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Unit-III 
ELEMENTS OF CIVIL ENGINEERING AND 
ENGINEERING MECHANICS 
by 
Prof. Karisiddappa, MCE, Hassan 
COMPOSITION OF FORCES: The reduction of a given system of forces 
to the simplest system that will be its equivalent is called the problem of 
composition of forces. 
• RESULTANT FORCE: It is possible to find a single force which 
will have the same effect as that of a number of forces acting on a 
body. Such a single force is called resultant force. 
• The process of finding out the resultant force is called composition of 
forces. 
COMPOSITION OF CO-PLANAR CONCURRENT FORCE SYSTEM 
COMPOSITION OF TWO FORCES: It is possible to reduce a given 
system of forces i.e., two forces to the simplest system as its equivalent 
(resultant force) with the help of parallelogram law of forces. 
• LAW OF PARALLELOGRAM OF FORCES: 
If two forces, which act at a point be represented in magnitude and 
direction by the two adjacent sides of a parallelogram drawn from one of its 
angular points, their resultant is represented by the diagonal of the 
parallelogram passing through that angular point, in magnitude and 
direction.
B C 
RR 
a 
R 
q 
O A 
2 cos a 1 2 
R = F 2 
+ F 2 
+ F F 
1 2
B C 
RR 
a 
O A 
α 
PROOF: 
R 
q 
D 
Consider two forces F1 and F2 acting at point O as shown in 
figure. Let α be the angle between the two forces. 
Complete the parallelogram ACBO .Drop perpendicular CD to 
OA produced. Let R be the resultant force of forces and 
.Let q be the inclination of the resultant force with the 
line of action of the force.
From triangle OCD, 
= + 
2 2 2 
OC OD CD 
= + + 
2 2 2 
( ) 
OC OA AD CD 
= = = = 
a a 
, cos , sin , 
OA F AD F CD F OC R 
= + + 
a a 
( cos ) ( sin ) 
R F F F 
= + + + 
a a a 
2 cos cos sin 
R F F F F F 
= + + 
R F F F F 
 
  
 
2 cos 
= + + 
R F F F F 
CD 
OD 
F 
2 
F F 
1 2 
 
  
F 
1 2 
 
sin 
+ 
q 
tan 
= 
+ 
= 
= 
− 
a 
a 
q 
a 
a 
q 
a 
a 
sin 
cos 
tan 
cos 
tan 
2 cos 
1 2 
1 2 
2 
2 
2 
1 
2 
1 2 2 
2 
1 
2 
2 2 
2 
2 2 
1 2 2 
2 
1 
2 
2 
2 
2 
1 2 
2 
1 2 2 
F F
= = + 
R F F 
= = + 
R F F 
= = − 
1 2 
90 , 
0 
1 2 
0 
1 2 
0 
0 , 
180 , 
R F F 
IF a 
a 
a 
IF 
IF 
1 F 
1 F 
1 F 
2 F 
2 F 
2 F 
R 
• TRIANGLE LAW OF FORCES: 
If two forces acting simultaneously on a body are 
represented by the sides of a triangle taken in order, 
their resultant is represented by the closing side of 
the triangle taken in the opposite order. 
O 
1 F 
2 F 
1 F 
2 F 
O A 
B 
R
• POLYGON LAW OF FORCES: 
If a number of concurrent forces acting simultaneously on a body ,are 
represented in magnitude and direction by the sides of a polygon, 
taken in order , then the resultant is represented in magnitude and 
direction by the closing side of the polygon, taken in opposite order. 
O 
1 F 
2 F 
3 F 
4 F 
O 
3 F 
4 F 
1 F 2 F 
R 
D 
A 
B 
C 
1 R 
2 R 
COMPOSITON OF FORCES BY 
RESOLUTION(Principle of resolved parts) 
• The components of each force in the system in two mutually 
perpendicular directions are found. 
• Then, the components in each direction are algebraically 
added to obtain the two components. 
• These two component forces which are mutually 
perpendicular are combined to obtain the resultant force.
1 q 
4 q 
2 q 
3 q 
X 
Y 
1 F 
2 F 
3 F 
4 F 
Algebraic sum of the components of forces in X 
direction 
1 1 2 2 3 3 4 4 F F cosq F cosq F cosq F cosq x  = − − + 
Algebraic sum of the components of forces in Y 
f direction 
1 1 2 2 3 3 4 4 F F sinq F sinq F sinq F sinq y  = + − − 
Now the system of forces is equal to two 
mutually perpendicular forces , 
  X Y F  F 
  
