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2.9: FORCES IN EQUILIBRIUM
Forces in Equilibrium 	 When an object is in equilibrium, the resultant force acting on it is zero.  The object will either be  1. at rest  2. move with constant velocity.
RESULTANT FORCE A single force that represents the combined effect of two of more forces in magnitude and direction.
Examples( Label the forces acted on the objects)
Addition of Forces  Resultant force,  F = ____ + ____ 	 Resultant force,  F = ____ + ____
STEP 1  Using ruler and protractor, draw the two forces F1 and F2 from a point.
STEP 2  Complete the parallelogram
STEP 3 Draw the diagonal of the parallelogram. The diagonal represent the resultant force, F in magnitude and direction.
Resolution of Forces 	 A force F can be resolved into components which are perpendicular to each other:  (a) horizontal component , FX  (b) vertical component, FY
Resolution of Forces  Component of weight parallel to the plane  		= mg sin θ  Component of weight normal to the plane  		= mg cosθ 	 Fx= F cosθ  Fy= F sin θ

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F4 ch2.9

  • 1. 2.9: FORCES IN EQUILIBRIUM
  • 2. Forces in Equilibrium When an object is in equilibrium, the resultant force acting on it is zero. The object will either be 1. at rest 2. move with constant velocity.
  • 3. RESULTANT FORCE A single force that represents the combined effect of two of more forces in magnitude and direction.
  • 4. Examples( Label the forces acted on the objects)
  • 5. Addition of Forces Resultant force, F = ____ + ____ Resultant force, F = ____ + ____
  • 6.
  • 7. STEP 1 Using ruler and protractor, draw the two forces F1 and F2 from a point.
  • 8. STEP 2 Complete the parallelogram
  • 9. STEP 3 Draw the diagonal of the parallelogram. The diagonal represent the resultant force, F in magnitude and direction.
  • 10. Resolution of Forces A force F can be resolved into components which are perpendicular to each other: (a) horizontal component , FX (b) vertical component, FY
  • 11. Resolution of Forces Component of weight parallel to the plane = mg sin θ Component of weight normal to the plane = mg cosθ Fx= F cosθ Fy= F sin θ