a1 = 3610 x 722 = 2,606,420 mm2; a2 = 5776 x 722 = 4,170,272 mm2; a3 = 2527 x 361 = 912,247 mm2
a1 + a2 + a3 = 2606420 + 4170272 + 912247 = 7,688,939 mm2
x1 = ; x2 = ; x3 =
y1 = ; y2 = ; y3 =
a1x1 |
4,704,588,100 mm3 |
a1y1 |
16,936,517,160 mm3 |
a2x2 |
1,505,468,192 mm3 |
a2y2 |
13,549,213,728 mm3 |
a3x3 |
1,152,624,084.5 mm3 |
a3y3 |
164,660,583.5 mm3 |
Total |
7362680376.5 mm3 |
30650391471.5 mm3 |
Thus and
The and are from the bottom left hand corner of the area/drawing.
First, the beam is separated into two sections at point P (where the internal hinge is located). The two beam sections are then solved separately (independently). It is also important to note that an internal pin (hinge) provides vertical reaction.
8 x UC = 8 x 361 = 2888 KN/m
15 x UC = 15 x 361 = 5415 KN
First section of the beam (the beam on the right hand side):
Summation of moments at P, ;
-5VC + 3(5415 sin 45) = 0; 5VC = 3(5415 sin 45); VC = 2297.39 KN
Summation of moments at C, ;
5VP – 2(5415 sin 45) = 0; 5VP = 2(5415 sin 45); VP = 1531.59 KN
Second section of the beam (the beam on the left hand side):
Summation of moments at P, ;
6VA – (2888 x 4 x 4) + (2VB) = 0
6VA – 46208 + 2VB = 0; 6VA + 2VB = 46208
Summation of moments at A, ;
(2888 x 4 x 2) – 4VB + 6VP = 0
23104 – 4VB + 6(1531.59) = 0; 23104 – 4VB + 9189.54 = 0
4VB = 32293.54; VB = 8073.385 KN
Summation of forces in y-direction (vertical forces), ;
VA – (2888 x 4) + VB – VP = 0; VA – 11552 + 8073.385 – 1531.59 = 0
VA – 5010.205; VA = 5010.205 KN
The summary of reactions at A, B and C are provided in the table below
Reaction |
Value |
A |
5010.205 KN |
B |
8073.385 KN |
C |
2297.39 KN |
Calculation of reactions at the supports of frame
Summation of forces in x-direction: ;
HA + 361 KN = 0; HA = -361 KN
HA = 361 KN ← (acting towards the left hand side)
Summation of forces in y-direction: ;
VA – 1083 – 722 + VB = 0; VA + VB = 1805 KN
Summation of moments at A: ;
(1083 x 1.5) + (722 x 4.5) + (361 x 3) – (6VB) = 0
1624.5 + 3249 + 1083 – 6VB = 0; 6VB = 5956.5; VB = 992.75 KN ↑ (acting upwards).
But VA + VB = 1085 KN; VA = 1085 – VB; VA = 1085 – 992.75 = 812.25 KN ↑ (acting upwards)
The summary of reaction forces is provided in the table below
Reaction |
Value |
HA |
361 KN ← |
VA |
812.25 KN ↑ |
VB |
992.75 KN ↑ |
This methods involves calculating member forces at each joint separately (SkyCiv Engineering, 2015). This is because it is assumed that the joints connect members in a way that rotation is allowed hence the members can only carry either compression or tension axial force (Krenk & Hogsberg, 2013).
Joint A:
Summation of forces in y-direction: ;
VA + AC sin 63.43 = 0; 812.25 + AC sin 63.43
AC sin 63.43 = -812.25; ; AC = 908.16 KN (compression)
Summation of forces in x-direction: ;
-HA + AF + AC cos 63.43 = 0
-361 KN + AF + (-908.16) cos 63.43 = 0; AF = 361 + 406.21 = 767.21 KN (tension)
Joint C:
Summation of forces in y-direction: ;
-1083 – AC sin 63.43 – CF sin 63.43 = 0
-1083 – (-908.16 sin 63.43) – CF sin 63.43 = 0
-1083 + 812.25 – CF sin 63.43 = 0; CF sin 63.43 = -270.75;
; CF = 302.72 KN (compression)
Summation of forces in x-direction: ;
CD + CF cos 63.43 – AC cos 63.43 = 0
CD + (-302.72) cos 63.43 – (-908.16) cos 63.43 = 0
CD – 135.40 + 406.21 = 0; CD = 135.40 – 406.21 = -270.81 KN; CD = 270.81 KN (compression)
Joint F:
Summation of forces in y-direction: ;
CF sin 63.43 + FD sin 63.43 = 0
CF sin 63.43 = -FD sin 63.43
CF = – FD; FD = -CF = – (-302.72)
FD = 302.72 KN (tension)
Summation of forces in x-direction: ;
FB + FD cos 63.43 – CF cos 63.43 – AF = 0
FB + 302.72 cos 63.43 – (-302.72) cos 63.43 – 767.21 = 0
FB + 135.40 + 135.40 – 767.21 = 0
FB = 767.21 – 135.40 – 135.40 = 496.41 KN (tension)
The summary of member forces is provided in the table below
Member |
Force |
Sense |
AC |
908.16 KN |
Compression |
AF |
767.21 KN |
Tension |
CD |
270.81 |
Compression |
CF |
302.72 KN |
Compression |
FD |
302.72 KN |
Tension |
FB |
496.41 KN |
Tension |
Forces in members using method of sections
It starts with cutting the truss or frame into 2 separate sections, ensuring that the cut runs through all the members that are being targeted. This is followed by drawing free body diagram for one of the sections and using equations of equilibrium to determine member forces (Moore, (n.d.)).
