Forces and Newtons Laws of Motion The most

Forces and Newton’s Laws of Motion The most important chapter of physics EVAR

What is a Force? • A force is a push or a pull • Contact forces: – Boat pulling a water skier – Pushing a car with a dead battery • Noncontact forces: – Gravitational attraction of moon to earth – Magnetic attraction/repulsion – Electrostatic attraction/repulsion • The SI unit of force is the Newton (N)

Newton’s First Law • “An object at rest will stay at rest. An object in motion will stay in motion in a straight line unless acted upon by an external net force. ” • Take a moment to contemplate this truth of the universe. • Now, let’s look at the individual pieces of that statement….

Deconstructing Newton’s First Law • “…An object at rest will stay at rest…” – Things don’t just move spontaneously. If an object is just sitting there, it will continue to sit there unless something else pushes or pulls it. • “…An object in motion will tend to stay in motion in a straight line…” – The reason you are used to seeing things slow down in the real world is because they are usually acted upon by friction (or air resistance). In the absence of friction, however, objects would continue in a straight line forever until they hit something.

Deconstructing Newton’s First Law • “…by some external net force…” – ‘external’ means it comes from ‘outside’. Forces from within do not count as external forces – A ‘net force’ is the resultant force if you have several different forces acting on an object. – If there is only one force, then the net force is that force. – If there are several, you add them together as vectors to find the one final resultant force. – In order to show that, we need to know that….

What else can we say about forces? • Forces are vectors – That means they have magnitude and direction • A group of forces acting on the same object will add together graphically to produce a “net force” • This is why you learned to add vectors together. It wasn’t just for your health.

Example of finding net force – Tug of war Freshman Class Senior Class 800 Newtons 1000 Newtons Add individual vectors together resultant = Net force = 200 N @ 00

Example of finding net force – Pushing a car Bubba Earl 800 Newtons Add individual vectors together resultant = 1000 Newtons Net Force = 1800 Newtons @ 00

But Dr. Mason, those examples were far too easy Let’s look at a contrived example: Three kids pulling on a tire. ropes Witness the artistry Top down view tire

Kids pulling on tire problem Let’s look at the forces from each individual rope 10 N Θ 2 = 1350 Θ 3 = 2700 14. 14 N Θ 1 = 450

Kids pulling on tire problem 10 N Θ 1 = 450 FY = 7. 07 N What are the horizontal and vertical components of each force? F = 10 N FX = 7. 07 N Find the horizontal and vertical components of force the same way you do for other vectors.

Kids pulling on tire problem F = 10 N Θ 2 = 1350 FX = -7. 07 N FY = 7. 07 N What are the horizontal and vertical components of each force?

Now let’s look at all the forces again • Forces acting horizontally: – X-component of force 1 = 7. 07 N – X-component of force 2 = -7. 07 N – X-component of force 3 = 0 N • Forces acting vertically: – Y-component of force 1 = 7. 07 N – Y-component of force 2 = 7. 07 N – Y-component of force 3 = -14. 14 N • So, all forces in the X-direction add to Zero and all forces in Y-direction add to Zero • So net force on tire is Zero Newtons

Inertia and Mass • Inertia: the tendency for an object to remain at rest or in motion in a straight line. • Mass: a quantitative measure of inertia – SI unit for inertia/mass: kilogram (kg) • We will discuss mass at length shortly

Newton’s Second Law • This is the most important physics law you will learn. • It is way more important than that E=MC 2 business. • You ready for it? • Here it is: • F = MA – Force = mass X acceleration

Investigating Newton’s Second Law • F = ma • Or, more specifically, ΣF = ma – Where ‘Σ’ = the greek letter “sigma” and means “sum of” – So the sum of all the forces on an object are equal to that objects mass times its acceleration – As before, the forces on an object add together vectorally. This is how you find the resultant.

Examples of Newton’s 2 nd law • You are pushing a 200 kg sled over a completely frictionless frozen lake. Your applied force is 150 N. What is the sled’s acceleration? • F = ma -> 150 N = (200 kg)(a) • a = (150 N)/(200 kg) = 0. 75 m/s 2

More Examples of Newton’s 2 nd law • Now, you are pushing a 200 kg sled over a frozen lake with some friction. Your applied force is still 150 N, but now it is counteracted by a 100 N friction force. What is the sled’s acceleration? • • ΣF = ma So, 150 N – 100 N = ma 50 N = (200 kg)(a) a = (50 N)/(200 kg) = 0. 25 m/s 2

Mini-competition 1: Question 1 • Chuck Norris (who once successfully ordered a Big Mac at Burger King) has a fist of mass 0. 7 kg. Starting from rest, his fist achieves a velocity of 8 m/s in 0. 15 sec. What avg force does he generate to achieve this level of performance? • 37 N • If paper beats rock, rock beats scissors, and scissors beats paper, what beats all 3 at the same time? • Chuck Norris.

