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Static Equilibrium in Physics

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26 diapositives · 476 Views · Jan 04, 2020

Learn about static equilibrium and rotational dynamics, including the conditions for equilibrium and torque equations to solve problems effectively.

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Static Equilibrium in Physics
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  1. Static Equilibrium AP Physics Chapter 9

  2. Static Equilibrium 8.4 Torque

  3. 8.4 Torque Rotational Dynamics – the causes of rotational motion Caused by Torque, or a force applied at a distance from the pivot point t=torque (Nm) F=force (N) r=torque arm (m) 8-4

  4. 8.4 Torque Force causes no rotation if it is applied at the pivot point 8-4

  5. 8.4 Torque If the force is applied at an angle then only the perpendicular component matters So q must be the angle Between the force And the torque arm 8-4

  6. Static Equilibrium 9.1 The Conditions of Equilibirum

  7. 9.1 The Conditions for Equilibrium Two Conditions The sum of all forces is zero mathematically examples Called Translational equilibrium 9.1

  8. 9.1 The Conditions for Equilibrium The second condition for equilibrium – the sum of all torques equals zero The pivot point chosen does not matter since there is no real rotation 9.1

  9. 9.1 The Conditions for Equilibrium Counterclockwise is considered positive torque Clockwise negative torque Mass – negative torque Spring scale – positive torque 9.1

  10. 9.1 The Conditions for Equilibrium Steps in Problem Solving Make a free body diagram Choose a coordinate system and resolve the forces into their components Write down the equilibrium equations for the forces Write down the torque equilibrium equation Solve 9.1

  11. 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? 9.1

  12. P1 P2 2m W 5m 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Free Body Diagram 9.1

  13. P1 P2 2m W 5m 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Force Equations 9.1

  14. P1 P2 2m W 5m 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Pivot Point 9.1

  15. P1 P2 2m W 5m 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Torque Equation Angles 9.1

  16. P1 P2 2m W 5m 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Torque Equation 9.1

  17. 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Solve 9.1

  18. 9.1 The Conditions for Equilibrium Example: A happy 50 kg dude stands 2 m from the left side of a 5 m long bridge. The bridge is supported at each end by pylons. What is the force on each pylon? Solve 9.1

  19. 9.1 The Conditions for Equilibrium Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. 9.1

  20. Nw NC 4 m f mg 9.1 9.1 The Conditions for Equilibrium Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Free body diagram

  21. Nw NC 4 m f mg 9.1 9.1 The Conditions for Equilibrium Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Axis?

  22. Nw NC 4 m f mg 9.1 9.1 The Conditions for Equilibrium Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Force Equations

  23. Nw NC 4 m f mg 9.1 9.1 The Conditions for Equilibrium 53o Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Torque Equations Pick a pivot the eliminates variable Calculate angles 37o 37o 53o

  24. Nw NC 4 m f mg 9.1 9.1 The Conditions for Equilibrium 53o Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Torque Equations Write your torque equation 37o 37o 53o

  25. 9.1 The Conditions for Equilibrium Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Solve

  26. 9.1 The Conditions for Equilibrium Example: A 5 m long ladder leans against a wall at a point 4 m above a cement floor. The ladder is uniform and has a mass of 12 kg. Assuming the wall is frictionless (but the floor is not) determine the forces exerted on the ladder by the floor and by the wall. Solve