The section chosen cuts through members DE, DB and FB
It is assumed that the right hand of the section is in equilibrium
Summation of moments at B to the right hand side, ;
(3 x 361) – (3 x DE) = 0; 1083 – 3DE = 0; DE = 361 KN (tension)
Summation of moments at D to the right hand side, ;
(3 x FB) – (1.5 x VB) = 0; 3FB – (1.5 x 992.75) = 0
3FB = 1489.125; FB = 496.375 KN (tension)
Summation of moments at E to the left hand side, : ;
(1.5 x VB) + (3 x FB) + (3 x DB cos 63.43) + (1.5 x DB sin 63.43) = 0
(1.5 x 992.75) + (3 x 496.375) + 1.34187DB + 1.34158DB = 0
1489.125 + 1489.125 + 2.68345DB = 0
2.68345DB = -2978.25; DB = -1109.8586 KN; DB = 1110 KN (compression)
The summary of member forces is provided in the table below
Member |
Force |
Sense |
DE |
361 KN |
Tension |
DB |
1110 KN |
Compression |
FB |
496.4 KN |
Tension |
Calculating second moment of area
The sketch of cross is as follows:
a1 = 200 x 15 = 3,000 mm2; a2 = 356 x 171 = 60,876 mm2; a3 = 200 x 15 = 3,000 mm2
a1 + a2 + a3 = 3,000 + 60,876 + 3,000 = 66,876 mm2
x1 = ; x2 = ; x3 =
a1x1 |
300,000 mm3 |
a2x2 |
6,087,600 mm3 |
a3x3 |
300,000 mm3 |
Total |
6,687,600 mm3 |
Thus
h1 = 100 – 7.5 = 92.5 mm
h2 = 193 – 100 = 93 mm
h3 = 378.5 mm
Ixx =
Ixx =
Ixx = 56250 + 25668750 + 642931728 + 526516524 + 56250 + 429786750
1,625,016,252 mm4
Calculating maximum UDL
Area = a1 + a2 + a3 = 3,000 + 60,876 + 3,000 = 66,876 mm2
Force = Stress x Area = 165 N/mm2 x 66876 mm2 = 11,034.54 KN
UDL span = 6 m = 6,000 mm
Why 200 x 15 mm plates are not required over the whole span
This is because the web of the I section beam is much wider and longer hence the load can be supported directly on the top center of the beam. As a result, the plates are not needed through the span of the beam.
First, the beam is separated into two sections at point P (where the internal hinge is located). The two beam sections are then solved separately (independently). It is also important to note that an internal pin (hinge) provides vertical reaction.
First section of the beam (the one on the right hand side):
Summation of moments at P, ;
-6VC + 4 (60 sin 45) = 0; 6VC = 4(60 sin 45); VC = 28.28 KN
Summation of moments at C, ;
-6VP – 2(60 sin 45) = 0; -6VP = 2(60 sin 45); VP = -14.14 KN; VP = 14.14 KN ↑
Second section of the beam (the beam on the left hand side):
Summation of moments at P, ;
8VA – (4.5 x 75) + (2VB) = 0
8VA – 337.5 + 2VB = 0; 8VA + 2VB = 337.5
Summation of moments at A, ;
(3.5 x 75) – (6 x VB) + 8VP = 0
262.5 – 6VB + 8(14.14) = 0; 262.5 – 6VB + 113.12 = 0
6VB = 375.62; VB = 62.60 KN
Summation of forces in y-direction (vertical forces), ;
VA – 75 + VB – VP = 0; VA – 75 + 62.60 – 14.14 = 0
VA – 26.53; VA = 26.53 KN
The summary of reactions at A, B and C are provided in the table below
Reaction |
Value |
A |
26.53 KN |
B |
62.60 KN |
C |
28.28 KN |
Point of contraflexure is a point on the bending moment (BMD) of a beam where the BMD intersects with or cuts the x-axis i.e. where the BMD changes sign from +ve to –ve or from –ve to +ve (Sharma, (n.d.)). Therefore point of contraflexure is determined from BMD. This involves calculating bending moments along the beam and identifying the point where the bending moment changes sign.
