Frame and distributed load 1 Consider the frame shown below
Solution
Can try Finite element approach
We have a system with 3 nodes ( 1,2, 3) with zero moment at 2 ( pin joint) and displacement only in y direction
Nodeal coordinate matrix nodel 1 1,0
node 2 0, L
node 3 L,L ( origin at lower left corner)
Direction cosines (l,m) for element 1 [ -.707/L , -.707/L]
DC for element 2 [ 1/L, 0 ]
Write stiffness matrices for elements 1 and 2, in terms of l,m
obtain 4X4 matrices for each element. (use bending matrix)
Assemble the Global Stiffness Matrix for the assemblage ( 6x6)
Now Global displacement vector { q1, Q2, q3, Q4, q5,Q6} where q1=0 (fixed for point 1), Q2` =1
q3 (for node 2) ( moves only in vertical and q4=0, no moment)
q5=q6 =0 ( cantilever end)
Applied Force vector is ( f1,f2,f3,f4,f5,f6) where we have zeros except for f3,f4,f5,f6
obtain these from the reactions`at the ends of element 1 and the b.m. at ends of element,=> f4=0
Set up the matrix eqn with given displacements and force moment vector. Using elimination method reduce to 2X2 matrix eqn, involving q2 and q3. (q2 is the displacment and q3 the slope at the moving end).
For a 2X2 matrix can use the invers ematrix identity shown.