Mini-competition 1: Question 2 • Carla Wong serves a 58 gram tennis ball and accelerates it from rest to 45 m/s. The impact gives it a constant acceleration over 44 cm. What is the magnitude of the force on the ball? • 133 N

Newton’s 3 rd Law • “Whenever one body exerts a force on a second body, the second body exerts an oppositely directed force of equal magnitude on the first body. ” • Whenever you push on something, that something pushes back on you with the same force.

Newton’s Third law example • From the book: – An astronaut (92 kg) pushes on a satellite (11, 000 kg) with a force of 36 N. What is the accel of the astronaut? Of the Satellite? • Fastronaut on satellite = - Fsatellite on astronaut • Aastronaut = -F/mastronaut = -36 N/92 kg = -0. 30 m/s 2 • Asatellite = F/msatellite = 36 N/11, 000 kg = 0. 0033 m/s 2

Mini-competition 2: Question 1 • Charles Steigerwald pushes on a wall to the right with a force of 200 N. What is the force that the wall exerts on Charles? • -200 N

Mini-competition 2: Question 2 • Kurt Stegmeier (mass 63 kg) and Dr. Mason (mass 110 Kg) are sitting opposite one another in rolling chairs. They push off one another in opposite directions with a force of 100 N. Assuming perfectly frictionless school chairs and floors, what is the magnitude of the acceleration each experiences? • Dr. Mason: 0. 909 m/s 2 • Kurt: 1. 58 m/s 2

Gravitational Force Gravitational force is always attractive Fg = Gm 1 m 2/r 2 Fg = force of gravity M 1 = mass of first object M 2 = mass of second object r = distance between them (or specifically, between their centers of mass • G = 6. 67 X 10 -11 Nm 2/kg 2 • • •

A note on the center of mass • Every object has a center of mass • For purposes of calculating forces like gravity, you can assume that all the mass of the object is at the center of mass. • For a sphere (assuming uniform density), center of mass is the actual center r m 1 is like m 2 r m 1 m 2

Gravitational Force example 1 • What is magnitude of gravitational force between two particles of masses m 1 = 12 kg and m 2 = 25 kg separated by distance r = 1. 2 m? • F = Gm 1 m 2/r 2 • = 6. 67 X 10 -11 Nm 2/kg 2 (12 kg)(25 kg)/(1. 2 m)2 • = 1. 4 X 10 -8 N • Fg is very small for normal sized objects, which is why you don’t feel yourself being pulled sideways every time a car passes by.

Gravitational Force example 2 • What is the magnitude of Fg between the earth and the moon? • Mearth = 5. 9742 × 1024 kilograms • Mmoon = 7. 36 × 1022 kilograms • According to the internet (which is never wrong), distance between centers of mass = 384, 403 Km, or 384, 403, 000 m • Fg = 1. 98 X 1020 N

Super-neato explanation of g • Recall that F = Gm 1 m 2/r 2 • If we set m 1 = mass of the earth and r = radius of the earth, let’s see what happens: • rearth = 6 378. 1 km = 6. 3781 X 106 m • F = (6. 67 X 10 -11 Nm 2/kg 2)(5. 9742 × 1024 kg)(m 2)/(6. 3781 X 106 m)2 • F = (9. 795 m/s 2)(m 2) • i. e. all those numbers other than m 2 work out to be 9. 8 m/s 2

Mini-competition 3: Question 1 • Saturn has an equatorial radius of 6 X 107 m and a mass of 5. 67 X 1026 kg. What is the acceleration due to gravity at the equator of Saturn? What is the ratio of Sami Fekadu’s weight on Saturn to that on Earth? • 10. 5 m/s 2 • Ratio = 1. 07

Mini-competition 3: Question 2 • The mass of the earth is 5. 9742 × 1024 kg and the mass of the sun is 1. 99 X 10 30 kg. They are separated by a distance of 146 X 109 m. What is the magnitude of the gravitational attraction on the earth by the sun? • 3. 72 X 1022 N

Gravity and Weight • Mass is the amount of material that makes up an object • Weight is the gravitational force on that mass • W = mg • W = weight, m = mass and g = -9. 8 m/s 2

