Title: Forces and the Laws of Motion
1Forces and the Laws of Motion
2What is a Force?
- Recall that acceleration describes a change in an
objects velocity and velocity describes a change
in an objects position. - dr/dt v
- dv/dt a
3What is a Force?
- A force is a push or a pull on an object that
causes a change in the objects acceleration. - Forces can start motion, stop motion, or change
the path of motion. - The SI unit of force is the newton (N) named
after Sir Isaac Newton.
4What is a Force?
- The newton is defined as the amount of force,
that when acting on a 1 kg mass, produces an
acceleration of 1 m/s2. - N kg m/s2
- Forces are vectors
- The object experiencing the force is called the
system, and the world around the object creating
the force is called the environment.
5What is a Force?
- There are two main types of forces Contact and
Field Forces - A contact force is a force that arises from the
physical contact of two objects. - A field force, or long range force, is exerted
without physical contact between objects.
6What is a Force?
- Examples of field forces include gravity and the
attraction/repulsion between electrical charges. - The theory of fields was developed by Michael
Faraday to explain how objects could exert a
force on each other without ever touching. - At the atomic level, all forces can be classified
as field forces.
7What is a Force?
- Currently, there are only four known forces.
- Strong Forces (subatomic particles)
- Electromagnetic (attraction/repulsion between
electric charges) - Weak Forces (radioactive decay processes)
- Gravity
8What is a Force?
- Each force has an immediate and identifiable
cause known as an agent. - The agent for gravity is the Earths mass.
- If you cannot identify the agent, the force does
not exist.
9Force-Diagrams
- A force diagram, also known as a free-body
diagram, is a pictorial representation of all the
forces acting on an object or system. - A free-body diagram shows only the object and any
forces (contact and field) acting on it.
10Force-Diagrams
- Represent the object by a dot (particle model).
- Represent all forces acting on the object by
using arrows. - The tail of the arrow (force vector) is always on
the object even if the force is a push. - Label the force using F and a subscript to denote
the type of force or agent. (Fg force due to
gravity).
11Force-Diagrams
12Newtons 1st Law of Motion
- In the late 1600s, Sir Isaac Newton summarized
the way in which force influence motion into
three clear and concise laws. - These laws apply only to objects with velocities
ltlt the speed of light, and for inertial reference
frames.
13Newtons 1st Law of Motion
- If an object has no force acting on it, is the
object at rest or in motion? - A common misconception is that an object with no
force acting on it will always be at rest. - Imagine rolling a ball on a variety of different
surfaces carpet, a smooth floor, etc. - What would happen to the motion of the ball if
all friction were eliminated?
14Newtons 1st Law of Motion
- Galileo theorized that an object sliding on a
smooth surface would slide forever in the absence
of an applied force. - In 1687, Newton further developed this idea, and
it is now known as his first law of motion.
15Newtons 1st Law of Motion
- An object at rest remains at rest, and an object
in motion will continue in motion with constant
velocity (constant speed in a straight line)
unless the object experiences a net external
force. - The tendency of an object not to accelerate is
called inertia. (Mass is a measurement of an
objects inertia.)
16Newtons 1st Law of Motion
- The first law of motion is also referred to as
the Law of Inertia. - Unless a force acts on an object and causes a
change in velocity (acceleration), the object
will preserve its current state of motion.
17Newtons 1st Law of Motion
- The acceleration an object experiences is the
result of the net external force. - The net external force is the vector sum of all
forces acting on an object. - The net external force is written as Fnet or SF.
18Newtons 1st Law of Motion
- When SF zero, then the object is in
equilibrium. - Note that being at rest is a special case of
constant velocity. - Newtons 1st Law identifies the net force as
something that disturbs equilibrium. - So, the net force changes the velocity of an
object, and the change in velocity (acceleration)
is the result of a net force on the object.
19Newtons 1st Law of Motion
20Newtons 2nd Law of Motion
- How does a known force affect the motion of an
object? - Imagine pushing a car on a flat level surface.
- Compare the speed of the car if only one person
is pushing versus multiple people. Which case
provides the greater increase in speed?
21Newtons 2nd Law of Motion
- The acceleration of an object is directly
proportional to the net external force acting on
it. - Does mass affect acceleration?
- Objects with greater mass have greater inertia,
or tendency to maintain its current state of
motion.
22Newtons 2nd Law of Motion
- Newton summarized the relationship between mass,
acceleration, and the net force acting on an
object. - SF ma
- Recall the acceleration and force are both vector
quantities and the force in this equation is the
vector sum of all forces acting on the object.
23Newtons 2nd Law of Motion
- Thus, the acceleration of an object is directly
proportional to the net force and inversely
proportional to the mass. - This is known as Newtons 2nd Law of Motion.
24Newtons 2nd Law of Motion
- The direction of the acceleration is in the same
direction as the net force acting on the object.
25Newtons 2nd Law of Motion
- Newtons 2nd Law of Motion identifies the cause
of a change in velocity and the resulting
displacement, and is sometimes called the law of
nature. - Newton believed that this law held true for all
motions. - However, scientists now know that Newtons 2nd
Law does not hold true for objects that approach
the speed of light or for atomic particles. - But, this law does govern the motion of our
everyday lives 300 years later.
26Newtons 2nd Law of Motion
- Problem Solving Skills
- Draw a free-body diagram and label all the forces
acting on the object. - Break the equation SFma into components.
