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Concurrent Force Systems ENGR 221 January 15, 2003
Lecture Goals ,[object Object],[object Object],[object Object],[object Object]
Introduction - Definition   Concurrent Force Systems : A concurrent force system contains forces whose lines-of action meet at some one point.  Forces may be  tensile (pulling)
Introduction - Definition   Concurrent Force Systems : A concurrent force system contains forces whose lines-of action meet at some one point.  Forces may be  compressive (pushing)
Introduction - Definition   ,[object Object],[object Object],Force exerted on a body has two effects :
Introduction - Definition   If the force system acting on a body produces no external effect, the forces are said to be  in  balance  and the body experience no change in motion is said to be in  equilibrium . The process of reducing a force system to a simpler equivalent stem is called a  reduction.  The process of expanding a force or a force system into a less simple equivalent system is called a  resolution.
Introduction - Definition A  force  is a vector quantity that, when applied to some rigid body, has a tendency to produce translation (movement in a straight line) or translation and rotation of body.  When problems are given, a force may also be referred to as a load or weight. Characteristics of force are the  magnitude ,  direction (orientation) and  point of application .
Introduction - Definition Scalar Quantity  has magnitude only (not direction) and can be indicated by a point on a scale.  Examples are temperature, mass, time and dollars. Vector Quantities  have magnitude and direction.  Examples are wind velocity, distance between to points on a map and forces.
Introduction - Definition Collinear  : If several forces lie along the same line-of –action, they are said to be collinear. Coplanar  When all forces acting on a body are in the same plane, the forces are coplanar.
Introduction - Definition Type of Vectors Free Vector  - is vector which may be freely moved creating couples in space. Sliding Vector  - forces action on a rigid body  are represented by vectors which may move or slid along their line of action. Bound  Vector or Fixed Vector  - can not be moved without modifying the conditions of the problem.
Introduction - Definition Principle of  Transmissibility The principle of transmissibility states that the condition of equilibrium or of motion of a rigid body will remain unchanged if a  force F  action at a given point of the rigid body is replace by a  force F’  of the same magnitude and the same direction, but acting at a different point, provided that the two forces have the same line of action.
Introduction - Definition Principle of  Transmissibility Line of action
Introduction - Definitions   ,[object Object],[object Object],Types of Forces(Loads)
Introduction - Definitions   Resultant Forces If two forces  P  and  Q  acting on a particle A may be replaced by a single force  R , which has the same effect on the particle.
Introduction - Definitions   Resultant Forces This force is called the resultant of the forces P and Q and may be obtained by constructing a parallelogram, using P and Q as two sides of the parallelogram.  The diagonal that pass through A represents the resultant.
Introduction - Definitions   Resultant Forces This is known as the  parallelogram law  for the addition of two forces.  This law is based on experimental evidence,; it can not be proved or derived mathematically.
Introduction - Definitions   Resultant Forces For multiple forces action on a point, the forces can be broken into the components of x and y.
Vectors ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Homework (Due 1/22/03) ,[object Object],[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]
Example Problems ,[object Object]

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Concurrent Forces

  • 1. Concurrent Force Systems ENGR 221 January 15, 2003
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  • 3. Introduction - Definition Concurrent Force Systems : A concurrent force system contains forces whose lines-of action meet at some one point. Forces may be tensile (pulling)
  • 4. Introduction - Definition Concurrent Force Systems : A concurrent force system contains forces whose lines-of action meet at some one point. Forces may be compressive (pushing)
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  • 6. Introduction - Definition If the force system acting on a body produces no external effect, the forces are said to be in balance and the body experience no change in motion is said to be in equilibrium . The process of reducing a force system to a simpler equivalent stem is called a reduction. The process of expanding a force or a force system into a less simple equivalent system is called a resolution.
  • 7. Introduction - Definition A force is a vector quantity that, when applied to some rigid body, has a tendency to produce translation (movement in a straight line) or translation and rotation of body. When problems are given, a force may also be referred to as a load or weight. Characteristics of force are the magnitude , direction (orientation) and point of application .
  • 8. Introduction - Definition Scalar Quantity has magnitude only (not direction) and can be indicated by a point on a scale. Examples are temperature, mass, time and dollars. Vector Quantities have magnitude and direction. Examples are wind velocity, distance between to points on a map and forces.
  • 9. Introduction - Definition Collinear : If several forces lie along the same line-of –action, they are said to be collinear. Coplanar When all forces acting on a body are in the same plane, the forces are coplanar.
  • 10. Introduction - Definition Type of Vectors Free Vector - is vector which may be freely moved creating couples in space. Sliding Vector - forces action on a rigid body are represented by vectors which may move or slid along their line of action. Bound Vector or Fixed Vector - can not be moved without modifying the conditions of the problem.
  • 11. Introduction - Definition Principle of Transmissibility The principle of transmissibility states that the condition of equilibrium or of motion of a rigid body will remain unchanged if a force F action at a given point of the rigid body is replace by a force F’ of the same magnitude and the same direction, but acting at a different point, provided that the two forces have the same line of action.
  • 12. Introduction - Definition Principle of Transmissibility Line of action
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  • 14. Introduction - Definitions Resultant Forces If two forces P and Q acting on a particle A may be replaced by a single force R , which has the same effect on the particle.
  • 15. Introduction - Definitions Resultant Forces This force is called the resultant of the forces P and Q and may be obtained by constructing a parallelogram, using P and Q as two sides of the parallelogram. The diagonal that pass through A represents the resultant.
  • 16. Introduction - Definitions Resultant Forces This is known as the parallelogram law for the addition of two forces. This law is based on experimental evidence,; it can not be proved or derived mathematically.
  • 17. Introduction - Definitions Resultant Forces For multiple forces action on a point, the forces can be broken into the components of x and y.
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