FORCE
Definition: - It may be defined as an agent which produces or tends to produces, destroy or tends to destroy the motion of a body.
A
force while acting on a body may –
- Change the motion of a body
- Retard the motion of a body
- Balance the forces already acting on a body
- Give rise to the internal stress in a body
Parameters to describe a force: -
- Magnitude of the force,
- Direction of the force,
- Point of application.
Units – In CGS System – dyne
= 105 N
In
SI System – N
In MKS System – Kgf = 9.81 N
Principle of Transmissibility: -
If a force is acting on a body at any point, it can be transferred to another point on its line of action, Provided this point is rigidly connected with the body.
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Fig. 1 | Principle of Transmissibility |
System of forces: -
Types-
Coplanar forces: - The
forces, which lines of action
lying in the same plane, are called Coplanar forces.
Collinear forces: - The
forces, which lines of action lying in the same line, are called collinear
forces.
Concurrent forces: - If
a set of forces are meeting at a point, then the set of forces are called, concurrent
forces.
Parallel forces: - If
the lines of actions of a number of forces are parallel to each other, then the
forces are called Parallel forces.
a.
Like
Parallel forces: - The
parallel forces which lines of action are in the same direction.
b.
Unlike
Parallel forces: - The
parallel forces which lines of action are in the opposite direction.
Coplanar, concurrent forces: - The
forces, which lines of action lying in the same plane and also meet at a point,
are called coplanar concurrent forces.
Coplanar, non-concurrent forces: - The
forces, which lines of action do not lying in the same plane but do not meet at
a point, are called coplanar non-concurrent forces.
Non-coplanar, concurrent forces: - The
forces, which lines of action do not lying in the same plane but meet at a
point, are called non-coplanar concurrent forces.
Non-Coplanar, Non-concurrent forces: - The
forces, which lines of action do not lying in the same plane and do not meet at
a point, are called Non-coplanar Non-concurrent forces.
Resultant Force – It
is a single force which produces the same effect as produced by all the given
forces acting on a body.
Resultant
force can be determined by –
- Parallelogram law of forces
- Triangle law of forces
- Polygon law of forces
Parallelogram Laws of Forces: -
It
states that if two forces acting simultaneously on a particle, be represented
in magnitude and direction by the two adjacent sides of a parallelogram, then
their resultant may be represented in magnitude and direction by the diagonal
of the parallelogram which passes through the point of intersection.
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Fig.2 | Parallelogram law for force |
If R is the resultant force, then
R
= √ (P2 + Q2 + 2PQcosθ)
If
the resultant force is act at an angle ‘α’ then,
tan α = Qsinθ/ (P+Qcosθ)
- If θ = 00, i.e. cosθ = 1; Forces are acting in the same line and at the same direction then, Resultant (R) = P +Q
- If θ = 900, i.e. cosθ = 0; Forces are acting at perpendicular direction, then Resultant R = √ (P2 + Q2)
- If θ = 1800, i.e. cosθ = (-1); Forces are acting in the same line and at the opposite direction then, Resultant (R) = P – Q (If P > Q)
- If P = Q, forces are equal then resultant force R = 2P cos(θ/2)
Triangular Laws of Forces: -
It states that if two forces are acting simultaneously on a particle, be
represented in magnitude and direction by the two sides of a triangle taken in
order, then their resultant may be represented in magnitude and direction by
the third sides of the triangle taken in opposite order.
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Fig.3 | Triangle Law of force |
Polygon Laws of Forces: - It states that if a number of forces are acting simultaneously on a particle, be represented in magnitude and direction by the sides of a polygon taken in order, then their resultant is represented in magnitude and direction by the closing sides of the polygon taken in opposite order.
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Fig. 4 | Polygon Law of Force |
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Fig. 5 | Resolution of force |
A force is generally resolved along two mutually perpendicular directions.
Equilibrium: -If the resultant of
a number of forces acting on a rigid body are exactly balanced i.e. zero, then
the particle is said to be in equilibrium.
Condition of Equilibrium:
For coplanar concurrent forces: -
- Σ H = 0
- Σ V = 0
For coplanar non concurrent forces: -
- Σ H = 0
- Σ V = 0
- Σ M = 0
Lami’s Theorem: -If three coplanar
forces acting at a point be in equilibrium, then each force is proportional to
the sine of the angle between other two forces.
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Fig.6 | Lami's Theorem |
P/
Sinα = Q / sinβ = R/ sinγ
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