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Page 1: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

ENGINEERING MECHANICS

CHAPTER 2

FORCES & RESULTANTS

By Jeff Lamoon

www.jefflamoon.comSlide 1 of 35

Page 2: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE21052005

2.1 Introduction

This chapter introduces the concept of vectors. Upon completion of this chapter, the student will be able

1 Distinguish between vector and scalar quantities.

2 Determine the resultants of two force vectors by using vector triangle, parallelogram law and vector polygon addition.

3 Resolving a force vector into its components. Determine the resultant of several force vectors using the method of perpendicular components.

4

Slide 2 of 35

Page 3: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

2.2 Vector Quantities

• Scalar quantity has only magnitude.

Examples: 10 kg mass, 8 m long, 20 m2 area, etc.

• Vector quantity has magnitude + direction.

E.g. 1) 5 km south.

E.g. 2) 8 kN horizontal force.

E.g. 3) 9 m/s north.

5 cm

9 cm

8 cm

Application

Application

Slide 3 of 35

Page 4: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

• • Scalar quantities can be added algebraically:

600 1500

4

3

3 cm + 5 cm = 8 cm

6 kg + 8 kg = 14 kg

However, vector quantities cannot be added

or subtracted because vector has the extra

property of direction.

• Vectors may be in any direction:

Slide 4 of 35

Page 5: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

2.3 Vector Triangle Method y 8 kN 6 kN 60 40 x

0

0

a) Graphical Method (Tip To Tail)

i) Choose a scale like 1 cm to 1 kN, then begin by drawing any force vector.

x

400 6 cm

Slide 5 of 35

Page 6: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

ii) Draw the other force taking care to join them tip-to-tail.

x

400

6 cm

600

8 cm

y 8 kN 6 kN 60 40 x

0

0

Tip of first arrow join to tail of nextarrow.

Slide 6 of 35

Page 7: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

x

400

6 cm

600

8 cm

R

Start point

End point

iii) Complete the triangle by drawing the resultant R from the start point of first arrow to end point of last arrow (force vector).

y 8 kN 6 kN 60 40 x

0

0

Application

Slide 7 of 35

Page 8: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

x

1500 8 cm

Lets draw the diagram another way : start withthe 8 kN force instead

The same resultant R is obtained and it makes no difference which force you start to draw first, as long as you follow ‘Tip to Tail, join start point to end point’ rule.

y 8 kN 6 kN 60 40 x

•0

•0

Step 1 Step 3Step 2

x

400 6 cm

8 cm 1500

x

400 6 cm

8 cm

R

Slide 8 of 35

Page 9: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

b) Analytical method

Start by sketching the triangle ABC.

x

400 6 cm

600 8 cm

R

C

A

B

Angle ABC = (300 + 400) = 700

As triangle is not a right-angle,

Cosine Law is used here.

03323232 )cos70)(6x102(8x10)(6x10)(8x10R

R = 8.20 kN

Slide 9 of 35

Page 10: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

To find direction of R, use sine rule to find ,then .

0

33

70sin

10x2.8

sin

10x8

8.2 kN

73.50

917.02.8

52.7sin

05.66

0

000

5.73

405.66180..

ei

x

400 6 kN

600 8 kN

C

B

8.2 kN

Slide 10 of 35

Page 11: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

2.4 Parallelogram Method

a) Graphical Method

i) Use scale of 1 cm to 1 kN, draw the forces from the same point as in the diagram.

y 8 kN 6 kN 60 40 x

•0

•0

Application

Slide 11 of 35

Page 12: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

ii) Construct a parallelogram by drawing parallel lines as shown.

400

6 kN

600 8 kN

x

y 8 kN 6 kN 60 40 x

0

0

Slide 12 of 35

Page 13: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

iii) Draw the diagonal R from the point where the tails of the two arrows meet.

400

6 kN

8 kN

x

R

y 8 kN 6 kN 60 40 x

•0

•0

Note that half of the parallelogram is exactly the same triangle as that obtained bythe Vector Triangle Method in 2.3.

Slide 13 of 35

Page 14: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

b) Analytical Method

We can select any half of the parallelogram to solve for the resultant. The right half here is exactly the same as the one in 2.3 b) above and the analytical method use is also exactly the same.

R

400 x

8 kN

6 kN Slide 14 of 35

Page 15: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

2.5 Vector Polygon Method

4 kN

3 kN

6 kN

200

400

8 kN

This method is used to find the resultant ofthree or more forces. Example below illustrates this principles

Slide 15 of 35

Page 16: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

a) Graphical Method 4 kN 3 kN

6 kN 200

400

8 kN

Start with any force drawn to scale, and follow tip-to-tail rule , draw the other 3 forces.

