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Also available on:
http://shilloi.iitg.ernet.in/~kd/me101.htm
Lecture Slides available on
http://www.iitg.ernet.in/kd/me101.htm
ME101 (Division III) webpage
Equivalent Systems: Resultants
Equilibrium
Equilibrium of a body is a condition in which the
resultants of all forces acting on the body is zero.
Condition studied in Statics
When the resultant of all forces on a body is not
zero, acceleration of the body is obtained by
equating the force resultant to the product of the
mass and acceleration of the body.
Condition studied in Dynamics
2ME101 - Division III Kaustubh Dasgupta
Equivalent Systems: Resultants
Vector Approach: Principle of Transmissibility can be used
Magnitude and direction of the resultant force R is obtained by
forming the force polygon where the forces are added head to
tail in any sequence
3ME101 - Division III Kaustubh Dasgupta
Equivalent Force and Couple
• Two dimensional plane
• Three dimensional space
5ME101 - Division III Kaustubh Dasgupta
Resultant of Force System:: 3D
• Three dimensional space
7ME101 - Division III Kaustubh Dasgupta
Equivalent
force-couple
systems for
each force
Resultant
equivalent
force-couple
system
Wrench Action
• Coincidence of resultant R and M axes
Positive Wrench Negative Wrench
8ME101 - Division III Kaustubh Dasgupta
Wrench Action
• Wrench action or Screw Driver action
9ME101 - Division III Kaustubh Dasgupta
Positive Wrench
Replacement of force system by wrench
10ME101 - Division III Kaustubh Dasgupta
Resolve M into components
Resolve M2 into a couple Resultant Wrench
For the beam, reduce the
system of forces shown to
(a) an equivalent force-
couple system at A,
(b) an equivalent force
couple system at B, and
(c) a single force or resultant
Solution:
a)Compute the resultant force for
the forces shown and the
resultant couple for the moments
of the forces about A.
b)Find an equivalent force-couple
system at B based on the
force-couple system at A.
c) Determine the point of
application for the resultant
force such that its moment
about A is equal to the
resultant couple at A.
Example on Equivalent System
11ME101 - Division III Kaustubh Dasgupta
SOLUTION:
a) Compute the resultant force and the
resultant couple at A.
jjjj
FR
N 250N 100N 600N 150
jR
N600
ji
jiji
FrM R
A
2508.4
1008.26006.1
kM R
A
mN 1880
Example on Equivalent System
12ME101 - Division III Kaustubh Dasgupta
b) Find an equivalent force-couple system at
B based on the force-couple system at A.
The force is unchanged by the movement
of the force-couple system from A to B.
jR
N 600
The couple at B is equal to the moment
about B of the force-couple system found
at A.
kk
jik
RrMM AB
R
A
R
B
mN 2880mN 1880
N 600m 8.4mN 1880
kM R
B
mN 1000
Example on Equivalent System
13ME101 - Division III Kaustubh Dasgupta
c)
FR = F1 + F2 + F3 + F4
R = 150-600+100-250 = -650 N
FRd = F1d1 + F2d2 + F3d3 + F4d4
d = 3.13 m
Example on Equivalent System
R
d
14ME101 - Division III Kaustubh Dasgupta
Example on resultant of a force system
• Determine the resultant of the system of parallel forces
acting on the plate. Solve with a vector approach.
15ME101 - Division III Kaustubh Dasgupta
Example on Wrench
• Replace the two forces and the negative wrench by a
single force R applied at A and the corresponding
couple M.
17ME101 - Division III Kaustubh Dasgupta
Rigid Body Equilibrium
A rigid body will remain in equilibrium provided
• sum of all the external forces acting on the body is
equal to zero, and
• Sum of the moments of the external forces about a
point is equal to zero
x
y
z
21ME101 - Division III Kaustubh Dasgupta
Rigid Body Equilibrium
Space Diagram: A sketch
showing the physical conditions
of the problem.
Free-Body Diagram: A sketch
showing only the forces on the
selected particle.
Free-Body Diagrams
22ME101 - Division III Kaustubh Dasgupta
Rigid Body Equilibrium
Support Reactions
Prevention of
Translation or
Rotation of a body
Restraints
23ME101 - Division III Kaustubh Dasgupta