VA = 51 KN; VB = 78 KNm
MA = 0 KNm
M1 = (51 x 1) – (15 x 1 x 0.5) = 51 – 7.5 = 43.5 KNm
M2 = (51 x 2) – (15 x 2 x 1) = 102 – 30 = 72 KNm
M3 = (51 x 3) – (15 x 3 x 1.5) = 153 – 67.5 = 85.5 KNm
M4 = (51 x 4) – (15 x 4 x 2) = 204 – 120 = 84 KNm
M5 = (51 x 5) – (15 x 5 x 2.5) – (25 x 1) = 255 – 187.5 – 25 = 42.5 KNm
M6(B) = (51 x 6) – (15 x 6 x 3) – (25 x 2) = 306 – 270 – 50 = -14 KNm
M7 = 7 x 1 x 0.5 = 3.5 KNm
M8 = 0 KNm
The sketch of BDM of the beam is as follows
From the above calculations, the sign of bending moments changes between the point when the point load is acting and the support at B. Assuming that the point where the bending moment changes sign (point of contraflexure) is P, which is at a distance x from support B, then the value of x can be determined as follows:
Summation of moments at point M to the right hand side:
(15 * x * 0.5x) – (VB * x) + (7 * 2 * (x + 1)) = 0
7.5x2 – 78x + 14(x + 1) = 0
7.5x2 – 78x + 14x + 14 = 0
7.5x2 – 64x + 14 = 0
x = 8.31 m or x = 0.225 m
Since x cannot be greater than 2m, it means that x = 0.225 m
Therefore the point of contraflexure from the left hand support A is: 4m + (2m – 0.225m)
= 4m + 1.775m = 5.775 m
Summation of forces in x-direction: ;
HA + 20 KN = 0; HA = -20 KN
HA = 20 KN ← (acting towards the left hand side)
Summation of forces in y-direction: ;
VA – 30 – 40 + VB = 0; VA + VB = 70 KN
Summation of moments at A: ;
(20 x 3) + (30 x 4.5) + (40 x 7.5) – (6VB) = 0
60 + 135 + 300 – 6VB = 0; 6VB = 495; VB = 82.5 KN ↑ (acting upwards).
But VA + VB = 70 KN; VA = 70 – VB; VA = 70 – 82.5 = -12.5 KN
VA = 12.5 KN ↓ (acting downwards)
The summary of reaction forces is provided in the table below
Reaction |
Value |
HA |
20 KN ← |
VA |
12.5 KN ↓ |
VB |
82.5 KN ↑ |
Calculation of member forces by method of joints
Joint A:
Summation of forces in y-direction: ;
VA + AC sin 63.43 = 0; 75 + AC sin 63.43
AC sin 63.43 = -75; ; AC = 83.86 KN (compression)
Summation of forces in x-direction: ;
HA + AF + AC cos 63.43 = 0
0 + AF + (-83.86) cos 63.43 = 0; AF = 37.51 KN (tension)
Joint C:
Summation of forces in y-direction: ;
-75 – AC sin 63.43 – CF sin 63.43 = 0
-75 – (-83.86 sin 63.43) – CF sin 63.43 = 0
-75 + 75 – CF sin 63.43 = 0; CF sin 63.43 = 0;
; CF = 0 KN
Summation of forces in x-direction: ;
CD + CF cos 63.43 – AC cos 63.43 = 0
CD + (0) cos 63.43 – (-83.86) cos 63.43 = 0
CD – 0 + 37.51 = 0; CD = -37.51 KN; CD = 37.51 KN (compression)
Joint F:
Summation of forces in y-direction: ;
CF sin 63.43 + FD sin 63.43 = 0
CF sin 63.43 = -FD sin 63.43
CF = – FD; FD = -CF = – (0)
FD = 0 KN
Summation of forces in x-direction: ;
FB + FD cos 63.43 – CF cos 63.43 – AF = 0
FB + 0(cos 63.43) – 0 (cos 63.43) – 37.51 = 0
FB + 0 – 0 – 37.51 = 0
FB = 37.51 KN (tension)
The summary of member forces in two decimal places is provided in the table below
Member |
Force |
Sense |
AC |
83.9 KN |
Compression |
AF |
37.5 KN |
Tension |
CD |
37.5 KN |
Compression |
CF |
0 KN |
– |
FD |
0 KN |
– |
FB |
37.5 KN |
Tension |
Forces in members using method of sections
The section chosen cuts through members CD, FD and FB
It is assumed that the right hand of the section is in equilibrium
Summation of moments at F to the right hand side, ;
Assuming that force CD is in tension
(1.5 x 75) – (3 x VB) – (3 x CD) = 0; 112.5 – 3(75) – 3CD = 0; 112.5 – 225 – 3CD = 0
-112.5 = 3CD; CD = -37.5 KN
Since CD was assumed to be in tension but the value obtained is -37.5 KN, it means that it is a compression force.