R F F 
X Y 
 
  
 
= + 
 
  
 
= 
 
 
− 
F 
Y 
F 
X 
1 
2 2 
q tan
NUMERICAL PROBLEMS 
1. Determine the magnitude and direction of the resultant of the 
two forces of magnitude 12 N and 9 N acting at a point ,if the 
angle between the two forces is 
GIVEN: 
F 12N 1 = F 9N 2 = 0 a = 30 
= + + 
R F F F F 
= + + × × × 
2 2 0 
12 9 2 12 9 cos30 
20.3 
 
− 
F 
1 2 
 
0 
0 
a 
0 
1 
sin 
1 2 
1 2 
2 
2 
2 
1 
12.81 
9sin 30 
12 9cos30 
tan 
cos 
tan 
2 cos 
= 
= 
 
 
  
 
  
 
+ 
= 
  
 
  
 
+ 
= 
− 
R 
q 
q 
a 
q 
a 
F F 
R N
2.Find the magnitude of two equal forces acting at a point with an 
angle of 600 between them, if the resultant is equal to30 3 N 
GIVEN: 
= + + a 
2 cos 
2 
2 
2 
1 
R F F F F 
1 2 
= + + × × 
2 2 0 
R F F F F 
= + + 
R F F F 
3 
= 
R F 
30 
3.The resultant of two forces when they act at right angles is 10 N 
.Whereas, when they act at a angle of 600 , the resultant is 
N. Determine the magnitude of the two forces. 
Let F1 and F2 be the two forces, 
Given – when α =900 R = 10N 
When α =600 R = N 
We have, 
2 
1 R = F + F + F F 
When α =900 
Squaring both sides 100= F1 
2 + F2 
2 (1) 
When α =600 
0 
148 = F 2 
+ F 2 
+ 2F F cos 60 
1 2 
1 2 
2 
1 F + F + F F × 
2 0.5 1 2 
2 
2 
F F F, say 1 2 = = 
0 R = 30 3N,a = 60 
F N 
2 cos60 
2 2 2 
= 
148 
148 
2 cosa 1 2 
2 
2 
2 
2 
2 
1 10 = F + F
squaring both sides 
148 = F1 
2 + F2 
2 (2) 
substituting (1) in (2) 
148 = 100+F1F2 
F1F2 = 48 (3) 
squaring equation (3),we get 
F1 
2 + F2 
2 = 482 (4) 
From (1) F2 
2 = 100 – F1 
2 (5) 
Subtracting (5) in (4)
( ) 
− = 
2 2 
1 
100 48 
2 
1 
F F 
− = − 
2 2 
1 
100 48 
4 
1 
F F 
( ) 
( ) 
2 2 2 2 
1 
F 
− = − + 
2 2 
1 
F 
2 
1 
F 
2 
1 
F 
50 48 50 
− = 
50 196 
− = 
50 14 
64 
= 
= = 
8  6 
F N F N 
1 2 
4.Find the magnitude and direction of the resultant 
force for the system of concurrent forces shown 
below. 
 
= − − 
F 
X 
20cos30 30cos45 35cos400 0 0 
 
= + + − 
F 
Y 
20sin 30 25 30sin 45 35sin 400 0 0 
=  + 
2 2 
R F FX Y 
R 
30.70 33.72 2 2 
= − + 
45.60 
= 
− 
1 
 
F 
Y 
F 
33.72 
tan 
 
 
 
 
q 
q 
5.The 26 KN force is the resultant of two forces. One of the force is as 
shown in figure .Determine the other force. 
20N 
25N 
30N 
35N 
0 30 
0 45 
0 40 
X 
Y 
 
= − 
F N 
X 
30.70 
 
= 
F N 
Y 
33.72 
( ) ( ) 
R N 
0 
1 
47.68 
30.70 
tan 
= 
 
 
= 
  
 
  
