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Topic 2: Mechanics: 2.1 - Motion Distance and Displacement

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Topic 2: Mechanics

See the guide for this topic.


2.1 – Motion

 Distance and displacement


Distance Displacement
Scalar Vector
A scalar quantity which measures how far A vector quantity defined by the length and
two locations are apart from each other direction of the line segment joining the
along a certain path. initial and final positions of an object.

 Speed and velocity


Speed Velocity
Scalar Vector
Rate of change of distance to time. Rate of change of displacement to time.
Velocity is a measure dependent on the motion of the observer. The relative velocity
of A to B is equal to the vector subtraction of the velocity of B from the velocity of A.

 Acceleration
Acceleration
Vector
Rate of change of velocity
Acceleration due to gravity of any free-falling object is given by g=9.81m/s^2. This
value does not depend on the mass of the object.
Take note that acceleration is a vector and thus has a direction. If we assume the
upwards direction to be positive, the acceleration due to gravity would have a
negative value of g=-9.81m/s^2.

 Graphs describing motion

Displacement-time graph

The slope gradient indicates the velocity.

Straight lines imply constant velocity.

Velocity-time graph
The slope gradient indicates the acceleration.

Straight slanted lines imply constant acceleration or deceleration.

The area under the lines indicates the change in displacement.

Acceleration-time graph

Horizontal lines imply constant acceleration.


The area under the lines indicates the change in velocity.

 Equations of motion for uniform acceleration


u = initial v = final
s = displacement velocity velocity a = acceleration t = time taken
If acceleration is constant (uniform), the following equations can be used

 Projectile motion
An object is said to undergo projectile motion when it follows a curved path due to
the influence of gravity.
If we assume air resistance to be negligible in a projectile motion:

 The horizontal component of velocity is constant


 The vertical component of velocity accelerates downwards at 9.81m/s^2
 The projectile reaches its maximum height when its vertical velocity is zero
 The trajectory is symmetric
The presence of air resistance changes the trajectory of the projectile by the following

 The maximum height of the projectile is lower


 The range of the projectile is shorter
 The trajectory is not symmetric

 Fluid resistance and terminal speed


Air resistance limits the maximum velocity an object could attain from free-falling.
For example:

 If you jump out of a plane and undergo free-falling, you will feel an upward
force exerted on you by the surrounding air due to air resistance.
 As you fall faster and faster due to gravity, this upward force exerted by air
becomes greater and greater until it balances your weight. At this point, the net
force acting on you becomes zero, and you no longer accelerate.
 This specific velocity at which you stop accelerating during a free-fall is called
the terminal velocity.

2.2 – Forces

 Objects as point particles


Forces change the velocity or shape of objects.

The unit of force is newton (N).

Objects are represented as a point mass to enable the representation for forces as
arrows in free-body diagrams.

 Free-body diagrams
On a free body diagram, forces acting on an object are represented as arrows which
stem from a point mass.

The length and direction of the arrows corresponds to the magnitude and the direction
of the forces acting on the body of interest.
Determining the resultant force
1. Resolve all acting forces into horizontal and vertical components
2. Add up the horizontal components
3. Add up the vertical components
4. Combine the sum of horizontal components and the sum of vertical components

 Translational equilibrium
A body is said to be in translational equilibrium if it the net force acting on the body is
zero. This means the body is either at rest or travels at constant velocity. For example:

 Mass hanging at rest


 Elevator moving upwards at constant velocity
 Parachutist reaching terminal velocity
 Newton’s laws of motion
Newton’s First Law (Law of Inertia) states that a body remains at rest or travels with
constant speed along a straight line unless acted upon by an external force. (Net force
= 0)

Newton’s Second Law states that net force is directly proportional to acceleration and
to mass. (F=ma)
Newton’s Third Law states that if a body A exerts a force on body B, then body B
exerts a force of the same magnitude but in the opposite direction of body A.

This pair of forces is called an action-reaction pair, which must act on two different
bodies.

 Solid friction
Friction is a non conservative force which opposes motion. If there is no motion, then
there will be no force caused by friction.

For two solid surfaces moving over each other, the friction will be affected by the
nature (roughness etc) of the two surfaces. However, the surface area and velocity of
the object does not affect the friction.

There are also two types of friction for solid surfaces: static friction and kinetic
friction. Static friction is that which stops objects from beginning to move. Kinetic
friction is that which slows objects down when they are moving. Static friction is
always larger than kinetic friction.

These two types of friction are defined individually by their constants µs and
µk respectively.

The forces of friction are also dependent on the normal force the surface is applying,
leading to Friction force (static) =< µs * Normal force for objects that are not moving
and Friction force (static) = µs * Normal force for objects that are moving.

2.3 – Work, energy and power

 Kinetic energy
Kinetic energy (KE) is the energy of a body due to its motion and is given by the
equation

 Gravitational potential energy


The gravitational potential energy (GPE) of an object changes with its height and is
given by the equation

 Elastic potential energy


Elastic energy is potential energy stored as a result of the deformation of an elastic
object such as the stretching of a spring and is given by the equation
 Work done as energy transfer
Work done measures the transfer of energy due to a force and is a scalar quantity.

The work done W by a force F on an object is given by the equation


In a force-displacement graph, work done is the area under the curve.

 Power as rate of energy transfer


Power (P) is the work done or the energy output per time given by the equation:

For constant force acting on an object with constant velocity, the power is given by
the equation: P=Fv.
 Principle of conservation of energy
Energy can neither be created nor destroyed; it can only be changed from one form to
another. For example:

 An electrical heater transforms electrical energy to thermal energy.


 A falling object transforms potential energy to kinetic energy.
Total energy of an isolated body remains constant. In other words, ΔKE+ΔPE=0

 Efficiency
Efficiency is the ratio of useful energy output to energy input as a percentage given by
the equation

2.4 – Momentum and impulse

 Newton’s second law expressed in terms of rate


of change of momentum
The linear momentum (p) is given by the equation
The linear momentum (p) is a vector with the same direction as the velocity of an
object.

The change of momentum of an object is called impulse.

Rearranging the formula describing Newton’s second law results in the following
expression

 Impulse and force–time graphs


Impulse is given by the area of a force-time graph.

 Conservation of linear momentum


The law of conservation of linear momentum states that the sum of initial momentum
is equal to the sum of final momentum in a closed system and can be given by the
equation
 Elastic collisions, inelastic collisions and
explosions
Type Total momentum Total kinetic energy
Elastic Conserved Conserved
Inelastic Conserved Not conserved
Explosion Conserved Not conserved

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