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Lec#19; Force Method recorded

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Analysis of Indeterminate
Structures
Force Method
Lecture 19
Force Method
Indeterminate Structure
• Stresses in indeterminate are generally lower than determinate structure.
• Deflection in case of indeterminate structure is less than those compared to
determinate due to greater stiffness.
Indeterminate Structure
• Statically indeterminate structure have capacity to redistribute the loads.
If a part (or member or support) of such a structure fails, the entire
structure will not necessarily collapse, and the loads will be redistributed
to the adjacent portions of the structure.
https://www.quora.com/What-are-the-advantages-ofindeterminate-structure-over-determinate-structure
Methods in the Analysis of Statically Indeterminate
Structures
• Force Method
➢ Virtual Work Method
➢ Castigliano’s Theorem
➢ Three Moment Theorem
• Displacement Method
➢ Slope Deflection Method
➢ Moment Distribution Method
➢ Stiffness Matrix Method
➢ Kani’s Method
Force Method
BASIS
• Originally Developed by
James Clerk Maxwell in
1864
• Later refined by Otto
Mohr and Heinrich
Muller-Breslau
• Flexibility Method
• Compatibility Method
• Method of consistent
displacement
Force Method
• Primary unknown are forces
• It is used to calculate reactions and internal forces in
statically indeterminate structure due to loads and
imposed deformation.
• Based on transforming a given structure into a statically
determinate primary system and calculating the
magnitude of the statically redundant forces required to
restore the geometric boundaru condition of original