- SFxmax
- SFymay
27Applications Newtons 2nd Law
- There are several types of forces that affect the
motion of an object. - Table 6-2 on page 123 lists some common forces
and the standard notation for each force. - Recall that forces are labeled using F and a
subscript denoting the type of force.
28Applications Newtons 2nd Law
- Aristotle versus Galileo on falling objects
- While there is no evidence that Galileo dropped
two balls from the Leaning Tower of Pisa, he did
propose a theory on falling objects. - Using Newtons 2nd Law and neglecting air
resistance, there are no contact forces acting on
falling objects. - So what is the force causing the object to
accelerate downward?
29Applications Newtons 2nd Law
- Recall that falling objects accelerate at a
constant rate equal to 9.8 m/s2 (g). - Using Newtons 2nd Law, the force causing the
object to accelerate is the weight force. (Fg) - Fg mg
- An objects weight is equal to its mass times the
acceleration it would have if it were freely
falling.
30Applications Newtons 2nd Law
- This is true on Earth and all planets, although
the value of g is different for different
planets. - Mass does not change.
- What then is weight, and what do scales measure?
31Applications Newtons 2nd Law
- When you step on a bathroom scale, you exert a
downward force on a spring, and the spring exerts
an upward force on you. - Because you are not accelerating, SF 0.
- Therefore, the magnitude of the force exerted by
the spring on you is equal to your weight, not
your mass. - If you were on a different planet, the
compression of the spring would be different, and
your weight would be different.
32Applications Newtons 2nd Law
- What happens to weight though if you are
accelerating? - Imagine weighing yourself in an elevator that is
accelerating downward. - Would your weight on the scale increase or
decrease? - You would experience weightlessness.
33Applications Newtons 2nd Law
- The weight you read on the scale is the apparent
weight. - Weightlessness does not mean that your weight is
zero, but that your apparent weight is zero. - All objects have weight and experience a force
directed downward caused by the acceleration due
to gravity.
34Applications Newtons 2nd Law
- Friction is often minimized in problem solving,
but in the real world friction is everywhere. - Friction allows motion to start and stop.
- Imagine walking on an ice rink, riding a bike, or
using a pencil.
35Applications Newtons 2nd Law
- Imagine pushing a car from rest on a level
surface. - Newtons 2nd Law states the car should move
unless there is another force acting upon it. - The resistive force that keeps the car from
moving is the static friction force. (Fs)
36Applications Newtons 2nd Law
- As long as an object does not move, the force of
static friction is always equal and opposite in
direction to the component of the applied force
in the horizontal direction. - But, we know that if we keep pushing on the car,
it will eventually move. - So, the force of static friction has a maximum.
37Applications Newtons 2nd Law
- When the applied force is a great as it can be
without causing the object to move, the force of
static friction reaches its maximum value. (Fs,
max) - When the applied force exceeds Fs, max the object
will begin to move. - But, experience again tells us that once we
remove the applied force, the car will eventually
come to a stop. - So, a retarding force is still acting upon the
car.
38Applications Newtons 2nd Law
- The retarding force, or force opposing the
direction of motion, is known as the kinetic
friction force. (Fk) - The kinetic friction force is the force exerted
on one surface by the other when the surfaces are
in relative motion.
39Applications Newtons 2nd Law
- Although frictional forces are complicated, a
simplified model can be used to find solutions
close to those found by experiments. - Recall that friction depends on the type of
surfaces in contact, the speed of their relative
motion, and the surface area of contact. - This model ignores surface area and speed, and
deals only with the surfaces in contact.
40Applications Newtons 2nd Law
- The magnitude of the force of friction is
proportional to the magnitude of the force
pushing one surface against the other. - This is the normal force. (FN)
- For objects on a flat level surface,
- FN Fg mg
- The normal force is always perpendicular to the
area of contact but is not always opposite in
direction to the force of gravity.
41Applications Newtons 2nd Law
- Fk µkFN
- Remember that the kinetic force of friction and
the normal force are vectors. - µk is the coefficient of kinetic friction and
depends on the composition of the surfaces in
contact. - Table 6-3 on page 131 lists typical coefficients
of frictions for various surfaces in contact.
42Applications Newtons 2nd Law
- Fs µsFN
- Thus, the force of static friction is greater
than the force of kinetic friction. - It is easier to keep an object in motion, than it
is to begin its motion.
43Newtons 3rd Law
- Have you hear the phrase, For every action,
there is an equal and opposite reaction? - What exactly is an action, reaction, and why are
they equal? - If a car hits a brick wall, we know the car
exerts a force on the wall. Does the wall exert a
force on the car?
44Newtons 3rd Law
- Yes the wall exerts a force on the car as well.
- The force of the car on the wall (Fcar on wall)
and the force of the wall on the car (F wall on
car) are sometimes called action-reaction pairs. - These forces are not a cause and effect pair.
- They either exist together or not at all.
45Newtons 3rd Law
- Newton theorized that forces always exist in
pairs, and formulated his third law of motion. - According to the third law of motion, an
interaction pair is two forces that are in
opposite directions and have equal magnitude.
46Newtons 3rd Law
- Action-Reaction pairs act on different objects.
- Recall the car hitting the wall.
- One force acts on the car, and the other force
acts on the wall. - Field forces also exist in pairs.
47References
- Physics. Holt, Rinehart, and Winston, 2002
- Physics Principles and Problems. Glencoe, 2002