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**Short Version : 5. Newton's Laws Applications**

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**Example 5.3. Restraining a Ski Racer**

A starting gate acts horizontally to restrain a 60 kg ski racer on a frictionless 30 slope. What horizontal force does the gate apply to the skier? since y n x : y : x Fh Fg

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**Alternative Approach Net force along slope (x-direction) : y n Fh**

Fg

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**5.2. Multiple Objects Example 5.4. Rescuing a Climber**

A 70 kg climber dangles over the edge of a frictionless ice cliff. He’s roped to a 940 kg rock 51 m from the edge. What’s his acceleration? How much time does he have before the rock goes over the edge? Neglect mass of the rope.

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Tension T = 1N throughout

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5.3. Circular Motion Uniform circular motion 2nd law: centripetal

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**Example 5.6. Engineering a Road**

At what angle should a road with 200 m curve radius be banked for travel at 90 km/h (25 m/s)? y x : y : n x a Fg

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**Example 5.7. Looping the Loop**

Radius at top is 6.3 m. What’s the minimum speed for a roller-coaster car to stay on track there? Minimum speed n = 0

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**Conceptual Example 5.1. Bad Hair Day**

What’s wrong with this cartoon showing riders of a loop-the-loop roller coaster? From Eg. 5.7: n m g = m a = m v2 / r ( a g ) Consider hair as mass point connected to head by massless string. Then T m g = m a where T is tension on string. Thus, T = m ( g a ) ( downward ) This means hair points upward ( opposite to that shown in cartoon).

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**Frictional Forces Pushing a trunk:**

Nothing happens unless force is great enough. Force can be reduced once trunk is going. Static friction s = coefficient of static friction Kinetic friction k = coefficient of kinetic friction k : < 0.01 (smooth), > 1.5 (rough) Rubber on dry concrete : k = 0.8, s = 1.0 Waxed ski on dry snow: k = 0.04 Body-joint fluid: k = 0.003

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**Example 5.11. Dragging a Trunk**

Mass of trunk is m. Rope is massless. Kinetic friction coefficient is k. What rope tension is required to move trunk at constant speed? y y : x : n T fs x Fg

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Rolling wheel:

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Skidding wheel 滑動的輪子 : kinetic friction 動摩擦 k 0.8 Rolling wheel 滾動的輪子 : static friction 靜摩擦 s 1 Rolling friction 滾動摩擦 r 0.01

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Dynamics of Wheels F fr fs

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Example Stopping a Car k & s of a tire on dry road are 0.61 & 0.89, respectively. If the car is travelling at 90 km/h (25 m/s), determine the minimum stopping distance. the stopping distance with the wheels fully locked (car skidding). (a) = s : (b) = k :

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**Steering Car turning to the left. Bicycle turning to the left.**

More details

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**Example 5.9. Steering A level road makes a 90 turn with radius 73 m.**

What’s the maximum speed for a car to negotiate this turn when the road is (a) dry ( s = 0.88 ). (b) covered with snow ( s = 0.21 ). (a) (b)

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5.5. Drag Forces Drag force: frictional force on moving objects in fluid. Depends on fluid density, object’s cross section area, & speed. Terminal speed: max speed of free falling object in fluid. Parachute: vT ~ 5 m/s. Ping-pong ball: vT ~ 10 m/s. Golf ball: vT ~ 50 m/s. Sky-diver varies falling speed by changing his cross-section. Drag & Projectile Motion

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Simple Machines

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Chapter 6 Force and Motion-II. 6.2 Friction Frictional forces are very common in our everyday lives. Examples: 1.If you send a book sliding down a horizontal.

Chapter 6 Force and Motion-II. 6.2 Friction Frictional forces are very common in our everyday lives. Examples: 1.If you send a book sliding down a horizontal.

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