8 kN 40 0

end point R 4 kN

start point

3 kN 20 0

6 kN

Slide 16 of 35

Page 17: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

1

b) Analytical Method

For 3 or more forces, this method involves more calculation steps. The polygon is divided into several triangles and cosine and sine rules are then applied. Using the example above:

8 kN

R

4 kN

3 kN

6 kN

R2

R1

40 0

20 0

The polygon is divided into three triangles 1, 2 and 3 as shown. Starting with triangle 1, using cosine and sine rules, calculate R1. Then the process is repeated for triangle 2 to find R2, and finally triangle 3 to find R, the resultant of the four forces. This is very tedious and not the preferred method.

* Check sections 2.6 and 2.7 for an easier method

3

2

Slide 17 of 35

Page 18: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

2.6 Resolution of A Force Into Components

Conversely, a single force F (like a resultant), can be replaced by 2 forces or components of F, which produce the same effect on the body.

We know that resultant is the sum of 2 or more forces and it produces the same effect on a body.

Hence a system of forces can be replaced by a single resultant force which have the same effect on the body.

Slide 18 of 35

Page 19: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

The method of resolving a single force vector into two components is the reverse of vector addition.

Any single force can be resolved into 2 components in any direction, but in order for us to develop an easier analytical method, we would choose to resolve a single force into its perpendicular components based on the x- and y-axis.

Slide 19 of 35

Page 20: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

One of the most important and useful concept is the resolution of a force vector into two perpendicular components, in the x and y axis as denoted by the Fx (x)

and Fy (y) components.

2.7 Resolution of A Force Into Perpendicular Components

y

FFy

Fx x

Fy = F sin

Fx = F cos

Slide 20 of 35

Page 21: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Sketch the parallelogram with Fy perpendicular to Fx.

Example 2.1Resolve the 300 N force into components along the x and y axes.

300 N

300

Fx

Fy

x

y

300

300 N

Slide 21 of 35

Page 22: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Select any half of the triangle, a vector triangle, for analysis.

As this is a right-angle triangle, cos 300 = Fx / 300 i.e Fx = 300 x cos 300

= 259.81 N

Also since sin 300 = Fy / 300 i.e Fy = 300 sin 300 = 150 N

Fx

Fy

x

300

Application

Slide 22 of 35

Page 23: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

For a number of forces, this section introduces an easieranalytical method of finding the resultant.Students should master this method as it would form the basis of all your calculations for resultant forces.

2.8 Resolution of A Force By Fx And Fy Components

Let us use the same simple example in section 2.3 above to demonstrate the method:

y 8 kN 6 kN 60 40 x

0

0

Slide 23 of 35

Page 24: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

1. We first resolved the 2 forces into perpendicular i.e. Fx and Fy components.

2. The 2 forces can now be replaced by the above 4 components as shown below.

30 0

8 kN

Fx = ( 8 x 103 cos 30o)

Fy = ( 8 x 103 sin 30o)

40 0

6 kN

Fy = ( 6 x103 sin 40o)

Fx = ( 6 x 103 cos 40o)

Fx = ( 6.93 kN)

Fy = ( 4.0 kN)

Fy = ( 3.86 kN)

Fx = ( 4.6 kN)A

Slide 24 of 35

Page 25: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

3. Now we can add the two Fx forces to form a single Rx, as they are both horizontal forces but only opposite in direction, if we adopt a sign convention. Similarly, we can also add the two Fy forces to form a single Ry.

Fx = Rx, is the sum of all the Fx forces, Fy = Ry , is the sum of all Fy forces.

Fx = ( 6.93 kN)

Fy = ( 4.0 kN)

Fy = ( 3.86 kN)

Fx = ( 4.6 kN)A

Fx = (4.6x103) - (6.93x103) {Fx pointing left is –ve} Rx = - 2.33 kN

Fy = (3.86x103) + (4.0x103) {Fy pointing up is +ve} Ry = + 7.86 kN

Slide 25 of 35

Page 26: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

4. These two forces, Rx and Ry can now replace the previous four component forces in (2) above, and we can use the vector triangle method to add them back to form a single force, which is the resultant R, as shown by the vector triangle below.

From the right-angle triangle, we then use the Pythagoras Theorem to find the magnitude of R.

Rx = 2.33 kN

Ry = 7.86 kN R

The magnitude of R is: R = Rx

2 + Ry2

= (2.33x103)2 + (7.86x103)2 = 8.2 kN

The angle of R is: = tan -1 (Ry/Rx) = tan -1 ((7.86x103)/(2.33x103)) = 73.5 0

Same answers as before.