 
= 
− 
 
q 
X 
 X F 
 Y F 
R 
q 
0
y 26kN 
12 
5 10kN 
3 
4 
X 
0 
Let F be magnitude of unscnorm force with Fx and Fy as its 
components in x and y directions. 
Component of R in x directions 13 q1 12 
Rx = 26 x cos q1 
= 26 x 5/13 = 10kN 5 
Component of R in y direction 
Ry = 26 x sin q1 = 26 x 12/13 = 24kN 
Component F and 10kN in X direction 
= Fx +10 cos q2 5 
= Fx + 10x 4/5 = Fx +8 q2 3 
4 
Component of F and 10kN in y direction 
= Fx + 10 x Sin q2 = Fy + 10 x 3/5 
= Fy + 6 
Using R/x = /Fx 
10 = Fx +8 
24 = Fy + 6 
Fx = 2kN, Fy = 18kN 
But F = ÖFx2+Fy2 = Ö22 + 182 
F = 18.11kN 
q2 = tan -1 (Fy /Fx) = tan -1 (18/2) = 83.660 
q2 = 83.660 ( inclination of F w.r.t x – axis)
6.Three forces act at a point in a plate as shown in figure. If the 
resultant of these forces is vertical, find the resultant force and 
angle .. 
100N 
160N 
. 
120 N  
0 
Since the resultant force is vertical, algebraic sum of horizontal components of these must 
be equal to zero. 
160 cos  – 120 – 100 sin  = 0 
120 + 100 sin  = 160 cos  
6 + 5 sin  = 8cos  
Squaring both the sides 
(6+5 sine  )2 = (8 cos  )2 
36 + 60 sin  + 25 sin2 = 64 (1-sin2 ) 
25 sin2  +64 sin2  + 60sin  = 64-36 
89 sin2  + 60 sin  = 28 
Sin2  + 0.674 sin  =0.315 
(sin  + 0.337)2 = 0.315 + 0.3372 
= 0.428 
sin  + 0.337 = Ö0.428 = 0.654 
sin  = 0.654 – 0.337 = 0.317 
 = sin-1 (0.317) = 18.50 
Resultant force R =  Fy 
= 160 sin  + 100 cos  
= 160sin 18.50 + 100 cos 18.50
R = 145.60 N 
7.ABCDE is a regular hexagon. Forces 90 N,P,Q,240 N and 180 N act along 
AB,CA,AD,AE and FA respectively as shown in the figure. Find the forces 
P and Q such that the resultant force is zero. 
C D 
B 
P Q E 
90N 300 300 
240N 
300 
600 300 
A 180N F X 
Since the resultant force is equal to zero,  Fx = 0 and  Fy = 0 
 Fx = -180 +240 cos 300 + Q cos 600 – p cos 900 + 90 cos 1200 = 0 
-180 + 207.85 + 0.5 Q – 45 =0 
0.5Q = 17.15 
Q = 34.308N 
 Fy = 180 sin00+240 sin300 + Q sin600 – P + 90 sin1200 = 0 
120 + 34.308 x sin 600 – P + 90 sin 1200 = 0 
P = 227.654 N
COMPOSITION OF COPLANAR NON-CONCURRENT 
FORCE SYSTEM 
MOMENT OF A FORCE: Moment is 
defined as the product of the magnitude of the force and 
perpendicular distance of the point from the line of 
action of the force. 
GEOMETRICAL REPRESENTATION OF MOMENT 
Consider a force F represented ,in magnitude and direction 
by the line AB. Let O be a point about which the moment 
of the force F is required. Let OC be the perpendicular 
drawn. Join OA and OB 
Moment of force F about O= F x a 
A 
= AB x OC 
F 
c 
B 
O 
a 
= twice the area of triangle OAB 
Thus moment of F about O= 2 x Area of triangle OAB
VARIGNON’S PRINCIPLE OF MOMENTS: 
If a number of coplanar forces are acting simultaneously on a particle, the algebraic sum 
of the moments of all the forces about any point is equal to the moment of their resultant 
force about the same point. 
PROOF: 
For example, consider only two forces F1 and F2 
represented in magnitude and direction by AB and AC as shown in figure below. 
C 
O 
B 
A 
D 
1 F 
2 F 
R 
Let O be the point, about which the moments are taken. Construct the parallelogram 
ABCD and complete the construction as shown in fig. 
By the parallelogram law of forces, the diagonal AD represents, in magnitude and 
direction, the resultant of two forces F1 and F2, let R be the resultant force. 
By geometrical representation of moments 
the moment of force about O=2 Area of triangle AOB 
the moment of force about O=2 Area of triangle AOC 
the moment of force about O=2 Area of triangle AOD 
But, 
Area of triangle AOD=Area of triangle AOC + Area of triangle ACD 
Also, Area of triangle ACD=Area of triangle ADB=Area of triangle AOB 
Area of triangle AOD=Area of triangle AOC + Area of triangle AOB 
Multiplying throughout by 2, we obtain 
2 Area of triangle AOD =2 Area of triangle AOC+2 Area of triangle AOB 
i.e., Moment of force R about O=Moment of force F1 about O + Moment of force F2 
about O 
Similarly, this principle can be extended for any number of forces.
NUMERICAL PROBLEMS 
1.For the non-concurrent coplanar system shown in fig below, 
determine the magnitude , direction and position of the resultant 
force with reference to A. 
R 
25N 
35N 
50N 
20N 
A 
B 
C 
D 
( ) 
 