structure.
General Procedure
Redundant
𝐴𝑐𝑡𝑢𝑎𝑙 𝐵𝑒𝑎𝑚
Redundant
𝑅𝐴
Step 1: determine which redundant to be removed, you may choose to removed the
roller support or change the fixed support to hinge or pin support.
𝑅𝐵
General Procedure
Step 2. Using superposition, calculate the force that would be required to achived
compatibility with the original structure
+
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝑆𝑡𝑟𝑢𝑐𝑡𝑢𝑟𝑒
𝐶𝑜𝑚𝑝𝑎𝑡𝑖𝑏𝑖𝑙𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛𝑠:
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐵𝑦 𝑎𝑝𝑝𝑙𝑖𝑒𝑑
𝒇𝑩𝑩
∆𝐵 + ∆′𝐵𝐵 = 0
∆𝐵 + 𝐵𝑦 𝑓𝐵𝐵 = 0
𝒏𝒐𝒕𝒆: 𝒇𝑩𝑩 − 𝒍𝒊𝒏𝒆𝒂𝒓 𝒇𝒍𝒆𝒙𝒊𝒃𝒊𝒍𝒊𝒕𝒚 𝒄𝒐𝒆𝒇𝒇𝒊𝒄𝒊𝒆𝒏𝒕
Measure of the deflection per unit force, m/N, ft/lb
General Procedure
𝑀𝐴
+
𝜃′𝐴𝐴 = 𝑀𝐴 𝛼𝐴𝐴
𝐶𝑜𝑚𝑝𝑎𝑡𝑖𝑏𝑖𝑙𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛𝑠:
𝜃𝐴 + 𝑀𝐴 𝛼𝐴𝐴 = 0
𝛼𝐴𝐴
𝑀𝐴 = −𝜃𝐴 /𝛼𝐴𝐴
𝑛𝑜𝑡𝑒: 𝑠𝑖𝑔𝑛 𝑖𝑛𝑑𝑖𝑐𝑎𝑡𝑒 𝑡ℎ𝑎𝑡𝑀𝐴 𝑎𝑐𝑡𝑠 𝑜𝑝𝑝𝑜𝑠𝑖𝑡𝑒 𝑡ℎ𝑒 𝑑𝑖𝑟𝑒𝑐𝑡𝑖𝑜𝑛 𝑡𝑜 𝑡ℎ𝑒 𝑢𝑛𝑖𝑡 𝑐𝑜𝑢𝑝𝑙𝑒 𝑚𝑜𝑚𝑒𝑛𝑡
General Procedure
=
+
+
=
+
+
𝐶𝑜𝑚𝑝𝑎𝑡𝑖𝑏𝑖𝑙𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛𝑠:
∆𝐵 + 𝐵𝑦 𝑓𝐵𝐵 + 𝐵𝑦 𝑓𝐶𝐵 = 0
∆𝐶 + 𝐶𝑦 𝑓𝐵𝐶 + 𝐶𝑦 𝑓𝐶𝐶 = 0
Deflections and Slopes of Beams (Cantilever Beam)
Deflections and Slopes of Beams
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Cantilever Beam)
Deflections and Slopes of Beams (Cantilever Beam)
Deflections and Slopes of Beams (Cantilever Beam)
Deflections and Slopes of Beams (Cantilever Beam)
Deflections and Slopes of Beams (Cantilever Beam)
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Simple Beam)
Deflections and Slopes of Beams (Simple Beam)
Problem #1
Determine the reactions and
draw the shear and moment
diagram of the given beam
Compatibility Equations
∆𝐴 + 𝐴𝑦 𝑓𝐴𝐴 = 0
∆𝐴
