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Engineering Fundamentals

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Title: Engineering Fundamentals


1
Engineering Fundamentals
  • Session 9

2
Equilibrium
  • A body is in Equilibrium if it moves with
    constant velocity. A body at rest is a special
    case of constant velocity i.e. v 0 constant.
  • For a body to be in Equilibrium the resultant
    force (meaning the vector addition of all the
    forces) acting on the body must be zero.
  • Resulting force vector addition of force
    vectors
  • A Force can be defined as 'that which tends to
    cause a particle to accelerate.

3
Equilibrium of Concurrent Forces
Equilibrant E are equal and opposite to Resultant
R
E -R
4
Particle Vs Rigid Body
  • A particle has dimension 0
  • A Rigid body is a non-particle body and it does
    not deform (change shape).

Concurrent forces all forces acting a the same
point
Coplanar forces all forces lie on the same plane
5
Conditions for Equilibrium
Explanation Sum of forces 0, Or F1 F2
Fn 0
Example
F1 F2 F3 0
6
Conditions for Equilibrium
  • Breaking down into x and y components

Example For three forces acting on a particle
7
Free Body Diagram
  • Free body diagram isolates a rigid body to
    describe the system of forces acting on it.

R
R
mg
R
R
8
Free Body Diagram
9
Definitions
  • System of Particles or BodiesTwo or more bodies
    or particles connected together are referred to
    as a system of bodies or particles.
  • External Force External forces are all the
    forces acting on a body defined as a free body or
    free system of bodies, including the actions due
    to other bodies and the reactions due to
    supports.

10
Transmissibility of Force
11
Load and Reaction
  • Loads are forces that are applied to bodies or
    systems of bodies.
  • Reactions at points supporting bodies are a
    consequence of the loads applied to a body and
    the equilibrium of a body.

12
Tensile and Compressive Forces
  • Pushing force on the body -- compressive force
  • Pulling force on a body -- a tensile force

13
Procedure for drawing a free body diagram
  • Step 1 Draw or sketch the body to be isolated
  • Step 2 Indicate all the forces that act on the
    particle.
  • Step 3 Label the forces with their proper
    magnitudes and directions

14
Example 1
15
Example 2
16
Example 3
17
Solution
  • Resultant R of the two forces in two ropes

18
Solution
Equilibrant E - R
19
Solution
Resultant R is the sum of the actions of the tow
ropes on the barge
E - R
Equilibrant E is the reaction of the barge to the
ropes
20
Moment and Couple
  • Moment of Force
  • Moment M of the force F about the point O is
    defined as M F dwhere d is the perpendicular
    distance from O to F
  • Moment is directional

21
Moment and Couple
Moment Force x Perpendicular Distance
22
Resultant of a system of forces
An arbitrary body subjected to a number of forces
F1, F2 F3. Resultant R F1 F2
F3 ComponentsRx F1x F2x F3xRy F1y F2y
F3y
23
Resultant Moment
Resultant moment Mo Sum of Moments Mo F1 l1
F2 l2 F3 l3 R l
24
Couple
  • For a Couple
  • R ???F 0
  • But Mo ? 0
  • Mo F(dl) - Fl Fd
  • Moment of couple is the same about every point
    in its plane

Mo F d
25
Example 4
  • Calculate the total (resultant) moment on the
    body.

26
Example 4 (Solution)
  • Taking moments about the corner A
  • Note that the forces form two couples or pure
    moments 3.6 Nm and 3.0 Nm (resultant force 0,
    moment is the same about any point).

27
F 10 N
Exercise
d 3 m
A
1. What is the moment of the 10 N force about
point A (MA)? A) 10 Nm B) 30 Nm
C) 13 Nm D) (10/3) Nm E) 7 Nm
28
APPLICATIONS
What is the net effect of the two forces on the
wheel?
29
APPLICATIONS
What is the effect of the 30 N force on the lug
nut?
30
MOMENT IN 2-D
The moment of a force about a point provides a
measure of the tendency for rotation (sometimes
called a torque).
31
Moment
F100
_____________
M
L20
32
Moment
F32N
L50cm
L300mm

M27.5N
F55N

M-9.6N
33
EXAMPLE 1
Given A 400 N force is applied to the frame and
? 20. Find The moment of the force at
A. Plan
1) Resolve the force along x and y axes. 2)
Determine MA using scalar analysis.
34
EXAMPLE 1
Solution ? Fx -400 cos 20 N ? Fy
-400 sin 20 N MA (400 cos 20)(2)
(400 sin 20)(3) Nm 1160 Nm
35
GROUP PROBLEM SOLVING
Given A 40 N force is applied to the wrench.
Find The moment of the force at O.
Plan 1) Resolve the force along x and y axes.
2) Determine MO using scalar analysis.
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