 
= − = ® 
25 20 5 
F N 
= − − = − 
X 
F N 
Y 
50 35 85 
= 85N(¯) 
R F F ( ) N X Y 5 85 85.15 =  2 + 2 = 2 + − 2 = 
 X F 
 Y F 
R 
× = × + × 
R d 
35 4 25 3 
2.525 
140 75 
d m q 
85.15 
= 
+ 
= 
or 
× = × + × 
85 x 
35 4 25 3 
2.53 
140 75 
x m 
85 
= 
+ 
=
2.Determine the resultant of the force system acting on the plate 
 X F 
 Y F 
R 
q 
as 
shown in figure given below wirh respect to AB and AD. 
10N 5N 
600 D 10Nm 300 
C 
3m 
A 4m B 
14.14N 1 
1 20 N 
 Fx = 5cos300 + 10cos600 + 14.14cos450 
= 19.33N 
 Fy = 5sin300 - 10sin600 + 14.14sin450 
= -16.16N 
R = (  Fx2 +  Fy2) = 25.2N 
= Tan-1( Fx/  Fy) 
= Tan-1(16.16/19.33) = 39.890 
D C 
y 
 
19.33N 
19.33N 
A x  B 
R 16.16N 
Tracing moments of forces about A and applying varignon’s principle of moments we get 
+16.16X = 20x4 + 5cos300x3-5sin300x4 + 10 + 10cos600x3
X = 107.99/16.16 = 6.683m 
Also tan39.89 = y/6.83 
y = 5.586m. 
3.The system of forces acting on a crank is shown in figure 
below. Determine the magnitude , direction and the point 
of application of the resultant force. 
500 N 150 700N 
150 
600 600 
150mm 150 mm 150 Cos600=75mm 
 Fx = 500cos600 – 700 
= 450N 
 Fy = 500sin600 
= -26.33N 
R = (  Fx2 +  Fy2) = (-450)2 + (-2633)2 
R = 267.19N (Magnitude)  Fx 
 
= Tan-1( Fx/  Fy) 
= Tan-1(2633/450) R  Fy 
= 80.300 (Direction) 
Fx 
 x 
R Fy 
Tracing moments of forces about O and applying varignon’s principle of moments 
we get 
-2633x x= -500x sin600x300-1000x150+1200x150cos600 -700x300sin600 
X = -371769.15/-2633 
X = 141.20mm from O towards left (position).
4.For the system of parallel forces shown below, determine the magnitude of the resultant 
and also its position from A . 
100N 200N 50N 400N 
R 
A B C D 
1m 1.5m 1m 
X 
 Fy = +100 -200 -50 +400 
= +250N 
ie. R =  Fy =250N ( ) Since  Fx = 0 
Taking moments of forces about A and applying varignon’s principle of moments 
-250 x = -400 x 3.5 + 50 x 2.5 + 200 x 1 – 100 x 0 
X = -1075/ -250 = 4.3m 
5.The three like parallel forces 100 N,F and 300 N are acting as shown in figure below. If 
the resultant R=600 N and is acting at a distance of 4.5 m from A ,find the magnitude of 
force F and position of F with respect to A. 
100N F 600 N 300N 
A B C D 
4.5m 2.5m 
X 
Let x be the distance from A to the point of application of force F 
Here R =  Fy 
600=100+F+300 
F = 200 N 
Taking moments of forces about A and applying varignon’s principle of moments, 
we get 
600 x 4.5 = 300 x 7 + F x 
200 x = 600 x 4.5 -300 x 7
X = 600/200 = 3m from A 
6.A beam is subjected to forces as shown in the figure given below. Find the magnitude , 
direction and the position of the resultant force. 
17kN 10kN 20kN 10kN 5kN 
 