Weight example: Hubble Telescope • Hubble telescope has a mass of 11, 600 kg • What is it’s weight – Resting on the surface of the earth – In orbit at 598 km above the surface of the earth? • Wsurface = 1. 14 X 105 N • Worbit: need total distance from earth center = 6. 38 X 106 m + 598 X 103 m = 6. 98 X 106 m • Worbit = 0. 95 X 105 N • Weighs less in orbit, as expected

More about gravity • According to F = Gm 1 m 2/r 2 , force of gravity decreases as square of distance from center of mass www. rpdp. net/sciencetips_v 2/P 12 B 4. htm

Mini-competition 4: Question 1 • On the surface of the mysterious planet Jay-Z, the acceleration due to gravity is 14. 5 m/s 2. If an object weighing 45 N on earth were transported to this other planet, how much would it weigh? • 66. 58 N

Mini-competition 4: Question 2 • In the World’s Strongest Man competition, the past three different winners were Žydrūnas Savickas (mass 175 kg), Mariusz Pudzianowski (mass 142 kg) and Phil Pfister (mass 156 kg). What is their combined weight in Newtons? If one kg weighs 2. 2 pounds, what was their combined weight in pounds? • 4635. 4 N • 1040 pounds

Other forces: Normal force • ‘Normal’ means ‘perpendicular’ • FN = Normal force = the force that surface exerts on an object sitting on it. • If a 10 kg block is sitting on a table, it weighs 98 N • The table, then, exerts a 98 N force upwards on the block

Normal force examples • A 5 kg book is resting on a table. What is the normal force exerted on the book by the table? • A 15 N block is on a table. I push on the block with an additional 11 N. What is FN on the block? • The same 15 N block is on the table, but now I pull upwards on it with 11 N. What is FN on the block?

Normal force and Apparent Weight

Explanation of apparent weight • Remember, ΣF = ma • When standing in an elevator, FN is the normal force (force from floor on you). • Your weight = W = mg • ΣFy = FN – mg = ma, so FN = mg + ma • FN is your apparent weight, mg = your true weight

Example: moving elevators • A 100 kg man is on an elevator that is accelerating upwards at a rate of 5 m/s 2. What is the man’s apparent weight? • FN = mg + ma (a is positive if going upwards) • FN = (100 kg)(9. 8 m/s 2) + (100 kg)(5 m/s 2) • FN = (100 kg)(14. 8 m/s 2) = 1480 N • Now, how about 5 m/s 2 downwards? • FN = (100 kg)(4. 8 m/s 2) = 480 N

Friction • Friction is a force that resists the motion of two surfaces sliding along one another. • Motion must be relative • Recall the normal force, FN. The normal force is perpendicular to the surface. • By contrast, the frictional force is parallel to the surface. • Friction always opposes the motion. Always always.

Coefficient of Friction • The coefficient of friction is a dimensionless number (no units! The only one you’ll get all year!) that is a proportionality constant between the normal force and the frictional force between two surfaces. • Ff = μFN • The symbol for the coefficient of friction is the greek letter μ (written “mu” and pronounced “myoo”) • Fun Fact: there is no friction in New Zealand

But Dr. Mason, tell us more interesting and awesome facts about friction • There are two kinds of friction, static and kinetic – Static friction is friction between two objects that are not moving relative to one another • Example: a heavy crate on a carpet floor that when you push on it, you can’t move it. – Kinetic friction is friction between two objects that are moving relative to one another • Example: same heavy crate that Tim Tebow is pushing on, who can move it.

Why the distinction between static and kinetic friction? • Because, in general, the two are different magnitudes, even when you have the same two surfaces in contact with one another. • For example, to pull two random materials off the internet, the coefficients of static and kinetic friction between glass and nickel are • μS = 0. 78 • μK = 0. 56 • In general, kinetic friction is less than static friction. • I. e. it’s harder to get a ‘stuck’ object to move than to keep a sliding object moving

A freaky note on static friction • Picture, if you will, a block resting on the ground. Let us say that the block is very heavy and is hard to get moving. • The force of static friction can change depending on how much sideways force you apply to the block. • If you apply a small force, the frictional force is small to counteract your push. If you apply a medium-sized force, the frictional force will be medium-sized to counteract your push.

Freaky note continued • In fact, the frictional force will vary up to a maximum value of FFmax = μS FN • After it starts moving, there is a constant force of kinetic friction on the block = μK FN. • What would the implication be if the static frictional force did not vary with applied horizontal force?