Therefore CD = 37.5 KN (compression)
Summation of moments at D to the right hand side;;
Assuming that force FB is in tension
-(1.5 x VB) + (3 x FB) = 0; -(1.5 x 75) + 3FB = 0; -112.5 + 3FB = 0;
3FB = 112.5; FB = 37.5 KN (tension)
Summation of moments at B to the left hand side, ;
-(1.5 x 75) – (3 x CD) – (3 x FD cos 63.43) – (1.5 x FD sin 63.43) = 0;
-112.5 – 3CD – 1.3419FD – 1.3419FD = 0
-112.5 – (3 x -37.5) – 2.6838FD = 0
-112.5 + 112.5 – 2.6838FD = 0
2.6838FD = 0; FD = 0 KN
The summary of member forces is provided in the table below
Member |
Force |
Sense |
CD |
37.5 KN |
Compression |
FD |
0 KN |
– |
FB |
37.5 KN |
Tension |
The values of CD, FD and FB above are the same as those obtained in section 6(b) using method of joints.
Question 7: Shear force diagram (SFD) and bending moment diagram (BMD)
Summation of moments at A, ;
(10 x 4 x 2) + (25 x 7) – (9VB) + (15 x 3.5 x 10.75) = 0
80 + 175 – 9VB + 564.375 = 0
819.375 = 9VB; VB = 91 KN ↑
Summation of forces in y-direction (vertical forces), ;
VA – (10 x 4) – 25 + VB – (15 x 3.5) = 0
VA – 40 – 25 + 91 – 52.5 = 0
VA = 26.5 KN
The SFD is as shown below
The BMD is as shown below
MA = 0 KNm
M1 = (26.5 x 1) – (10 x 1 x 0.5) = 26.5 – 5 = 21.5 KNm
M2 = (26.5 x 2) – (10 x 2 x 1) = 53 – 20 = 33 KNm
M3 = (26.5 x 3) – (10 x 3 x 1.5) = 79.5 – 45 = 34.5 KNm
M4 = (26.5 x 4) – (10 x 4 x 2) = 106 – 80 = 26 KNm
M5 = (26.5 x 5) – (10 x 4 x 3) = 132.5 – 120 = 12.5 KNm
M6 = (26.5 x 6) – (10 x 4 x 4) = 159 – 160 = -1 KNm
M7 = (26.5 x 7) – (10 x 4 x 5) = 185.5 – 200 = -14.5 KNm
M8 = (26.5 x 8) – (10 x 4 x 6) – (25 x 1) = 212 – 240 – 25 = -53 KNm
MB = 15 x 3.5 x 1.75 = -91.875 KNm
M10 = 15 x 2.5 x 1.25 = -46.875 KNm
M11 = 15 x 1.5 x 0.75 = -16.875 KNm
References
Krenk, S. & Hogsberg, J., 2013. Truss Structures. In: Statics and Mechanics of Structures. Dordrecht: Springer, pp. 39-89.
Moore, J., (n.d.). The Method of Sections. [Online]
Available at: https://adaptivemap.ma.psu.edu/websites/structures/method_of_sections/methodofsections.html
[Accessed 28 July 2018].
Sharma, S., (n.d.). Procedure for drawing shear force and bending moment diagram:. [Online]
Available at: https://nptel.ac.in/courses/112107146/lects%20&%20picts/image/lect23%20and%2024/lecture%2023%20and%2024.htm
[Accessed 28 July 2018].
SkyCiv Engineering, 2015. Tutoral for truss method of joints. [Online]
Available at: https://skyciv.com/tutorials/tutorial-for-truss-method-of-joints/
[Accessed 28 July 2018].
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