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DEFINITION
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The
process of splitting a vector into various parts
or components is called "RESOLUTION OF VECTOR"
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These parts of a vector may act
in different directions and are called "components of vector".
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We
can resolve a vector into a number of components .Generally there are three
components of vector viz.
Component along X-axis called x-component Component along Y-axis called Y-component Component along Z-axis called Z-component |
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Here
we will discuss only two components x-component & Y-component which are
perpendicular to each other.These components are called rectangular components of
vector.
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METHOD OF RESOLVING
A VECTOR INTO RECTANGULAR COMPONENTS |
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Consider
a vector V acting at a point making
an angle q with positive
X-axis. Vector V is
represented by a line OA.From point A draw a perpendicular AB on X-axis.Suppose OB and BA represents two vectors.Vector OA is parallel to X-axis and vector BA is parallel to Y-axis.Magnitude of these vectors are Vx and Vy respectively.By the method of head to tail we notice that the sum of these vectors is equal to vector V.Thus Vx and Vy are the rectangular components of vector V. Vx = Horizontal component of V. Vy = Vertical component of V. |
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MAGNITUDE OF
HORIZONTAL COMPONENT |
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Consider
right angled triangle DOAB
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MAGNITUDE OF
VERTICAL COMPONENT |
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Consider
right angled triangle DOAB
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Moments
The moment (or torque) of a force about
a turning point is the force multiplied by the perpendicular distance
to the force from the turning point.
Moments
are measured in newton metres (Nm).
Moment = F d
§ F = the force in newtons (N)
§ d = perpendicular distance in metres (m)
Example; A 10N force acts at a perpendicular
distance of 0.50m from the turning point. What is the moment of the force?
Moment = Fd
= 10 x 0.50
= 5.0 Nm
= 10 x 0.50
= 5.0 Nm
The
principle of moments.
” When
an object is in equilibrium the sum of the anticlockwise moments about a
turning point must be equal to the sum of the clockwise moments.”
sum of
anticlockwise moments = sum clockwise moments
Example;
Couple
If two opposite moments act to cause an object to rotate, such
as when your two hand are at the 'quarter-past-three' position on a car steering wheel, it is called a
couple. The moment of a couple is called the torque. It is
quite often said of engines and applys to the ability of the engine to turn the
wheels, or wrongly by Jeremy
Clarkson from 'Top
Gear' as in,
"This engine has a lot of torques."
Figure 2. A couple.
The torque is a psuedo-vector quantity. That is, it has
magnitude and it has a direction that is
projected perpendicular to the plane of the vectors F andr.
The direction of the vector from the plane follows a right-handed corkscrew
rule or equivalently the right-hand screw rule.
Torque is a psuedo-vector quanitity with the direction given by
the right-hand screw rule.
The
magnitude of the torque of a couple can be found by finding the net torque from clockwise and anti clockwise
moments acting on an arbitrary point of rotation.
T =F(x + d)
T =F x
Equating, F x +F d = F x.
Net Torque. T = F d
Equating, F x +F d = F x.
Net Torque. T = F d
Conditions for
Equilibrium
An object at equilibrium has no net influences to cause it to
move, either in translation (linear motion) or rotation. The basic conditions
for equilibrium are:
![](file:///C:/Users/FLAMES~1/AppData/Local/Temp/msohtmlclip1/01/clip_image010.gif)
The conditions for equilibrium are basic to the design of any
load-bearing structure such as a bridge or a building since such structures
must be able to maintain equilibrium under load. They are also important for
the study of machines, since one must first establish equilibrium and then
apply extra force or torque to produce the desired movement of the machine. The
conditions of equilibrium are used to analyze the "simple machines" which are the building blocks for more
complex machines.
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