PARTICLE
It is a body of infinite small dimensions may be considered as a point
only having the existence
For the shake of analysis, a body may be considered as a particle.
RIGID BODY
This is define as the body having no deformation or do not change it’s
shape and size ,called rigid body
In practical , no body is perfectly rigid body , but for the shake of
analysis we can take a body as rigid body.
DEFORMABLE BODY
This is define as the body having no deformation or changes it’s shape
and size under the action of forces called deformable body.
In practical , all the
bodies in this universe are deformable body.
ENGINEERING MECHANICS
It is the branch of science which most deals with the forces acting on a
body or particle. It is devided in two branches.
1.
Statics
2.
Dynamics
STATICS
It is the branch of engineering mechanics , which deals with the forces
and their effects when acting on body or particle at rest
In this branch the body is said to be in rest.
DYNAMICS
It is the branch of engineering mechanics , which deals with the forces
and their effects while acting upon the bodies in motions.
In this branch the bodies are said to be in motion under the action of
forces or without forces
It is devided into two branch.
1 . Kinetics
2 . Kinematics
1 . Kinetics
2 . Kinematics
KINETICS
It is the branch of engineering mechanics in which the motion of the
body occurred under the action of forces.
KINEMATICS
It is the branch of engineering mechanics in which the motion of the
body occurred without forces.
RESULTANT FORCE
If a number of forces are acting simultaneously on a body or particle ,
then it is possible to replace all the forces of a single forces which produce
the same effect as that produced by all the forces then the single force is
called resultant force of all the forces.
Here , R is the resultant force of f1, f2, f3.
EQUILIBRANT
EQUILIBRANT
The forces acting on a body exactly equalto the resultant force but
directed oppositly to the resultant force in the same line of action, called
equilibrant.
Here ,R be the resultant force and r` be the equilibrant.
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