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Force and Motion Force and Motion

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Page 1: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Force and MotionForce and Motion

Page 2: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

This week –This week – Force and Motion – Chapter 4Force and Motion – Chapter 4

Page 3: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Thinking About MotionThinking About Motion

What makes objects move?What makes objects move? How do they move?How do they move? Can we make our daily observations Can we make our daily observations

quantitative? Can we understand??quantitative? Can we understand??

Page 4: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Sir Isaac Newton 1643-Sir Isaac Newton 1643-17271727 One of the two One of the two

“inventors” of the “inventors” of the CalculusCalculus

The Law of GravitationThe Law of Gravitation Optics Optics Laws of Motion (N1, N2, Laws of Motion (N1, N2,

N3)N3)

Page 5: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Force Force is the fundamental concept being

introduced in this chapter. We have an intuitive understanding of what a

FORCE is … a push or a pull. We will discuss the physical changes that are

induced when we apply a FORCE to an object.

Page 6: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Force Forces are what cause any change in the

velocity of an object A force is that which causes an acceleration

The net force is the vector sum of all the forces acting on an object Also called total force, resultant force, or

unbalanced force The net force on an object can be ZERO

Page 7: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

NEWTON’S FIRST LAW (N1) An object is in EQULIBRIUM when the sum

of all of the forces acting on it is zero. An object in EQUILIBRIUM will either be

(and remain) at rest (no motion), or Will move with CONSTANT VELOCITY

Page 8: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

What if the net force is NOT ZERO? N2

Newton’s SECOND LAW If there is a non-zero (unbalanced) force applied to

an object, it will accelerate. The acceleration is proportional to the force but is

different for every object. The proportionality constant is “m” and is called the

mass. The mass of an object is a measure of the total

“amount of matter” contained by the object.

Page 9: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Newton’s Second Law

Page 10: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

More better ….

aF

aF

m

m

objecttheonacting

Forcesallj

Page 11: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Units of Mass

Page 12: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Inertia and Mass The tendency of an object to resist any

attempt to change its velocity is called inertia Mass is that property of an object that

specifies how much resistance an object exhibits to changes in its velocity

Page 13: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Zero Net Force When the net force is equal to zero:

The acceleration is equal to zero The velocity is constant

Equilibrium occurs when the net force is equal to zero The object, if at rest, will remain at rest If the object is moving, it will continue to move at

a constant velocity

Page 14: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Classes of Forces Contact forces involve

physical contact between two objects

Field forces act through empty space No physical contact is

required

Page 15: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Weight a minute ….

a

FORCE=

WEIGHT

Object will “fall” with an accelerationof g m/s2

Since F=ma=mg in this case, theWEIGHT of the object can bedescribed by

W=mgW=mg

Page 16: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

More About Forces A spring can be used to

calibrate the magnitude of a force

Forces are vectors, so you must use the rules for vector addition to find the net force acting on an object

Page 17: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

More About Mass Mass is an inherent property of an object Mass is independent of the object’s

surroundings Mass is independent of the method used to

measure it Mass is a scalar quantity The SI unit of mass is kg

Page 18: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Newton’s First Law – Alternative Statement In the absence of external forces, when viewed from

an inertial reference frame, an object at rest remains at rest and an object in motion continues in motion with a constant velocity Newton’s First Law describes what happens in the

absence of a force Also tells us that when no force acts on an object, the

acceleration of the object is zero

Page 19: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Mass vs. Weight Mass and weight are two different quantities Weight is equal to the magnitude of the

gravitational force exerted on the object Weight will vary with location

Page 20: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Newton’s THIRD Law – N3

mg

Because it was in equilibrium, the table must have been pushing UP on the brick with the same force as the weight of the brick. This is “action and Reaction”.

Page 21: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Newton’s Third Law If two objects interact, the force F12 exerted

by object 1 on object 2 is equal in magnitude and opposite in direction to the force F21 exerted by object 2 on object 1

F12 = - F21

Note on notation: FAB is the force exerted by A on B

Page 22: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Newton’s Third Law, Alternative Statements Forces always occur in pairs A single isolated force cannot exist The action force is equal in magnitude to the

reaction force and opposite in direction One of the forces is the action force, the other is the

reaction force It doesn’t matter which is considered the action and which

the reaction The action and reaction forces must act on different

objects and be of the same type

Page 23: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

VERY IMPORTANT CONCEPT

The “action” force The “action” force and the “reaction” and the “reaction”

force act on force act on DIFFERENT bodies.DIFFERENT bodies.

