tarek hegazy, univ. of waterloo 2 t / m 2 t 1m 2m xa ya yb xb yc step 1: stability check no. of...
DESCRIPTION
Tarek Hegazy, Univ. of Waterloo M + at (e), right side only = 0 2 t 2m Yb Xb e Xb. 0 = 0 +Xb. 0 = 0 +Yb. 4 +Yb. 4 Solve, Yb = +1 i.e., correct direction Solve, Yb = +1 i.e., correct direction Sign Force DistanceTRANSCRIPT
Tarek Hegazy, Univ. of Waterloo [email protected]
2 t / m
2 t
1m
2m 2m 2m 2m
Xa
Ya
Yb
Xb
Yc
Step 1: Stability Check
No. of Equilibrium Equations: 3No. of Extra Conditions: 2 (two intermediate pins)
Since the unknowns 5 = Equations (3 + 2) Then, Structure is Stable & Statically Determinate
Assumed reactions
No. of Unknown Reactions? 5
Draw the B.M.D. & the S.F.D.
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2mYc
2 t / m
2 t
1mXa
Ya
Step 2: Reactions Sign Convention
=0
=0
=0 M
+
X+
Y+
Any point
For the whole structure considering all forces including reactions
2m 2mYb
Xbe
d
Start writing an equation with least number of unknowns:
M+
Since (e) is an intermediate pin, then
at (e) right side only = 0
Tarek Hegazy, Univ. of Waterloo [email protected]
M+
at (e), right side only = 0
2 t
2m 2m
Yb
Xb
e
-2 . 2 +Xb . 0 = 0+Yb . 4
Solve, Yb = +1 i.e., correct directionSign Force Distance
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2mYc
2 t / m
2 t
1mXa
Ya2m 2m
1
Xb
M+
Since (d) is an intermediate pin, then
at (d) right side only = 0
Let’s write another equation:
d
Tarek Hegazy, Univ. of Waterloo [email protected]
M+
at (d), right side only = 0
2 t
2m 2m 1
Xb
d
-2 . 2 +Xb . 1 = 0+1 . 4
Solve, Xb = 0
1m
Sign Force Distance
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2mYc
2 t / m
2 t
1mXa
Ya2m 2m
1
Now, = 0 , +Xa - 0 = 0, or Xa = 0 X+
0
M+
Since (d) is an intermediate pin, then
at (d) left side only = 0
0
Let’s now write two equations to get the last two unknowns:
d
Tarek Hegazy, Univ. of Waterloo [email protected]
- Ya.4
2m 2mYc
2 t / m
Ya
d
M+
at (d), left side only = 0
Equivalent = 2 x 4 = 8
- Yc.2 + 8 .2 = 0
Or, 4 Ya + 2 Yc = 16 . . . . . (1)Sign Force Distance
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2mYc
2 t / m
2 t
1m
Ya2m 2m
1
Now, then, Y=0+
Solve (1) & (2), Ya = -1 , Yc = 10 Opposite direction Same direction
+Ya +Yc +1 -2x4 -2 = 0
4 Ya + 2 Yc = 16 . . . (1)
Ya + Yc = 9 . . . (2)
All Up All Down
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
Let’s first define the beam sections with changes in load or beam’s Shape.
We are now ready to draw the B.M.D. and the S.F.D.
1 2
3 45
67 8
910
Now, we analyze each section separately, considering only one side of the structure.
Final Reactions:
Shear is Paralle to the section & Perpendicular to the beam
Axial (i.e., Normal) force is parallel to the beam
Section2
Section3
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
B.M.D.
Section Analysis:Analyze the right side or the left side, whichever has less calculation.
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
B.M.D.
Section 1Left
Section 1 B.M. = -1 . 0 = 0
0
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
3 45
67 8
910
B.M.D.
1 2
Section 2 B.M. = -1 . 2 - 4 . 1 = - 6
0
-6
Section 2Left
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
3 45
67 8
910
B.M.D.
1 2
10
0
-6
Section 3 B.M. = - 1 . 2 - 4 . 1 +10 . 0 = -6
Section 3Left
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
3 45
67 8
910
B.M.D.
1 2
10
Section 4 B.M. = -1 . 4 -4 . 3 -4 . 1 +10 . 2 = 0
Section 4Left
0
-6
0
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
3 45
67 8
910
B.M.D.
1 2
10
0
-6
0
Section 5Left
Section 5 B.M. = 0 (same as section 4)
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
B.M.D.
Section 10Right
Section 10 B.M. = +1 . 0 = 0
0
-6
0
0
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
B.M.D.
Section 9Right
Section 9 B.M. = +1 . 2 = +2
0
-6
0
0
+2
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
B.M.D.
Section 8Right
0
-6
0
0
+2
Section 8 B.M. = +1 . 2 = +2
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
B.M.D.
Sections 7 & 6Right
Sections 7 & 6 B.M. = 0
0
-6
0
0
+20
SS
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m
11 10
4 4
B.M.D.
0
-6
0
0
+2
0
-3-3
w.L2/8 = 1w.L2/8 = 1
Now, we connect the moment values
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
S.F.D.
Section 1Left
Section 1 S.F. = -1 +Shear is a
force perpendicular to the beam
-1
S
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
3 45
67 8
910
1 2
Section 2 S.F. = -1 - 4 = - 5
Section 2Left
S.F.D.
-5
-1
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
3 1 2
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
45
67 8
910
10
Section 3 S.F. = - 1 - 4 +10 = +5
Section 3Left
S.F.D.
-5
-1
+5
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
3 4567 8
910
1 2
10
Section 4 S.F. = - 1 - 4 +10 - 4 = +1
Section 4Left
S.F.D.
-5
-1
+5+1
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
10
Section 5Left
Section 5 S.F. = 0
S.F.D.
3 4567 8
910
1 2
-5
-1
+5+1
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11
4 4
10
Section 6Left
Section 6 S.F. = 0
S.F.D.
3 4567 8
910
1 2
-5
-1
+5+1
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
1 23 4
56
7 89
10
Section 10Right
Section 10 S.F. = -1
S.F.D.
-5
-1
+5+1
-1
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
Section 9Right
Section 9 S.F. = -1
S.F.D.
1 23 4
567 8 9 10
-5
-1
+5+1
-1-1
S
+
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
Section 8Right
S.F.D.
1 23 4
567 8 9 10
-5
-1
+5+1
-1-1
+1
S
+Section 8 S.F. = -1 +2 = +1
Tarek Hegazy, Univ. of Waterloo [email protected]
2m 2m
2 t/m
2 t
1m
2m 2m 11 10
4 4
Sections 7Right
Sections 7 S.F. = -1 +2 = +1
S.F.D.
1 23 4
567 8 9 10
-5
-1
+5+1
-1-1
+1+1
+
S
Tarek Hegazy, Univ. of Waterloo [email protected]
S.F.D.
2m 2m
2 t/m
2 t
1m
2m 2m
11 10
4 4
-5
+5+1
-1-1
+1+1
-1
Now, we connect the shear values
Tarek Hegazy, Univ. of Waterloo [email protected]
S.F.D.
2m 2m
2 t/m
2 t
1m
2m 2m
11 10
4 4
0
-6
0
0
+2
0
-3-3
w.L2/8 = 1w.L2/8 = 1
-5
+5+1
-1-1
+1+1
-1
B.M.D
Final Answer