 4kN 
A B C D E 
2m 3m 2m 1m 
Given tan  = 15/8 sin  = 15/ 17 cos  = 8/17 
tan  = 3/4 sin  = 3/5 cos  = 4/5 
 Fx = 4 +5 cos  – 17 cos  
= 4+5 x 4/5 – 17 x 8/17 
 Fx = 0 
 Fy = 5 sin  -10 +20 – 10 + 17 sin  
= 5 x 3/5 -10+20 – 10 + 17 x 15/17 
 Fy = 18 kN ( ) 
Resultant force R = Ö 2Fx 2 +  Fy2 = Ö 0+182 
R = 18 kN ( ) 
Let x = distance from A to the point of application R 
Taking moments of forces about A and applying Varignon’s theorem of 
moments 
-18 x = -5 x sin  x 8 +10 x 7 -20 x 5 + 10 x 2 
= -3 x 8 +10 x7 – 20 x 5 + 10 x 2 
X = -34/-18 = 1.89m from A (towards left)

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Ks

  • 1. Unit-III ELEMENTS OF CIVIL ENGINEERING AND ENGINEERING MECHANICS by Prof. Karisiddappa, MCE, Hassan COMPOSITION OF FORCES: The reduction of a given system of forces to the simplest system that will be its equivalent is called the problem of composition of forces. • RESULTANT FORCE: It is possible to find a single force which will have the same effect as that of a number of forces acting on a body. Such a single force is called resultant force. • The process of finding out the resultant force is called composition of forces. COMPOSITION OF CO-PLANAR CONCURRENT FORCE SYSTEM COMPOSITION OF TWO FORCES: It is possible to reduce a given system of forces i.e., two forces to the simplest system as its equivalent (resultant force) with the help of parallelogram law of forces. • LAW OF PARALLELOGRAM OF FORCES: If two forces, which act at a point be represented in magnitude and direction by the two adjacent sides of a parallelogram drawn from one of its angular points, their resultant is represented by the diagonal of the parallelogram passing through that angular point, in magnitude and direction.
  • 2. B C RR a R q O A 2 cos a 1 2 R = F 2 + F 2 + F F 1 2
  • 3. B C RR a O A α PROOF: R q D Consider two forces F1 and F2 acting at point O as shown in figure. Let α be the angle between the two forces. Complete the parallelogram ACBO .Drop perpendicular CD to OA produced. Let R be the resultant force of forces and .Let q be the inclination of the resultant force with the line of action of the force.
  • 4. From triangle OCD, = + 2 2 2 OC OD CD = + + 2 2 2 ( ) OC OA AD CD = = = = a a , cos , sin , OA F AD F CD F OC R = + + a a ( cos ) ( sin ) R F F F = + + + a a a 2 cos cos sin R F F F F F = + + R F F F F 2 cos = + + R F F F F CD OD F 2 F F 1 2 F 1 2 sin + q tan = + = = − a a q a a q a a sin cos tan cos tan 2 cos 1 2 1 2 2 2 2 1 2 1 2 2 2 1 2 2 2 2 2 2 1 2 2 2 1 2 2 2 2 1 2 2 1 2 2 F F
  • 5. = = + R F F = = + R F F = = − 1 2 90 , 0 1 2 0 1 2 0 0 , 180 , R F F IF a a a IF IF 1 F 1 F 1 F 2 F 2 F 2 F R • TRIANGLE LAW OF FORCES: If two forces acting simultaneously on a body are represented by the sides of a triangle taken in order, their resultant is represented by the closing side of the triangle taken in the opposite order. O 1 F 2 F 1 F 2 F O A B R
  • 6. • POLYGON LAW OF FORCES: If a number of concurrent forces acting simultaneously on a body ,are represented in magnitude and direction by the sides of a polygon, taken in order , then the resultant is represented in magnitude and direction by the closing side of the polygon, taken in opposite order. O 1 F 2 F 3 F 4 F O 3 F 4 F 1 F 2 F R D A B C 1 R 2 R COMPOSITON OF FORCES BY RESOLUTION(Principle of resolved parts) • The components of each force in the system in two mutually perpendicular directions are found. • Then, the components in each direction are algebraically added to obtain the two components. • These two component forces which are mutually perpendicular are combined to obtain the resultant force.