Page 24: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

To solve problems using N123 Always ISOLATE the SINGLE object that you are

considering. Indicate ALL of the forces acting on the object

including reaction forces. Resolve all of the forces into the appropriate

components. For each component:

forces = 0 for a body in equilibrium forces = ma for a body that is accelerating

Page 25: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Free Body Diagram In a free body diagram,

you want the forces acting on a particular object

The normal force and the force of gravity are the forces that act on the monitor

Page 26: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Equilibrium, Example

A lamp is suspended from a chain of negligible mass

The forces acting on the lamp are the force of gravity (Fg)

the tension in the chain (T) Equilibrium gives

0 0y gF T F gT F

Page 27: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Equilibrium, Example 1b The forces acting on the

chain are T’ and T” T” is the force exerted by

the ceiling T’ is the force exerted by

the lamp T’ is the reaction force to T Only T is in the free body

diagram of the lamp, since T’ and T” do not act on the lamp

Page 28: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Equilibrium Conceptualize the

traffic light Categorize as an

equilibrium problem No movement, so

acceleration is zero forces = 0

Page 29: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Objects Experiencing a Net Force If an object that can be modeled as a particle

experiences an acceleration, there must be a nonzero net force acting on it.

Draw a free-body diagram Apply Newton’s Second Law in component

form

Page 30: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Newton’s Second Law Forces acting on the

crate: A tension, the

magnitude of force T The gravitational force,

Fg

The normal force, n, exerted by the floor

Page 31: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Note About the Normal Force The normal force is not

always equal to the gravitational force of the object

For example, in this case

n may also be less than Fg

0y gF n F F and gn F F

Page 32: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Inclined Planes Forces acting on the object:

The normal force, n, acts perpendicular to the plane

The gravitational force, Fg, acts straight down

Choose the coordinate system with x along the incline and y perpendicular to the incline

Replace the force of gravity with its components

Page 33: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Multiple Objects When two or more objects are connected or in

contact, Newton’s laws may be applied to the system as a whole and/or to each individual object

Whichever you use to solve the problem, the other approach can be used as a check

Page 34: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Multiple Objects First treat the system as a

whole:

Apply Newton’s Laws to the individual blocks

Solve for unknown(s) Check: |P21| = |P12|

systemx xF m a

Page 35: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Multiple Objects Forces acting on the objects:

Tension (same for both objects, one string)

Gravitational force Each object has the same

acceleration since they are connected

Draw the free-body diagrams Apply Newton’s Laws Solve for the unknown(s)

Page 36: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Multiple Objects

Draw the free-body diagram for each object One cord, so tension is the same for both objects Connected, so acceleration is the same for both objects

Apply Newton’s Laws Solve for the unknown(s)

Page 37: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Forces of Friction When an object is in motion on a surface or

through a viscous medium, there will be a resistance to the motion This is due to the interactions between the object

and its environment This resistance is called the force of friction

Page 38: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Forces of Friction Friction is proportional to the normal force

ƒs µs n and ƒk= µk n

These equations relate the magnitudes of the forces, they are not vector equations

The force of static friction is generally greater than the force of kinetic friction

The coefficient of friction (µ) depends on the surfaces in contact

Page 39: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Forces of Friction The direction of the frictional force is

opposite the direction of motion and parallel to the surfaces in contact

The coefficients of friction are nearly independent of the area of contact

Page 40: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Static Friction Static friction acts to keep

the object from moving If F increases, so does ƒs

If F decreases, so does ƒs

ƒs µs n where the equality holds when the surfaces are on the verge of slipping Called impending motion

Page 41: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Kinetic Friction The force of kinetic

friction acts when the object is in motion

Although µk can vary with speed, we shall neglect any such variations

ƒk = µk n

Page 42: Force and Motion This week – This week – Force and Motion – Chapter 4 Force and Motion – Chapter 4

Some Coefficients of Friction