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BASICS OF APPLIED MECHANICS
PART 1
CONTENTS:-
• Concept of Rigid Body
• Scalar & Vector Quantities
• Concept of Force & its characterstics
• System of Forces
• Principle of Transimissibility
• Composition & Resolution of Forces
• Laws of Forces
A rigid body (also known as a rigid object) is a solid body in which deformation is
zero or so small it can be neglected. The distance between any two given points
on a rigid body remains constant in time regardless of external forces exerted on
it.
FORCE :-
Force is the push or pull on an object with mass that causes it to change velocity (to
accelerate). Force represents as a vector, which means it has both magnitude and
direction.
IMPORTANT FACTORS OF FORCE:-
LAW OF FORCES
Law of Parallelogram:-
The law of parallelogram of forces states that if two vectors acting on a particle at the same time be
represented in magnitude and direction by the two adjacent sides of a parallelogram drawn from a point
their resultant vector is represented in magnitude and direction by the diagonal of the parallelogram drawn
from the same point .
DERIVATION OF LAW
LAMI'S THEOREM
Basics of applied mechanics

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Basics of applied mechanics

  • 1. BASICS OF APPLIED MECHANICS PART 1
  • 2. CONTENTS:- • Concept of Rigid Body • Scalar & Vector Quantities • Concept of Force & its characterstics • System of Forces • Principle of Transimissibility • Composition & Resolution of Forces • Laws of Forces
  • 3. A rigid body (also known as a rigid object) is a solid body in which deformation is zero or so small it can be neglected. The distance between any two given points on a rigid body remains constant in time regardless of external forces exerted on it.
  • 4.
  • 5. FORCE :- Force is the push or pull on an object with mass that causes it to change velocity (to accelerate). Force represents as a vector, which means it has both magnitude and direction.
  • 7.
  • 8.
  • 9.
  • 10.
  • 12. Law of Parallelogram:- The law of parallelogram of forces states that if two vectors acting on a particle at the same time be represented in magnitude and direction by the two adjacent sides of a parallelogram drawn from a point their resultant vector is represented in magnitude and direction by the diagonal of the parallelogram drawn from the same point .