L l m l mAE K l l mL m l m l m l mAE K l l m l mL m                                               2 2 2 2 2 2 2 2 l lm l lm lm m lm mAE K L l lm l lm lm m lm m                
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