1 of 26

SEMESTER:- 2ND SEMESTER

SUBJECT:-ENGINEERING MECHANICS

CHAPTER : 1

TOPIC : FUNDAMENTALS OF ENGINEERING MECHANICS

PREPARED BY :-

ER.B.N.MOHANTA

ER. B.C.PANDEY

1

2 of 26

ER. B.N.MOHANTA

2

3 of 26

ER. B.N.MOHANTA

3

4 of 26

ER. B.N.MOHANTA

4

5 of 26

ER. B.N.MOHANTA

5

6 of 26

ER. B.N.MOHANTA

6

7 of 26

ER. B.N.MOHANTA

7

8 of 26

ER. B.N.MOHANTA

8

9 of 26

ER. B.N.MOHANTA

9

10 of 26

ER. B.N.MOHANTA

10

11 of 26

ER. B.N.MOHANTA

11

12 of 26

ER. B.N.MOHANTA

12

EFFECTS OF A FORCE

*It may change the motion of a body. i.e. if a body is at rest, the force may set it in motion. And if the body is already in motion, the force may accelerate it.

*It may retard the motion of a body.

* It may retard the forces, already acting on a body, thus bringing it to rest or in equilibrium

13 of 26

CHARACTERISTICS OF A FORCE

  • 1. Magnitude of the force (i.e., 10 N, 20 kN, 5 kN, etc.)

  • 2. The direction of the line, along which the force acts (i.e., along OX, OY, at 60° North of East etc.). It is also known as line of action of the force.

  • 3. Nature of the force (i.e., whether the force is push or pull). This is denoted by placing an arrow head on the line of action of the force.

  • 4. The point at which (or through which) the force acts on the body

ER. B.N.MOHANTA

13

14 of 26

PRINCIPLE OF TRANSMISSIBILITY OF FORCES

It states, “If a force acts at any point on a rigid body, it may also be considered to act at any other point on its line of action, provided this point is rigidly connected with the body.”

ER. B.N.MOHANTA

14

15 of 26

RESULTANT FORCE

  • If a number of forces are acting simultaneously on a particle, then it is possible to find out a single force which could replace them i.e., which would produce the same effect as produced by all the given forces. This single force is called resultant force and the given forces R ... etc. are called component forces.

ER. B.N.MOHANTA

15

16 of 26

PARALLELOGRAM LAW OF FORCES

It states, “If two forces, acting simultaneously on a particle, be

represented in magnitude and direction by the two adjacent sides of

a parallelogram ; their resultant may be represented in magnitude

and direction by the diagonal of the parallelogram, which passes through their point of intersection.”

ER. B.N.MOHANTA

16

17 of 26

ER. B.N.MOHANTA

17

18 of 26

RESOLUTION OF A FORCE

  • The process of splitting up the given force into a number of components, without changing its effect on the body is called resolution of a force.
  • A force is, generally, resolved along two mutually perpendicular directions.

ER. B.N.MOHANTA

18

19 of 26

PRINCIPLE OF RESOLUTION

  • It states, “The algebraic sum of the resolved parts of a no. of forces, in a given direction, is equal to the resolved part of their resultant in the same direction.”
  • In general, the forces are resolved in the vertical and horizontal directions.

ER. B.N.MOHANTA

19

20 of 26

POLYGON LAW OF FORCES

  • It states, “If a number of forces acting simultaneously on a particle, be represented in magnitude and direction, by the sides of a polygon taken in order ; then the resultant of all these forces may be represented, in magnitude and direction, by the closing side of the polygon, taken in opposite order.”

ER. B.N.MOHANTA

20

21 of 26

ER. B.C.PANDEY

21

22 of 26

ER. B.N.MOHANTA

22

MOMENT

It is the turning effect produced by a force, on the body, on which it acts.

The moment of a force is equal to the product of the force and the perpendicular distance of the point, about which the moment is required and the line of action of the force.

23 of 26

ER. B.N.MOHANTA

23

TYPES OF MOMENTS

  1. Clockwise moments.

  • Anticlockwise moments.

24 of 26

VARIGNON’S THEOREM

  • It states, “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.”

ER. B.N.MOHANTA

24

25 of 26

COUPLE

  • A pair of two equal and unlike parallel forces (i.e. forces equal in magnitude, with lines of action parallel to each other and acting in opposite directions) is known as a couple.
  • As a matter of fact, a couple is unable to produce any translatory motion (i.e., motion in a straight line).
  • But it produces a motion of rotation in the body, on which it acts.
  • The simplest example of a couple is the forces applied to the key of a lock, while locking or unlocking.

ER. B.N.MOHANTA

25

26 of 26

ER. B.N.MOHANTA

26

THANK YOU