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝐵𝑒𝑎𝑚
𝐴𝑦𝑓𝐴𝐴
Ay = 1
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐴𝑦
Primary Beam
𝑃𝑎2
𝑀𝑜 𝐿2
∆𝐴 = −
3𝐿 − 𝑎 +
6𝐸𝐼
2𝐸𝐼
𝑃𝑎2
∆=
(3𝐿 − 𝑎)
6𝐸𝐼
120 62
∆𝐴 = −
6𝐸𝐼
∆𝐴 = −
𝑀0𝐿2
∆=
2𝐸𝐼
75 122
3 12 − 6 +
2𝐸𝐼
16200
𝑘𝑁𝑚3
𝐸𝐼
Redundant
Ay
𝑓𝐴𝐴 =
(1)123
3𝐸𝐼
1
Compatibility Equations
∆𝐴
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝐵𝑒𝑎𝑚
∆𝐴 = −
∆𝐴 + 𝐴𝑦 𝑓𝐴𝐴 = 0
16200
𝑘𝑁𝑚3
𝐸𝐼
𝐴𝑦𝑓𝐴𝐴
Ay = 1
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐴𝑦
𝐴𝑦 = 28.125 𝑘𝑁 ↑
Ex.1:Determine the reactions and draw the shear
and moment diagram of the given beam
𝑀𝐶 = 307.5 𝑘𝑁𝑚
𝐵𝑦 = 91.875 𝑘𝑁
𝐴𝑦 = 28.125 𝑘𝑁
28.125 𝑘𝑁
75 𝑘𝑁𝑚
243.75 𝑘𝑁𝑚
−91.875 𝑘𝑁
−307.5 𝑘𝑁𝑚
Problem#2
Determine the reactions and draw the shear and moment
diagram of the given beam
∆𝐶
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝐵𝑒𝑎𝑚
𝐶𝑦𝑓𝐶𝐶
Compatibility Equations
∆𝐶 + 𝐶𝑦 𝑓𝑐𝑐 = 0
𝐶𝑦 = 1
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐶𝑦
Primary
𝐴𝑦 = 356.25 𝑘𝑁
𝐷𝑦 = 318.75 𝑘𝑁
𝐴𝑦 = 0.5 𝑘𝑁
𝐷𝑦 = 0.5 𝑘𝑁
Redundant
𝑹𝒆𝒂𝒍
𝑽𝒊𝒓𝒕𝒖𝒂𝒍
𝐶
𝐴𝑦 = 0.5 𝑘𝑁
𝐶
𝐷𝑦 = 0.5 𝑘𝑁
𝐴𝑦 = 0.5 𝑘𝑁
𝐷𝑦 = 0.5 𝑘𝑁
Primary
Segment
origin
Limit
M
m
AB
A
0-5
356.25𝑥
0.5𝑥
BC
A
5-10
356.25𝑥 − 375 𝑥 − 5
0.5𝑥
DC
D
0-10
318.75𝑥 − 15𝑥 2
0.5𝑥
1 𝐿
න 𝑀𝑚 𝑑𝑥
𝐸𝐼 0
1 5
2473.96
න 356.25𝑥 0.5𝑥 𝑑𝑥 =
3𝐸𝐼 0
𝐸𝐼
10
1
න 356.25𝑥 − 375 𝑥 − 5 0.5𝑥 𝑑𝑥
3𝐸𝐼 5
10807.29
=
𝐸𝐼
10
1
34375
න 318.75𝑥 − 15𝑥 2 0.5𝑥 𝑑𝑥 =
𝐸𝐼 0
𝐸𝐼
47656.25
∆𝐶 =
𝑘𝑁𝑚3 ↓
𝐸𝐼
Redundant
Segment
origin
Limit
M
m
1 𝐿
න 𝑀𝑚 𝑑𝑥
𝐸𝐼 0
AC
A
0-10
−0.5𝑥
−0.5𝑥
1 10
න −0.5𝑥 −0.5𝑥 𝑑𝑥 = 27.78
3𝐸𝐼 0
DC
D
0-10
−0.5𝑥
−0.5𝑥
1 10
න −0.5𝑥 −0.5𝑥 𝑑𝑥 = 83.33
𝐸𝐼 0
𝑓𝐶𝐶
111.11
=
𝑘𝑁𝑚3 ↑
𝐸𝐼
𝐶𝑜𝑚𝑝𝑎𝑡𝑖𝑏𝑖𝑙𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛
∆𝐶
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝐵𝑒𝑎𝑚
