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Chapter 5: Applications of Newton’s Laws
Brent Royuk Phys-111
Concordia University
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Friction • Definition: a _____ that opposes motion • Three types
– Static Contact – Kinetic Sliding – Rolling
• Friction depends on two things – The load – Nature of the two surfaces
• Smooth vs. scratchy • Real friction: Van der Waal’s Forces • Cold welding of metals
• Consider: What would you do if you were on a completely frictionless surface?
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Friction • http://www.engin.brown.edu/courses/en3/Notes/Statics/friction/friction.htm
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Friction Load
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Kinetic Friction • fk = µk N • What is µk?
– Coefficients: Table 5.1, p. 165 and next slide
• Kinetic Friction is: – Proportional to N – Independent of the relative speed of the
surfaces
– Independent of the area of contact of the surfaces
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Kinetic Friction Examples • Someone at the other end of the table
asks you to pass the salt. Feeling quite dashing, you slide the 50.0-g salt shaker in their direction, giving it an initial speed of 1.15 m/s. If the shaker comes to rest with a constant acceleration in 0.840 m, what is µk?
• Suppose you then lift up the table and incline it at an angle of 22o. Then you give the shaker a push. What acceleration does the shaker experience as it slides down the table?
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Static Friction • What is the nature of friction between surfaces that are
at rest with respect to each other? • What does it mean that µs > µk ?
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Static Friction • The static friction laws:
0 ≤ fs ≤ fs max fs max = µs N
• The Crate Problem – A worker wishes to use a rope to pull a 40.0-kg
crate across a floor. What force is necessary to get it moving if µs = 0.650?
– If he keeps pulling with that force and µk = 0.450, what will the acceleration of the crate be?
– Rework the problem with the worker pulling at a 30.0o angle.
• Place a penny on a board. Lift the board until the penny just starts to slide and measure the angle θ. What is µs?
Strings and Springs • String tension
– Strings can’t push, can only pull – Heavy vs. ideal
• Ideal pulleys merely change direction • Springs follow Hooke’s Law
F = -kx • The spring constant, k
– Units – Meaning
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Examples • A 10 kg weight and a 5 kg weight are hung
from a string, one above another. An upward force of 170 N is applied. What are the string tensions and the acceleration of the block?
– Standard Trick #1 • Two blocks of mass m1 = 2.5 kg and m2 =
3.5 kg are side-by-side on a frictionless table and connected by a string. A horizontal force of 12.0 N is applied to the block on the left. Find the acceleration of the blocks and the tension of the connecting string.
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Examples • Find T in terms of m, g and θ.
F θ
m T
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Examples • Find the acceleration of Atwood’s
Machine in terms of its masses m1 and m2. Find the string tension.
– Standard Trick #2
• Given m1 on an inclined plane at 32o, m2 hanging over a pulley at the top and pulling up the plane. m1 = 4.0 kg; m2 = 3.5 kg, µk = 0.24. The box is moving up the plane. What is the acceleration?
• Desk Problem: At a 30o angle, a box accelerates down an inclined plane at a rate of 0.85 m/s2.. Find µk.
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The Drag Force • An object moving through a fluid experiences a drag
force. – cannon ball sinking in water, car on
highway, baseball, parachutist, dust, coffee filters
• Fdrag α v2
• At terminal speed, Fdrag = mg
• Equation:
• ρ is the density of the fluid (1.2 kg/m3 for air), A is cross-sectional area, C is the shape coefficient, generally ranging from 0.5-1 (next slide)
€
vt =2mgCρA
F
drag= 1
2CρAv2
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Some Approximate Terminal Speeds • Object Speed (m/s) • cannonball 250 • 16-lb shot 145 • high caliber bullet 100 • sky diver 60-100 • baseball 42 • tennis ball 31 • basketball 20 • mouse 13 • ping-pong ball 9 • penny 9 • raindrop 7 • parachutist 5 • snowflake 1 • sheet of paper (flat) 0.5 • fluffy feather 0.4
You can drop a mouse down a thousand-yard mine shaft and, on arriving at the bottom, it gets a slight shock and walks away. A rat is killed, a man is broken, a horse splashes. -J.B.S. Haldane, British geneticist, 1892-1964
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Elevator Dynamics • If you stand on a scale in an accelerating
elevator, what does the scale read (W’)? • Scenarios:
• at rest or constant speed: W’ = W = mg • a = g/2 up • a = g/2 down • cable breaks • a = 2g up • a = 2g down
• So could you jump at the last second in a free-falling elevator in order to survive?