  • 7. 1 q 4 q 2 q 3 q X Y 1 F 2 F 3 F 4 F Algebraic sum of the components of forces in X direction 1 1 2 2 3 3 4 4 F F cosq F cosq F cosq F cosq x = − − + Algebraic sum of the components of forces in Y f direction 1 1 2 2 3 3 4 4 F F sinq F sinq F sinq F sinq y = + − − Now the system of forces is equal to two mutually perpendicular forces , X Y F F R F F X Y = + = − F Y F X 1 2 2 q tan
  • 8. NUMERICAL PROBLEMS 1. Determine the magnitude and direction of the resultant of the two forces of magnitude 12 N and 9 N acting at a point ,if the angle between the two forces is GIVEN: F 12N 1 = F 9N 2 = 0 a = 30 = + + R F F F F = + + × × × 2 2 0 12 9 2 12 9 cos30 20.3 − F 1 2 0 0 a 0 1 sin 1 2 1 2 2 2 2 1 12.81 9sin 30 12 9cos30 tan cos tan 2 cos = = + = + = − R q q a q a F F R N
  • 9. 2.Find the magnitude of two equal forces acting at a point with an angle of 600 between them, if the resultant is equal to30 3 N GIVEN: = + + a 2 cos 2 2 2 1 R F F F F 1 2 = + + × × 2 2 0 R F F F F = + + R F F F 3 = R F 30 3.The resultant of two forces when they act at right angles is 10 N .Whereas, when they act at a angle of 600 , the resultant is N. Determine the magnitude of the two forces. Let F1 and F2 be the two forces, Given – when α =900 R = 10N When α =600 R = N We have, 2 1 R = F + F + F F When α =900 Squaring both sides 100= F1 2 + F2 2 (1) When α =600 0 148 = F 2 + F 2 + 2F F cos 60 1 2 1 2 2 1 F + F + F F × 2 0.5 1 2 2 2 F F F, say 1 2 = = 0 R = 30 3N,a = 60 F N 2 cos60 2 2 2 = 148 148 2 cosa 1 2 2 2 2 2 2 1 10 = F + F
  • 10. squaring both sides 148 = F1 2 + F2 2 (2) substituting (1) in (2) 148 = 100+F1F2 F1F2 = 48 (3) squaring equation (3),we get F1 2 + F2 2 = 482 (4) From (1) F2 2 = 100 – F1 2 (5) Subtracting (5) in (4)
  • 11. ( ) − = 2 2 1 100 48 2 1 F F − = − 2 2 1 100 48 4 1 F F ( ) ( ) 2 2 2 2 1 F − = − + 2 2 1 F 2 1 F 2 1 F 50 48 50 − = 50 196 − = 50 14 64 = = = 8 6 F N F N 1 2 4.Find the magnitude and direction of the resultant force for the system of concurrent forces shown below. = − − F X 20cos30 30cos45 35cos400 0 0 = + + − F Y 20sin 30 25 30sin 45 35sin 400 0 0 = + 2 2 R F FX Y R 30.70 33.72 2 2 = − + 45.60 = − 1 F Y F 33.72 tan q q 5.The 26 KN force is the resultant of two forces. One of the force is as shown in figure .Determine the other force. 20N 25N 30N 35N 0 30 0 45 0 40 X Y = − F N X 30.70 = F N Y 33.72 ( ) ( ) R N 0 1 47.68 30.70 tan = = = − q X X F Y F R q 0
  • 12. y 26kN 12 5 10kN 3 4 X 0 Let F be magnitude of unscnorm force with Fx and Fy as its components in x and y directions. Component of R in x directions 13 q1 12 Rx = 26 x cos q1 = 26 x 5/13 = 10kN 5 Component of R in y direction Ry = 26 x sin q1 = 26 x 12/13 = 24kN Component F and 10kN in X direction = Fx +10 cos q2 5 = Fx + 10x 4/5 = Fx +8 q2 3 4 Component of F and 10kN in y direction = Fx + 10 x Sin q2 = Fy + 10 x 3/5 = Fy + 6 Using R/x = /Fx 10 = Fx +8 24 = Fy + 6 Fx = 2kN, Fy = 18kN But F = ÖFx2+Fy2 = Ö22 + 182 F = 18.11kN q2 = tan -1 (Fy /Fx) = tan -1 (18/2) = 83.660 q2 = 83.660 ( inclination of F w.r.t x – axis)
