as defined before, force is the action of one body on...
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As defined before, force is the action of one body on another.
It is a vector quantity since its effect depends on the direction as
well as on the magnitude.
The effect of the force applied to the bracket depends on , the
angle q and the location of the point of application of .
P
P
P
q
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We can separate the action of a force on a body into two effects
as external and internal. External effects are the reactive forces
exerted on the bracket by the wall. Forces external to a body can
be either applied or reactive forces. Internal effect is the
resulting internal forces and deformations distributed
throughout the material of the bracket.
P
mgW yF
xF
M
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Forces are classified as either contact or body forces.
A contact force is produced by direct physical contact; an
example is the force exerted on a body by a supporting surface.
A body force is generated when a body is located within a force
field such as a gravitational, electric or magnetic field.
An example of a body force is your weight.
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Forces may be further classified as concentrated or
distributed.
Every contact force is applied over a finite area and is therefore
a distributed force.
However, when the dimensions of the area are very small
compared with the other dimensions of the body, the force may
be considered concentrated at a point.
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The weight of a body is the force of gravitational attraction
distributed over its volume and may be taken as a concentrated
force acting through the center of gravity.
concrete
Concentrated force
Distributed force
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Concrete (Beton)
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According to Newton’s third law, the action of a force is always
accompanied by an equal and opposite reaction. It is essential
to distinguish between the action and the reaction in a pair of
forces.
To do so, we first isolate the body in question and then identify
the force exerted on that body (not the force exerted by the
body).
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Concurrent forces are forces whose line of action all pass through a common point.
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The force vectors are all in the same plane.
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The line of action of the forces are parallel to each other.
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All the forces have a common line of action.
FB
FA=FBFA
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A tensile force applied on a body will tend to stretch or elongate the body,whereas a compressive force will tend to shrink the body in the direction ofthe applied force.
F
F
F
F
Tensile Compressive
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Let’s consider two bodies which are in contact. The force acting on body 1 from
body 2 is . can be divided into two components as a normal force , drawn
perpendicular to the tangent line at the point of contact and force , drawn
parallel to the tangent line.
F
F
fFN
(1)
(2)
tangent
(2)F
N
fF
(1)
tangent
F
N
fF
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is named as the normal component of the contact force and is named
as the friction component of the contact force. If the contacting surfaces
are smooth, then can be neglected ( ); but if the contacting surfaces
are rough it has to be taken into consideration.
N
fF
0fF
fF
The relationship between and is given by
Ff = mN
where m is a dimensionless coefficient of friction varying between 0 and 1.
N
fF
(1)
tangent
F
N
fF
tangent
(2)F
N
fF
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T
Forces in strings, cables, etc. are always taken along the string, cable, etc. and
their direction always points away from the body in consideration. They
exert force only when they are tight. When loose they exert no force. Hence,
they always work in tension. Usually their weights are neglected compared to
the forces they carry or support.
BCT
ADT
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Pulleys are wheels with grooves that are used to change the directions of belts
or ropes and generate a higher output load with a much smaller input force.
Unless stated otherwise, or apparent from the problem, the tension forces at
both sides of a belt are taken as equal. They are equal as long as the belt does
not slide on the pulley, and the pulley rotates freely with a constant
velocity.
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Spring force is always directed along the spring and is in the direction as if to
return the spring into its undeformed length.
Fspring=kx (Spring force)
(k: spring constant, x: deformation of the spring)
Fspring
P
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F=kx
F=kx
F=kx F=kx
F F
x1 x x2x1 x x2
F=kx F=kx
Unstretched Stretched Uncompressed CompressedPosition Position Position Position
x x
Stretched Compressed