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Figure 12.1 A single force F acts on a rigid object at the point P.
Fig. 12.1, p.363
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Figure 12.2 Two forces of equal magnitude are applied at equal distances from the center of mass of a rigid object. Fig. 12.2, p.364
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Figure 12. 3 Three forces act on an object
Figure Three forces act on an object. Notice that the lines of action of all three forces pass through a common point. Fig. 12.3, p.364
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Figure 12.4 Construction showing that if the net torque is zero about origin O, it is also zero about any other origin, such as O’. Fig. 12.4, p.365
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Figure 12.5 An object can be divided into many small particles each having a specific mass and specific coordinates. These particles can be used to locate the center of mass. Fig. 12.5, p.365
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Figure 12.6 The center of gravity of an object is located at the center of mass if g is constant over the object. Fig. 12.6, p.365
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Figure This one-bottle wine holder is a surprising display of static equilibrium. The center of gravity of the system (bottle plus holder) is directly over the support point. (Charles D. Winters) Fig. 12.7, p.366
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Figure 12.8 A balanced system.
Fig. 12.8, p.367
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Figure 12.9 (a) The biceps muscle pulls upward with a force F that is essentially at a right angle to the forearm. Fig. 12.9a, p.368
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Figure 12.9 (b) The mechanical model for the system described in part (a).
Fig. 12.9b, p.368
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Figure 12. 10 (a) A uniform beam supported by a cable
Figure 12.10 (a) A uniform beam supported by a cable. A person walks outward on the beam. Fig a, p.369
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Figure 12. 10 (b) The free-body diagram for the beam
Figure 12.10 (b) The free-body diagram for the beam. (c) The free-body diagram for the beam showing the components of R and T. Fig bc, p.369
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Figure 12.10 (b) The free-body diagram for the beam.
Fig b, p.369
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Figure 12.10 (c) The free-body diagram for the beam showing the components of R and T.
Fig c, p.369
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Figure (a) A uniform ladder at rest, leaning against a smooth wall. The ground is rough. (b) The free-body diagram for the ladder. (c) A person of mass M begins to climb the ladder when it is at the minimum angle found in part (a) of the example. Will the ladder slip? Fig ab, p.370
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Figure 12.11 (a) A uniform ladder at rest, leaning against a smooth wall. The ground is rough.
Fig a, p.370
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Figure 12.11 (b) The free-body diagram for the ladder.
Fig b, p.370
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Figure (c) A person of mass M begins to climb the ladder when it is at the minimum angle found in part (a) of the example. Will the ladder slip? Fig c, p.370
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Figure 12.12 (a) A wheelchair and person of total weight mg being raised over a curb by a force F.
Fig a, p.371
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Figure 12. 12 (b) Details of the wheel and curb
Figure 12.12 (b) Details of the wheel and curb. (c) The free-body diagram for the wheel when it is just about to be raised. Three forces act on the wheel at this instant: F, which is exerted by the hand; R, which is exerted by the curb; and the gravitational force mg. (d) The vector sum of the three external forces acting on the wheel is zero. Fig bcd, p.371
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Figure 12.12 (b) Details of the wheel and curb.
Fig b, p.371
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Figure 12.12 (c) The free-body diagram for the wheel when it is just about to be raised. Three forces act on the wheel at this instant: F, which is exerted by the hand; R, which is exerted by the curb; and the gravitational force mg. (d) The vector sum of the three external forces acting on the wheel is zero. Fig c, p.371
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Figure 12.12 (d) The vector sum of the three external forces acting on the wheel is zero.
Fig d, p.371
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Figure 12. 13 (a) Truss structure for a bridge
Figure 12.13 (a) Truss structure for a bridge. (b) The forces acting on the pins at points A, B, C, and E. Force vectors are not to scale. Fig , p.372
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Figure 12.13 (a) Truss structure for a bridge.
Fig a, p.372
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Figure 12.13 (b) The forces acting on the pins at points A, B, C, and E. Force vectors are not to scale. Fig b, p.372
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Active Figure A long bar clamped at one end is stretched by an amount ∆L under the action of a force F. At the Active Figures link at you can adjust the values of the applied force and Young’s modulus to observe the change in length of the bar. Fig , p.373
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Figure 12.15 Stress-versus-strain curve for an elastic solid.
Fig , p.374
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Active Figure 12.16 (a) A shear deformation in which a rectangular block is distorted by two forces of equal magnitude but opposite directions applied to two parallel faces. (b) A book under shear stress. At the Active Figures link at you can adjust the values of the applied force and the shear modulus to observe the change in shape of the block in part (a). Fig , p.374
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Active Figure 12.16 (a) A shear deformation in which a rectangular block is distorted by two forces of equal magnitude but opposite directions applied to two parallel faces. Fig a, p.374
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Fig. 12.16b, p.374 Active Figure 12.16 (b) A book under shear stress.
At the Active Figures link at you can adjust the values of the applied force and the shear modulus to observe the change in shape of the block in part (a). Fig b, p.374
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Table 12.1, p.374
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Active Figure 12.17 When a solid is under uniform pressure, it undergoes a change in volume but no change in shape. This cube is compressed on all sides by forces normal to its six faces. At the Active Figures link at you can adjust the values of the applied force and the bulk modulus to observe the change in volume of the cube. Fig , p.375
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Figure 12.18 (a) A concrete slab with no reinforcement tends to crack under a heavy load. (b) The strength of the concrete is increased by using steel reinforcement rods. (c) The concrete is further strengthened by prestressing it with steel rods under tension. Fig , p.376
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Fig. P12.1, p.378
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Fig. P12.4, p.378
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Fig. P12.5, p.378
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Fig. P12.8, p.379
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Fig. P12.15, p.380
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Fig. P12.73, p.387
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