  • 13. 6.Three forces act at a point in a plate as shown in figure. If the resultant of these forces is vertical, find the resultant force and angle .. 100N 160N . 120 N 0 Since the resultant force is vertical, algebraic sum of horizontal components of these must be equal to zero. 160 cos – 120 – 100 sin = 0 120 + 100 sin = 160 cos 6 + 5 sin = 8cos Squaring both the sides (6+5 sine )2 = (8 cos )2 36 + 60 sin + 25 sin2 = 64 (1-sin2 ) 25 sin2 +64 sin2 + 60sin = 64-36 89 sin2 + 60 sin = 28 Sin2 + 0.674 sin =0.315 (sin + 0.337)2 = 0.315 + 0.3372 = 0.428 sin + 0.337 = Ö0.428 = 0.654 sin = 0.654 – 0.337 = 0.317 = sin-1 (0.317) = 18.50 Resultant force R = Fy = 160 sin + 100 cos = 160sin 18.50 + 100 cos 18.50
  • 14. R = 145.60 N 7.ABCDE is a regular hexagon. Forces 90 N,P,Q,240 N and 180 N act along AB,CA,AD,AE and FA respectively as shown in the figure. Find the forces P and Q such that the resultant force is zero. C D B P Q E 90N 300 300 240N 300 600 300 A 180N F X Since the resultant force is equal to zero, Fx = 0 and Fy = 0 Fx = -180 +240 cos 300 + Q cos 600 – p cos 900 + 90 cos 1200 = 0 -180 + 207.85 + 0.5 Q – 45 =0 0.5Q = 17.15 Q = 34.308N Fy = 180 sin00+240 sin300 + Q sin600 – P + 90 sin1200 = 0 120 + 34.308 x sin 600 – P + 90 sin 1200 = 0 P = 227.654 N
  • 15. COMPOSITION OF COPLANAR NON-CONCURRENT FORCE SYSTEM MOMENT OF A FORCE: Moment is defined as the product of the magnitude of the force and perpendicular distance of the point from the line of action of the force. GEOMETRICAL REPRESENTATION OF MOMENT Consider a force F represented ,in magnitude and direction by the line AB. Let O be a point about which the moment of the force F is required. Let OC be the perpendicular drawn. Join OA and OB Moment of force F about O= F x a A = AB x OC F c B O a = twice the area of triangle OAB Thus moment of F about O= 2 x Area of triangle OAB
  • 16. VARIGNON’S PRINCIPLE OF MOMENTS: If a number of coplanar forces are acting simultaneously on a particle, the algebraic sum of the moments of all the forces about any point is equal to the moment of their resultant force about the same point. PROOF: For example, consider only two forces F1 and F2 represented in magnitude and direction by AB and AC as shown in figure below. C O B A D 1 F 2 F R Let O be the point, about which the moments are taken. Construct the parallelogram ABCD and complete the construction as shown in fig. By the parallelogram law of forces, the diagonal AD represents, in magnitude and direction, the resultant of two forces F1 and F2, let R be the resultant force. By geometrical representation of moments the moment of force about O=2 Area of triangle AOB the moment of force about O=2 Area of triangle AOC the moment of force about O=2 Area of triangle AOD But, Area of triangle AOD=Area of triangle AOC + Area of triangle ACD Also, Area of triangle ACD=Area of triangle ADB=Area of triangle AOB Area of triangle AOD=Area of triangle AOC + Area of triangle AOB Multiplying throughout by 2, we obtain 2 Area of triangle AOD =2 Area of triangle AOC+2 Area of triangle AOB i.e., Moment of force R about O=Moment of force F1 about O + Moment of force F2 about O Similarly, this principle can be extended for any number of forces.