Example from the book • A sled is resting on some snow with μS = 0. 35 • Sled + rider have mass = 38 kg. • What is the magnitude of horizontal force needed to get the sled moving? • Fneeded = μS FN = μS mg = (0. 35)(38 kg)(9. 8 m/s 2) = 130 N

A different example from the book • A sled is traveling with an initial velocity of 4 m/s on a horizontal stretch of snow. The coefficient of kinetic friction μK = 0. 05. How far does the sled go before coming to a halt? • Ff = μK FN = μKmg • Omg, we don’t know m! Whatever shall we do? ? • By Newton’s 2 nd law, ax = -Ff/m = - μKmg/m = - μKg • Now can use Vf 2 = Vi 2 + 2 ax to find x • X = 16. 3 m

Mini-competition 5: Question 1 • A rocket blasts off from rest and attains a speed of 45 m/s in 15 sec. An astronaut on board has a mass of 57 kg. What is his apparent weight during takeoff? • 730 N

Mini-competition 5: Question 2 • A box of calculators that students perpetually borrow weighs 45 N and sits at rest on a horizontal table. The coefficients of static and kinetic friction are 0. 65 and 0. 42, respectively. • A horizontal force of 36 N is applied to the box. Will it move and, if so, what will its acceleration be? • Yes, it will move @ 3. 72 m/s 2.

Mini-competition 5: Question 3 • Edward is driving a car at constant speed and Jacob is in the passenger seat. A cup of hot coffee is on the dashboard and μS = 0. 3 between it and the dash. What is the maximum acceleration the car can have without spilling the coffee on Jacob and making him go all aggro ‘n’ stuff? • A = F/m = Ff/m = μKmg/m = μKg = 2. 94 m/s 2. • You know vampires can’t go out during the day, right? I mean, like, seriously?

Equilibrium • Equilibrium means that the sum of all the forces acting on an object = zero. • If ΣF = ma and ΣF = 0, then what does a =? • a = 0 • For an object to be truly in equilibrium, we must look at both horizontal and vertical directions. – ΣFX = 0 – ΣFY = 0

You must achieve…. balance…. • How to analyze equilibrium situations: • Identify the system you wish to analyze – Is it a single object? Are two objects acting together? Are there ropes or pulleys or other things? • Draw a free body diagram • Choose a set of x- and y-axes. Resolve all forces along these axes. • Apply ΣFX = 0 and ΣFY = 0 • Solve for any unknown quantities

Example from the book – replacing an engine 100 T 1 Yoon Jae Sung is replacing the engine to his car. There is a rope with tension T 1 that goes up to a pulley and he pulls with tension T 2 as shown in the diagram. If the engine weighs 3150 N, find the tensions T 1 and T 2. 100 Engine W T 2

Example from the book – replacing an engine 100 T 1 Step 1: identify the system -The system is the engine plus two ropes Step 2: Draw the free body diagram All forces are acting on the ring at the center, so use that point as the center of your free body diagram. 100 Engine W T 2

Example from the book – replacing an engine 100 T 1 T 2 W 100 Engine W 100 T 2 Free Body Diagram

Example from the book – replacing an engine 100 T 1 Step 3: Choose a set of x- and y-axes. -Done Step 4: Resolve all forces along these axes. 100 T 2 W Force X-comp Ycomp T 1 cos(1000) T 1 sin(1000) T 2 T 2 cos(3500) T 2 sin(3500) W 0 - W

Example from the book – replacing an engine Step 5: Apply ΣFX = 0 and ΣFY = 0 100 T 1 ΣFX = 0 so T 1 cos(1000) + T 2 cos(3500) = 0 100 cos(1000) = -0. 173 cos(3500) = 0. 985 T 2 W so T 1*(-0. 173) + T 2*(0. 985) = 0

Example from the book – replacing an engine Step 5: Apply ΣFX = 0 and ΣFY = 0 100 T 1 ΣFY = 0 so T 1 sin(1000) + T 2 sin(3500) – W = 0 100 sin(1000) = 0. 985 sin(3500) = -0. 173 T 2 W so T 1*(0. 985) + T 2*(-0. 173) – W = 0

Example from the book – replacing an engine Step 6: Solve for the unknowns T 1*(-0. 173) + T 2*(0. 985) = 0 T 1*(0. 985) + T 2*(-0. 173) – W = 0 T 1*(-0. 173) + T 2*(0. 985) = 0, so T 1 = T 2[(0. 985/0. 173)] Substitute this into second equation T 2[(0. 985/0. 173)]*(0. 985) + T 2*(-0. 173) – 3150 = 0 T 2 = 579 N, so then T 1 = 3300 N