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Great explanation for determining the force in each member of the truss
Typology: Schemes and Mind Maps
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Free-body diagram of entire truss. Calculating the reactions is a good place to start because they are usually easy to compute, and they can be used in the equilibrium equations for the joints where the reactions act.
3 m
5 m
10 kN
Equilibrium equations for entire truss
Fx = 0: Ax + 10 kN = 0 (1)
Fy = 0: Ay + By = 0 (2)
MA = 0: (10 kN)(3 m) + By(5 m) = 0 (3)
Solving these equations simultaneously gives
Ax = 10 kN, Ay = 6 kN, and By = 6 kN
Ax Ay (^) B y
3 m
5 m
10 kN
By = 6 kN
FBC = 6 kN
10 kN
11.66 (T)
7 Free-body diagram of joint B
An "Answer diagram" summarizes the analysis of the entire truss (All forces are in kN).
(^9) Equilibrium equation for joint B 10
Fx^ = 0: FAB = 0
Solving gives
FAB = 0 Ans.
2 kip 4 kip 2 kip
14 ft
10 ft 10 ft 10 ft 10 ft
Free-body diagram of joint E. This joint is chosen because only two unknown forces are present. Thus we know that we can solve for these forces because two equations of equilibrium are available for the joint. Note also that we assume that both unknown forces are in tension (directed away from the joint).
Using = 54.46° in Eqs. 4 and 5 and solving simultaneously gives
FDE = 2.857 kip (T) Ans.
FEH = 4.916 kip = 4.916 kip (C) Ans.
We arbitrarily assumed member EH to be in tension. We then found that the member force was negative, so we know that our assumption was wrong. Member EH is in compression, and we show this by writing a positive "4.916" followed by "(C)".
Equilibrium equations for joint E
Fx = 0: FDE FEH cos = 0 (4)
Fy = 0: FEH sin 4 kip = 0 (5)
= tan-1( ) = 54.46°
Geometry
Ey = 4 kip
14 ft
10 ft
Use a free-body diagram of joint H next because only two member forces are unknown.
FEH = 4.916 kip (C)
FDE = 2.857 kip (T)
Equilibrium equations for joint H
Fx = 0: FGH (4.916 kip) cos 54.46° = 0 (6)
Fy = 0: FDH + (4.916 kip) sin 54.46° = 0 (7)
Solving simultaneously gives
FGH = 2.858 kip = 2.858 kip (C) Ans.
and
FDH = 4.0 kip (T) Ans.
As before, we assume that the unknown member forces (GH and DH in this instance) are tension, so are directed away from the joint. The force in member EH has already been found to be 4.916 kip compression, so it is directed towards the joint, not away from it.
Free-body diagram of joint H
2 kip (^) 4 kip 2 kip
FEH = 4.916 kip (C)
FDE = 2.857 kip (T)
FEH = 4.916 kip (C)
F
2 kip (^) 4 kip 2 kip
FGH = 2.857 kip(C)
FDG= 2.458 kip (C)
FDH = 4.0 kip (T)
FCD = 4.286 kip (T) Use a free-body diagram of joint C because only two member forces are unknown. Free-body diagram of joint C The unknown forces in members CG and BC are assumed to be tension, so are directed away from the joint. The force in member CD has already been found to be 4. kip (T).
Equilibrium equations for joint C.
Fx = 0: FBC + 4.286 kip = 0 (10)
Fy = 0: FCG 4 kip = 0 (11)
Solving gives
FBC = 4.286 kip (T) Ans.
and
FCG = 4 kip (T) Ans. 4 kip
FBC^ FCD = 4.286 kip (T)
All remaining bar forces follow from symmetry.
Answer diagram
All forces in kips.
900 lb
400 lb
10 ft
12 ft
Ex Ey
Because AB is a two-force member, the line of action of FAB must pass through A and B.
Free body-diagram of entire truss
Equilibrium equations for entire truss
Fx = 0: FAB sin 60° + Ex + (900 lb) cos 30° = 0 (1)
Fy = 0: FAB cos 60° + Ey + (900 lb) sin 30° 400 lb = 0 (2)
MC = 0: (400 lb)(10 ft + FAB cos 60°(10 ft) + Ex(12 ft) = 0 (3)
Solving simultaneously gives
FAB = 347.8 lb
Ex = 478.2 lb,
Ey = 123.9 lb
Free-body diagram of joint D. Joint D is chosen because only two member forces are unknown there.
Equilibrium equations for joint D
Fx = 0: FDE = 0 (4)
Fy = 0: FBD 400 lb = 0 (5)
Solving gives
FBD = 400 lb (T) Ans.
FDE = 0 Ans.
Free-body diagram of joint C. Joint C is chosen because only two member forces are unknown there.
Equilibrium equations for joint C
Fx = 0: FBC +779.4 lb = 0 (6)
Fy = 0: FCE + 450 lb = 0 (7)
Solving gives
FBC = 779.4 lb (T) Ans.
FCE = 450.0 lb (T) Ans.
400 lb
(900 lb) sin 30° = 450.0 lb
(900 lb) cos 30°= 779.4 lb
The unknown forces have been assumed to be tension. The unknown forces have been assumed to be tension.
2 kip
2 kip
2 kip
2 kip
2 kip
6 ft 6 ft 6 ft 6 ft 6 ft 6 ft
6 ft 6 ft 6 ft 6 ft 6 ft 6 ft
2 kip
2 kip
2 kip
2 kip
2 kip
Ax Ay (^) D y
Free-body diagram of entire truss
Equilibrium equations for entire truss
Fx = 0: Ax = 0
Fy = 0: Ay + Dy 2 kip 2 kip 2 kip 2 kip 2 kip = 0
MA = 0: 2(kip)(6 ft) 2 kip(12 ft) 2(kip)(18 ft) 2 kip(24 ft) 2(kip)(30 ft) + Dy(36 ft) = 0
Solving simultaneously gives
Ax = 0
Ay = 5 kip
Dy = 5 kip
Three unknown member forces are present at joint I, but two of them, FEI and FIK, are collinear, so summing forces perpendicular to FEI and FIK would give an equation with FFI as the only unknown.
Free-body diagram of joint I
Geometry of members at joint I
Equilibrium equations for joint I
Fy = 0: FFI sin 90° (2 kip) sin 60° = 0
Solving gives
FFI = 1.732 = 1.732 kip (C) Ans.
So member FI is perpendicular to the x axis. Thus the member force FFI lies on the y axis.
2 kip
2 kip
2 kip
2 kip
2 kip
Ax = 0 Ay = 5 kip Dy = 5 kip
2 kip
y
x
x
y
Use the same technique at joint F as was used at joint I: sum forces perpendicular to collinear members BF and FK.
Geometry of members at joint F
Free-body diagram of joint F
Equilibrium equations for joint F
Fy = 0: FEF sin 60° (1.732 kip) sin 60° = 0
Solving simultaneously gives
FEF = 1.732 kip (T) Ans.
2 kip
2 kip
2 kip
2 kip
2 kip
Ax = 0 Ay = 5 kip Dy = 5 kip
FFI = 1.732 kip (C) (already known)
y 60°
x
FFI = 1.732 kip (C)