Slide 26 of 35

Page 27: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Resultant By Method of Perpendicular Components:

-ve

Fy

Fy

+ ve

Fx

+ ve

Fx

- ve

Use the Sign convention forthe force components:

1. Resolve all (but not horizontal or vertical) forces into Fx and Fy components.2. Use Fx = Rx,

Fy = Ry

3. Magnitude: R = Rx2 + Ry

2 Angle: = tan -1 (Ry/Rx) (from x axis)

Ry

Rx Rx

R

Ry

Rx Rx Ry

R R

RRy

4. Direction of R:

Slide 27 of 35

Page 28: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Example 2.2 Four forces act on a bolt as shown. Determine the resultant force.

ySolution:

Fx components in the x direction

F1x = +150 cos 30 0 = 129.9 N

80 N 200 150 N 30 0 x 15 0

100 N 110 N

F2x = +100 cos 15 0 = 96.6 N

F3x = - 80 cos 70 0 = - 27.4 N

F4x = 0 N, (for 110 N force)

i.e. Fx = Rx = 150 cos 30 0 + 100 cos 15 0 - 80 cos 70 0

= 129.9 + 96.6 – 27.4 + 0 Rx = 199.1N

Application

Slide 28 of 35

Page 29: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Fy components in the y direction

F1y = +150 sin 30 0 = 75 N

y 80 N 200 150 N 30 0 x 15 0

100 N 110 N

F2y = - 100 sin 15 0 = - 25.9 N F3y = + 80 sin 70 0 = 75.2 N

F4y = - 110 N (it is a Fy or vertical force)

i.e. Fy = Ry = 150 sin 30 0 - 100 sin 15 0 + 80 sin 70 0

= 75 – 25.9 +75.2 - 110 Ry = 14.3 N

Slide 29 of 35

Page 30: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

The magnitude of R is

y 80 N 200 150 N 30 0 x 15 0

100 N 110 N

R = ( Rx2 + Ry

2)

R = ( 199.12 + 14.32) = 199.6 N

The angle , R makes with the horizontal is

= tan-1 Ry / Rx

= tan-1 14.3 / 199.1 = 4.10

Since Rx and Ry are positive values,

R = 199.6 N and = 4.10 Rx

Rx

R

Slide 30 of 35

Page 31: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Example 2.3The rocket’s main engine exerts a total thrust of 900,000 N parallel to the y axis. Each of its two small side engines exerts a thrust of 22,250 N in the direction as shown.Determine the magnitude and direction of the resultant force exerted on the rocket by the engines.

22250 N

16 031 0

y

22250 N

900,000 N

Slide 31 of 35

Page 32: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

tan = Ry / Rx = 940460 / 5326.67 = 176.55 = 89.68 0

R

Solution:

Fx = Rx = 22,250 sin 16 – 22,250 sin 31 = - 5326.67 N Fy = Ry = -22,250 cos 16 – 22,250 cos 31 – 900,000 = - 21388 – 19072 – 900,000 = - 940460 N

  R = (Rx2 + Ry2) = (5326.672 + 9404602) = 940475 N

Slide 32 of 35

Page 33: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

Example 2.4 A bracket is being pulled by 3 forces as shown. Determine the angle and the magnitude of force P if the resultant’s direction is along the y-axis and its magnitude is 20 kN.

y 10 kN

P kN 600

8 kN x

Application

Special situations:

1. Resultant’s direction is along the x-axis (Horizontal)

Fy = Ry = 0 Fx = Rx = R2. Resultant’s direction is along the y-axis (Vertical)

Fx = Rx = 0 Fy = Ry = R

Slide 33 of 35

Page 34: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

i.e Fx = Rx = 0 (No Rx component)

Since the resultant’s direction is along the y-axis.

and Fy = Ry = 20x103 N ( R must be = Ry)

Fx = Rx = 0

(10x103)(cos 60o) + (8x103) – (Px103)(cos ) = 0 (1)

and Fy = Ry = 20x103 N (10x103)(sin 60o) + (Px103)(sin ) = 20 (2)

y 10 kN

P kN 600

8 kN x

Slide 34 of 35

Page 35: Engineering Mechanics – Chapter 2: Forces & ResultantsEE05042007 ENGINEERING MECHANICS CHAPTER 2 FORCES & RESULTANTS By Jeff Lamoon

Engineering Mechanics – Chapter 2: Forces & Resultants EE05042007

y 10 kN

P kN 600

8 kN x

i.e. tan = 11.34 / 13 = 0.8723

= tan -1 (0.8723)

To find magnitude of P, substitute = 41.1 0 into equations (1) or (2).

P cos = 13 P = 13 / cos = 17.25 (P kN = 17.25 kN)

= 41.1 0

End of Chapter 2

From equation (1), P cos = 13 (3)

From equation (2), P sin = 11.34 (4)

Equation (4)/(3), P sin / P cos = (11.34 / 13)

Slide 35 of 35