𝐶𝑦 𝑓𝐶𝐶
𝐶𝑦 = 1
∆𝐶 =
47656.25
𝑘𝑁𝑚3 ↓
𝐸𝐼
𝑓𝐶𝐶 =
∆𝐶 + 𝐶𝑦 𝑓𝑐𝑐 = 0
111.11
𝑘𝑁𝑚3 ↑
𝐸𝐼
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐶𝑦
𝐶𝑦 = 428.911 𝑘𝑁
428.91 𝑘𝑁
141.795 𝑘𝑁
104.295 𝑘𝑁
195.705 𝑘𝑁
141.795 𝑘𝑁
10 − 𝑥 = 3.476𝑚
x = 6.524m
−104.295 𝑘𝑁
−233.205 𝑘𝑁
708.975 kNm
181.34 𝑘𝑁𝑚
−457.05 𝑘𝑁𝑚
Ex.3:Determine the reactions and draw the shear
and moment diagram of the given Frame
𝐷𝑦𝑓𝐷𝐷
∆𝐷
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝐹𝑟𝑎𝑚𝑒
𝐶𝑜𝑚𝑝𝑎𝑡𝑖𝑏𝑖𝑙𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛
∆𝐷 + 𝐷𝑦 𝑓𝐷𝐷 = 0
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐷𝑦
Primary frame
𝐷
200𝑘𝑁
200 kN
1750 + 10P
segme origin
nt
limit
DC
D
0-5
CB
D
5-10
AB
A
0-10
M
𝑴
𝑷
M (P=0)
𝟏 𝑳 𝑴
න 𝑴
𝒅𝒙
𝑬𝑰 𝒐
𝑷
Primary frame
𝐷
200𝑘𝑁
200 kN
1750 + 10P
segme origin
nt
limit
M
𝑴
𝑷
M (P=0)
𝟏 𝑳 𝑴
න 𝑴
𝒅𝒙
𝑬𝑰 𝒐
𝑷
DC
D
0-5
−𝑃𝑥
−𝑥
0
0
CB
D
5-10
−𝑃𝑥 − 150(𝑥 −5)
−𝑥
−150(𝑥 −5)
15625/𝐸𝐼
AB
A
0-10
− 1750 + 10𝑃
− 10𝑥 2 + 200𝑥
−10
−1750 − 10𝑥 2
+ 200𝑥
108333.333/𝐸𝐼
∆𝑫 = 𝟏𝟐𝟑𝟗𝟓𝟖. 𝟑𝟑𝟑/𝑬𝑰
𝐷
Redundant
10𝑚
10𝑚
10P
seg orig lim
me in
it
nt
DB
D
0-5
AB
A
0-10
M
M (P=1)
𝐷
Redundant
10𝑚
10𝑚
10P
segme origin
nt
limit
M
𝑴
𝑷
M (P=1)
𝟏 𝑳 𝑴
න 𝑴
𝒅𝒙
𝑬𝑰 𝒐
𝑷
DB
D
0-10
𝑃𝑥
𝑥
𝑥
333.333/𝐸𝐼
AB
A
0-10
10𝑃
10
10
1000/𝐸𝐼
𝒇𝑫𝑫 = 𝟏𝟑𝟑𝟑. 𝟑𝟑𝟑/𝑬𝑰
𝐷𝑦𝑓𝐷𝐷
∆𝐷
𝑃𝑟𝑖𝑚𝑎𝑟𝑦 𝐹𝑟𝑎𝑚𝑒
∆𝑫 = 𝟏𝟐𝟑𝟗𝟓𝟖. 𝟑𝟑𝟑/𝑬𝑰
𝐶𝑜𝑚𝑝𝑎𝑡𝑖𝑏𝑖𝑙𝑖𝑡𝑦 𝑒𝑞𝑢𝑎𝑡𝑖𝑜𝑛
∆𝐷 + 𝐷𝑦 𝑓𝐷𝐷 = 0
𝑅𝑒𝑑𝑢𝑛𝑑𝑎𝑛𝑡 𝐷𝑦
𝒇𝑫𝑫 = 𝟏𝟑𝟑𝟑. 𝟑𝟑𝟑/𝑬𝑰
𝟏𝟐𝟑𝟗𝟓𝟖. 𝟑𝟑𝟑
𝐷𝑦 =
1333.333
𝑫𝒚 = 𝟗𝟐. 𝟗𝟔𝟗 𝒌𝑵
𝑫𝒚 = 𝟗𝟐. 𝟗𝟕 𝒌𝑵
𝑨𝒙 = 𝟐𝟎𝟎 𝒌𝑵
𝑴𝑨 = 𝟖𝟐𝟎. 𝟑 𝒌𝑵𝒎 𝑨𝒚 = 𝟓𝟕. 𝟎𝟑 𝒌𝑵
𝑴𝑩 = 𝟏𝟕𝟗. 𝟕𝒌𝑵𝒎
𝑩𝒚 = 𝟓𝟕. 𝟎𝟑 𝒌𝑵
179.7 𝑘𝑁𝑚
𝑩𝒙 =0
𝑨𝒙 = 𝟐𝟎𝟎 𝒌𝑵
𝑴𝑨 = 𝟖𝟐𝟎. 𝟑 𝒌𝑵𝒎 𝑨𝒚 = 𝟓𝟕. 𝟎𝟑 𝒌𝑵
200 𝑘𝑁
−820.3 𝑘𝑁
𝑴𝑩 = 𝟏𝟕𝟗. 𝟕𝒌𝑵𝒎
𝑩𝒙 =0
𝑩𝒚 = 𝟓𝟕. 𝟎𝟑 𝒌𝑵
𝑫𝒚 = 𝟗𝟐. 𝟗𝟕 𝒌𝑵
𝟓𝟕. 𝟎𝟑 𝒌𝑵
𝟒𝟔𝟒. 𝟖𝟓𝒌𝑵𝒎
𝟏𝟕𝟗. 𝟕𝒌𝑵𝒎
−𝟗𝟐. 𝟗𝟕 𝒌𝑵
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