CH5 Applying Newton's Laws
 

 
1-D equilibrium¡ªFigure 5.1
 · Consider an athlete hanging on a massless rope.
 · Follow Example 5.1.
 
1-D equilibrium considering the rope¡ªFigure 5.2
 · If we re-did the previous example in a less ideal world? The weight of the rope should be included.
 · Refer to Example 5.2.
 
A crate on an inclined plane¡ªFigure 5.4
 · An object on an inclined plane will have components of force in x and y space.
 · Refer to Example 5.4.
 
Consider a mass on a plane tied to a cord over a pulley
 · You must draw two-free body diagrams.? The tension from the mass hanging is the same force that draws the cart up the ramp.
 · Refer to Example 5.5.
 
Straight-line motion with constant force¡ªFigure 5.7
 · Consider the sailboat mounted on an ice skate.
 · Refer to Example 5.6.
 
Consider motion against friction¡ªFigure 5.8
 · Earlier, we considered the effect of using ¡°real¡± rope in a tension calculation.? How about friction at work in a problem that slides an object?
 · Consider Example 5.7.
 
Calculation of tension in an elevator cable¡ªFigure 5.9
 · The elevator mass is balanced by tension in the cable (that¡¯s why they have that ¡°maximum capacity¡± sign on the wall).
 · Refer to Example 5.8.
 
More adventures in the elevator¡ªFigure 5.10
 · The elevator allows riders to experience different weights (without dieting).
 · Refer to Example 5.9.
 
Acceleration down a hill¡ªFigure 5.12
 · If you grew up in the northeast, you could often ride on snow and ice in the winter using sleds.
 
Two bodies with the same magnitude of acceleration
 · A glider on the air track connected over a pulley (»¬ÂÖ) to a falling mass.
 · Refer to Example 5.12 using Figure 5.15.

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