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Transcript
Chapter 4
Forces in One Dimension
Classical Mechanics


Describes the relationship between the
motion of objects in our everyday world
and the forces acting on them
Conditions when Classical Mechanics
does not apply


very tiny objects (< atomic sizes)
objects moving near the speed of light
Forces



Usually think of a force as a push or
pull
Vector quantity
May be a contact force or a field
force


Contact forces result from physical contact
between two objects
Field forces act between disconnected
objects

Also called “action at a distance”
Force


A force is a push or pull. An
object at rest needs a force
to get it moving; a moving
object needs a force to
change its velocity.
The magnitude of a force
can be measured using a
spring scale.
Contact and Field Forces
Fundamental Forces

Types





Strong nuclear force
Electromagnetic force
Weak nuclear force
Gravity
Characteristics



All field forces
Listed in order of decreasing strength
Only gravity and electromagnetic in
mechanics
Electromagnetic Forces

Only forces that attract and repel

Electric Forces




Act between charged objects particles
Like charges repel
Opposite charges attract
Magnetic Forces


Act on certain metals
North and south poles
Strong Nuclear Force

Acts only on the protons and neutrons
in the nucleus.


Only acts at very short distances


Holds them together
Diameter of a proton
100x stronger than electromagnetic
force
Weak Nuclear Force


Not as strong as the strong nuclear
force
Responsible for radioactive decay
Gravitational Force

Weakest of the universal forces

Attractive force between two masses.

Proportional to mass

Decreases rapidly with distance

But still effective over long distances.
Newton’s First Law

An object moves with a velocity
that is constant in magnitude and
direction, unless acted on by a
nonzero net force


The net force is defined as the vector
sum of all the external forces exerted
on the object
In English please…..
Newton’s First Law

Every object continues in its state
of rest, or of uniform velocity in a
straight line, as long as no net
force acts on it.
External and Internal
Forces

External force


Any force that results from the
interaction between the object and its
environment
Internal forces


Forces that originate within the object
itself
They cannot change the object’s
velocity
Inertia


Newton’s first law is often called
the law of inertia.
Inertia is the tendency of an object
to continue in its original motion
Mass



Mass is the measure of inertia of
an object. In the SI system, mass
is measured in kilograms.
Mass is not weight:
Mass is a property of an object.
Weight is the force exerted on that
object by gravity.
Mass



If you go to the moon, whose
gravitational acceleration is about
1/6 g, you will weigh much less.
Your mass, however, will be the
same.
Scalar quantity
SI units are kg
Newton’s Second Law

Newton’s Second Law
of Motion

Acceleration of an object is always in
the same direction as the net force.
150N
a=ΣF/m
F = 150-50 =
100N
m = 50kg
a = 100/50
a = 2m/s2
50kg
50N
Units of Force

SI unit of force is a Newton (N)
kg m
1N  1 2
s

US Customary unit of force is a
pound (lb)

1 N = 0.225 lb
Sir Isaac Newton





1642 – 1727
Formulated basic
concepts and laws
of mechanics
Universal
Gravitation
Calculus
Light and optics
Weight

The magnitude of the gravitational
force acting on an object of mass
m near the Earth’s surface is called
the weight w of the object

w = m g is a special case of Newton’s
Second Law


g is the acceleration due to gravity
g can also be found from the Law
of Universal Gravitation
More about weight

Weight is not an inherent property
of an object


mass is an inherent property
Weight depends upon location
Newton’s Third Law

If object 1 and object 2 interact,
the force exerted by object 1 on
object 2 is equal in magnitude but
opposite in direction to the force
exerted by object 2 on object 1.
 F12  F21

Equivalent to saying a single isolated
force cannot exist
Newton’s Third Law of Motion


Helpful notation: the first subscript is the
object that the force is being exerted on; the
second is the source.
This need not be done indefinitely,
but is a good idea until you get
used to dealing with these forces.
Newton’s Third Law cont.

F12 may be called the
action force and F21
the reaction force


Actually, either force
can be the action or
the reaction force
The action and
reaction forces act
on different objects
Newton’s Third Law of
Motion

Action and Reaction forces
Newton’s Third Law of
Motion

Why don’t action/reaction
forces cancel each other?
Some Action-Reaction
Pairs

n and n '
n is the normal force,
the force the table
exerts on the TV
 n is always
perpendicular to the
surface
 n 'is the reaction – the
TV on the table
 n  n '

Applications of Newton’s
Laws

Assumptions

Objects behave as particles



can ignore rotational motion (for now)
Masses of strings or ropes are
negligible
Interested only in the forces acting
on the object

can neglect reaction forces
Free Body Diagram



Must identify all the forces acting
on the object of interest
Choose an appropriate coordinate
system
If the free body diagram is
incorrect, the solution will likely be
incorrect
Free Body Diagram,
Example

The force is the
tension acting on the
box


The tension is the same
at all points along the
rope
n and Fg are the
forces exerted by the
earth and the ground
Equilibrium


An object either at rest or moving
with a constant velocity is said to
be in equilibrium
The net force acting on the object
is zero (since the acceleration is
zero)
F  0