Work, Energy, and Power Flashcards

1
Q

Energy

A

Ability to do work

  • Different forms of energy as there are different types of forces
    • Kinetic energy (E.g. train)
    • Gravitational energy (E.g. meteor)
    • Elastic energy (E.g. rubber band)
    • Thermal energy (E.g. oven)
    • Radiant energy (E.g. sunlight)
    • Electrical energy (E.g. lamp)
    • Nuclear energy (nuclear power plants)
    • Mass energy (E= mc2)
  • Energy can come into a system or leave it via various interactions that produce changes
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
2
Q

Force, Work, Energy

A
  • Force acts as agent of change
  • Energy acts as measure of change
  • Work acts the way of transferring energy from one system to another
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
3
Q

Law of Conservation of Energy

A

Total amount of energy in a given process will stay constant- it will be conserved

  • Equivalent to the first law of thermodynamics
  • Energy cannot be created or destroyed; it can only be transferred (from one system to another) or transformed (from one form to another)
    • E.G. electrical energy can be converted into light and heat (lightbulb)
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
4
Q

Work

A

The application of force over a distance and the resulting change in energy of the system give rise to the concept of work

  • If a constant foce F acts over a distance d, and F is parallel to d, then the work done by F is the product of force and distance
    • If a constant force F acts over a distance d, and θ is the angle between F and d, then the work done by F is the product of the component of force in the direction of the motion and the distance
      • W= Fdcosθ
        • W= Fdcosθ only works when the force does not change as the object moves
  • Although work depends on two vectors (F and d, where d points in the direction of the motion), work itself is not a vector
    • Work is a scalar quantitiy
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
5
Q

Antiparallel

A

Angle of 180o

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
6
Q

Values of Work

A
  • Work may be positive, negative, or zero
  • If θ is less than 90o, then the work is positive
    • cosθ is positive in this case
  • If θ= 90o then work is zero
    • cos90o= 0
  • If θ is greater than 90o, then the work is negative
    • cosθ is negative in this case
  • If a force helps the motion, then the work done by the force is positive
    • If the force opposes the motion then the work done by the force is negative
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
7
Q

Breaking force into components F and F||

A

F is the component perpendicular to the direction of the motion

F|| is the component in the direction of the motion (or opposite if it is negative)

W= F||d

  • Used for situations where θ is something other than 0o, 90o, or 190o
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
8
Q

Work Done by Variable Force

A
  • If force remains constant over the distance through which it acts, then the work done by the force is the just the product of force and distance
    • If force doesn’t remain constant, then the work done by the force can be calculated through integrated area
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
9
Q

Kinetic Energy

A

The energy an object posseses by virtue of its motion is therefore defined as 1/2mv2 and is called kinetic energy: K= 1/2mv2

  • Force acting on an object from rest causing it to acclerate, work done by force: W= 1/2mv2
    • The work done on the object has transferred energy to it, in the amount 1/2mv2
  • Stopping an object means changing its kinetic energy to 0
  • Kinetic ernegy, like work, is a scalar quantitiy
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
10
Q

The Work-Energy Theorem

A

The total work done on an object- the work done by the net force- is equal to the object’s change in kinetic energy

Wtotal= ΔK

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
11
Q

Kinematics Vs. Work-Kinetic Energy

A

For objects moving in a straight line with a constant force, you can use the work-kinetic energy theorem or kinematic equations for problems where time is not involved

How well did you know this?
1
Not at all
2
3
4
5
Perfectly
12
Q

Potential Energy

A

Independent of motion and arises from the object’s position; energy an object or system has by virtue of its position

  • Sybmolized by U or PE
  • Work was done to put an object at its given position (E.g. ball placed at a top of a table)
    • Work is a means of transferring energy, energy was stored and can be retrieved as kinetic energy
  • When an object falls, gravity does positive work, giving the object kinetic energy
  • Kinetic energy comes from a “storehouse” of energy, this energy is called potential energy
  • As there are different types of forces there are different types of potential energy
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
13
Q

Gravitational Potential Energy

A

Energy stored by virtue of an object’s position in a gravitational field

  • Symbolized by Ugrav
  • Energy can be converted to kinetic energy as gravity pulls object to ground/floor
  • Wby gravity= -mgh
  • ΔUgrav= -Wby gravity
  • E.G. a ball resting on a tabletop, gravity “did work” of -mgh to place ball on tabletop storing potential energy, as ball falls to the floor the change of potential energy as energy is converted to kinetic energy
  • Increase in an object’s gravitational potential energy as a raised height can be found by
    • ΔUgrav= mgh
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
14
Q

Conservative Force

A

Gravity is said to be a conservative force

  • Work done by gravity as the object is raised does not depend on the path taken by the object, the ball could be lifted straight upward or a curved path, it will make no difference
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
15
Q

Gravitational Potential Energy General Equation

A

Wby grav= GMm(1/r2 - 1/r1)

since ΔUgrav= -Wby grav

U2 - U1= -GMm(1/r2 - 1/r1)

U= 0 at reference level as r2 approaches infinity

  • U= -GMm/r
    • According to this equation, the gravitational potential energy is always negative, meaning energy has to be added to bring an object (mass m) bound to the gravitational field of M to a point very far from M, at which U= 0
How well did you know this?
1
Not at all
2
3
4
5
Perfectly
16
Q

Mechanical Energy

A

The mechanical energy, E, is the sum of the kinetic energy, K, and the potential energy, U

E= K + U

17
Q

Conservation of Mechanical Energy

A

Assuming no nonconservative forces (E.G. friction) act on an object or a system as it undergoes some change, mechanical energy is conserved

  • The intial mechanical energy, Ei, is equal to the final mechanical energy Ef
    • Ki + Ui= Kf + Uf
  • Shorthand conservation of mechanical energy formula:
    • v= Radical(2gh)
18
Q

Escape Speed

A

Speed needed in order to escape Earth’s gravitational field

19
Q

Shorthand Formula For When a Nonconservative Force Does Work

A

Wtotal= ΔK

  • Work done by gravity replaces the change in potential energy
20
Q

Power

A

Rate at which work is done (or energy is transferred, which is the same thing)

  • Power= Work/time
    • P= W/t
  • Unit of power is joule per second (J/s)
    • Renamed the watt and symbolized W (not to be confused with the symbol for work, W)
    • One Watt is 1 joule per second: 1 W= 1 J/s
  • E.G. two machines doing the same amount of total work, but one doing the work in less time is considered more powerful