The stiffness matrix for a Timoshenko beam-column element in its local coordinate system (where x is along the beam length) is: L² A (1+ 4) L²A (1 + 0) 12 6L -12 6L E I 6L L²(4 + $) -6L L?(2 – 4) [K'] = L³ (1 + $) L²A L²A (1+ ø) 7(1+ $) -12 -6L 12 -6L 6L L2 (2 — Ф) -6L L2(4 + ¢)] 12EI GAĻL² a) Derive the transformation matrix [T] for this element, such that the stiffness matrix of the element can be transformed to the global coordinate system using the following relation: [K] = [T.]*[K°][7.]

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
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Q1
The stiffness matrix for a Timoshenko beam-column element in its local coordinate system
(where x is along the beam length) is:
L²A
L²A
ī(1+$)
-7 (1+ 4)
12
6L
-12
6L
E I
6L
L²(4 + ¤)
-6L L(2 – 4)
[K'] =
L²A
(1 + 4)
L³ (1 + Ø)
L²A
(1+ ø)
I
-12
-6L
12
-6L
6L
L²(2 – $)
-6L L2(4+ ¢)]
12EI
GAŞL?
a) Derive the transformation matrix [T] for this element, such that the stiffness matrix of the
element can be transformed to the global coordinate system using the following relation:
[K«] = [T<]*[K¢°][Te]
Transcribed Image Text:Q1 The stiffness matrix for a Timoshenko beam-column element in its local coordinate system (where x is along the beam length) is: L²A L²A ī(1+$) -7 (1+ 4) 12 6L -12 6L E I 6L L²(4 + ¤) -6L L(2 – 4) [K'] = L²A (1 + 4) L³ (1 + Ø) L²A (1+ ø) I -12 -6L 12 -6L 6L L²(2 – $) -6L L2(4+ ¢)] 12EI GAŞL? a) Derive the transformation matrix [T] for this element, such that the stiffness matrix of the element can be transformed to the global coordinate system using the following relation: [K«] = [T<]*[K¢°][Te]
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