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Copyright © 2012 Pearson Education Inc. Quilibrium Physics 7C lecture 15 Thursday November 19, 8:00 AM – 9:20 AM Engineering Hall 1200.

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Presentation on theme: "Copyright © 2012 Pearson Education Inc. Quilibrium Physics 7C lecture 15 Thursday November 19, 8:00 AM – 9:20 AM Engineering Hall 1200."— Presentation transcript:

1 Copyright © 2012 Pearson Education Inc. Quilibrium Physics 7C lecture 15 Thursday November 19, 8:00 AM – 9:20 AM Engineering Hall 1200

2 Copyright © 2012 Pearson Education Inc. Introduction Many bodies, such as bridges, aqueducts, and ladders, are designed so they do not accelerate. Real materials are not truly rigid. They are elastic and do deform to some extent. We shall introduce concepts such as stress and strain to understand the deformation of real bodies.

3 Copyright © 2012 Pearson Education Inc. Conditions for equilibrium First condition: The sum of all the forces is equal to zero:  F x = 0  F y = 0  F z = 0 Second condition: The sum of all torques about any given point is equal to zero.

4 Copyright © 2012 Pearson Education Inc. Conditions for equilibrium First condition: The sum of all the forces is equal to zero:  F x = 0  F y = 0  F z = 0 Second condition: The sum of all torques about any given point is equal to zero.

5 Copyright © 2012 Pearson Education Inc. Conditions for equilibrium First condition: The sum of all the forces is equal to zero:  F x = 0  F y = 0  F z = 0 Second condition: The sum of all torques about any given point is equal to zero.

6 Copyright © 2012 Pearson Education Inc. Conditions for equilibrium First condition: The sum of all the forces is equal to zero:  F x = 0  F y = 0  F z = 0 Second condition: The sum of all torques about any given point is equal to zero.

7 Copyright © 2012 Pearson Education Inc. Which of the following situations satisfies both the first condition for equilibrium (net force = 0) and the second condition for equilibrium (net torque = 0)? A. an automobile crankshaft turning at an increasing angular speed in the engine of a parked car B. a seagull gliding at a constant angle below the horizontal and at a constant speed C. a thrown baseball that does not rotate as it sails through the air D. more than one of the above E. none of the above Q11.1

8 Copyright © 2012 Pearson Education Inc. Which of the following situations satisfies both the first condition for equilibrium (net force = 0) and the second condition for equilibrium (net torque = 0)? A. an automobile crankshaft turning at an increasing angular speed in the engine of a parked car B. a seagull gliding at a constant angle below the horizontal and at a constant speed C. a thrown baseball that does not rotate as it sails through the air D. more than one of the above E. none of the above A11.1

9 Copyright © 2012 Pearson Education Inc. Center of gravity We can treat a body’s weight as though it all acts at a single point— the center of gravity. If we can ignore the variation of gravity with altitude, the center of gravity is the same as the center of mass.

10 Copyright © 2012 Pearson Education Inc. Walking the plank find the stable positions

11 Copyright © 2012 Pearson Education Inc. Walking the plank find the stable positions

12 Copyright © 2012 Pearson Education Inc. A rock is attached to the left end of a uniform meter stick that has the same mass as the rock. How far from the left end of the stick should the triangular object be placed so that the combination of meter stick and rock is in balance? A.less than 0.25 m B.0.25 m C. between 0.25 m and 0.50 m D. 0.50 m E. more than 0.50 m Q11.2

13 Copyright © 2012 Pearson Education Inc. A rock is attached to the left end of a uniform meter stick that has the same mass as the rock. How far from the left end of the stick should the triangular object be placed so that the combination of meter stick and rock is in balance? A11.2 A.less than 0.25 m B.0.25 m C. between 0.25 m and 0.50 m D. 0.50 m E. more than 0.50 m

14 Copyright © 2012 Pearson Education Inc. Will the ladder slip? find the tilt angles for stable conditions

15 Copyright © 2012 Pearson Education Inc. Will the ladder slip? find the tilt angles for stable conditions

16 Copyright © 2012 Pearson Education Inc. A.T = w sin  B.T = w cos  C. T = w/(sin  ) D. T = w/(cos  ) E. none of the above Q11.3 A metal advertising sign (weight w) is suspended from the end of a massless rod of length L. The rod is supported at one end by a hinge at point P and at the other end by a cable at an angle  from the horizontal. What is the tension in the cable?

17 Copyright © 2012 Pearson Education Inc. A11.3 A metal advertising sign (weight w) is suspended from the end of a massless rod of length L. The rod is supported at one end by a hinge at point P and at the other end by a cable at an angle  from the horizontal. What is the tension in the cable? A.T = w sin  B.T = w cos  C. T = w/(sin  ) D. T = w/(cos  ) E. none of the above

18 Copyright © 2012 Pearson Education Inc. A.the weight of the sign B.the tension in the cable C. the vertical force component exerted on the rod by hinge P D. two or more of these are tied for least A11.4 A metal advertising sign (weight w) is suspended from the end of a massless rod of length L. The rod is supported at one end by a hinge at point P and at the other end by a cable at an angle  from the horizontal. Which of these forces is least?

19 Copyright © 2012 Pearson Education Inc. A11.4 A metal advertising sign (weight w) is suspended from the end of a massless rod of length L. The rod is supported at one end by a hinge at point P and at the other end by a cable at an angle  from the horizontal. Which of these forces is least? A.the weight of the sign B.the tension in the cable C. the vertical force component exerted on the rod by hinge P D. two or more of these are tied for least

20 Copyright © 2012 Pearson Education Inc. Equilibrium and pumping iron Follow Example 11.4 using Figure 11.10 below.


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