  • 17. NUMERICAL PROBLEMS 1.For the non-concurrent coplanar system shown in fig below, determine the magnitude , direction and position of the resultant force with reference to A. R 25N 35N 50N 20N A B C D ( ) = − = ® 25 20 5 F N = − − = − X F N Y 50 35 85 = 85N(¯) R F F ( ) N X Y 5 85 85.15 = 2 + 2 = 2 + − 2 = X F Y F R × = × + × R d 35 4 25 3 2.525 140 75 d m q 85.15 = + = or × = × + × 85 x 35 4 25 3 2.53 140 75 x m 85 = + =
  • 18. 2.Determine the resultant of the force system acting on the plate X F Y F R q as shown in figure given below wirh respect to AB and AD. 10N 5N 600 D 10Nm 300 C 3m A 4m B 14.14N 1 1 20 N Fx = 5cos300 + 10cos600 + 14.14cos450 = 19.33N Fy = 5sin300 - 10sin600 + 14.14sin450 = -16.16N R = ( Fx2 + Fy2) = 25.2N = Tan-1( Fx/ Fy) = Tan-1(16.16/19.33) = 39.890 D C y 19.33N 19.33N A x B R 16.16N Tracing moments of forces about A and applying varignon’s principle of moments we get +16.16X = 20x4 + 5cos300x3-5sin300x4 + 10 + 10cos600x3
  • 19. X = 107.99/16.16 = 6.683m Also tan39.89 = y/6.83 y = 5.586m. 3.The system of forces acting on a crank is shown in figure below. Determine the magnitude , direction and the point of application of the resultant force. 500 N 150 700N 150 600 600 150mm 150 mm 150 Cos600=75mm Fx = 500cos600 – 700 = 450N Fy = 500sin600 = -26.33N R = ( Fx2 + Fy2) = (-450)2 + (-2633)2 R = 267.19N (Magnitude) Fx = Tan-1( Fx/ Fy) = Tan-1(2633/450) R Fy = 80.300 (Direction) Fx x R Fy Tracing moments of forces about O and applying varignon’s principle of moments we get -2633x x= -500x sin600x300-1000x150+1200x150cos600 -700x300sin600 X = -371769.15/-2633 X = 141.20mm from O towards left (position).
  • 20. 4.For the system of parallel forces shown below, determine the magnitude of the resultant and also its position from A . 100N 200N 50N 400N R A B C D 1m 1.5m 1m X Fy = +100 -200 -50 +400 = +250N ie. R = Fy =250N ( ) Since Fx = 0 Taking moments of forces about A and applying varignon’s principle of moments -250 x = -400 x 3.5 + 50 x 2.5 + 200 x 1 – 100 x 0 X = -1075/ -250 = 4.3m 5.The three like parallel forces 100 N,F and 300 N are acting as shown in figure below. If the resultant R=600 N and is acting at a distance of 4.5 m from A ,find the magnitude of force F and position of F with respect to A. 100N F 600 N 300N A B C D 4.5m 2.5m X Let x be the distance from A to the point of application of force F Here R = Fy 600=100+F+300 F = 200 N Taking moments of forces about A and applying varignon’s principle of moments, we get 600 x 4.5 = 300 x 7 + F x 200 x = 600 x 4.5 -300 x 7
  • 21. X = 600/200 = 3m from A 6.A beam is subjected to forces as shown in the figure given below. Find the magnitude , direction and the position of the resultant force. 17kN 10kN 20kN 10kN 5kN 4kN A B C D E 2m 3m 2m 1m Given tan = 15/8 sin = 15/ 17 cos = 8/17 tan = 3/4 sin = 3/5 cos = 4/5 Fx = 4 +5 cos – 17 cos = 4+5 x 4/5 – 17 x 8/17 Fx = 0 Fy = 5 sin -10 +20 – 10 + 17 sin = 5 x 3/5 -10+20 – 10 + 17 x 15/17 Fy = 18 kN ( ) Resultant force R = Ö 2Fx 2 + Fy2 = Ö 0+182 R = 18 kN ( ) Let x = distance from A to the point of application R Taking moments of forces about A and applying Varignon’s theorem of moments -18 x = -5 x sin x 8 +10 x 7 -20 x 5 + 10 x 2 = -3 x 8 +10 x7 – 20 x 5 + 10 x 2 X = -34/-18 = 1.89m from A (towards left)