Chapter 3: Work, Energy, and Momentum Flashcards

1
Q

Energy

A

A property or characteristic of a system to do work / make something happen

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2
Q

Kinetic Energy

A

The energy of motion

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3
Q

Objects with mass and some form of velocity will have:

A

Kinetic Energy

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4
Q

Kinetic Energy Equation

A

KE = ½mv2

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5
Q

The SI Unit for Kinetic Energy is:

A

Joules (J)

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6
Q

If velocity doubles, kinetic energy will:

A

quadruple (assuming the mass is constant)

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7
Q

Potential Energy

A

An object that has mass and the potential to do something.

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8
Q

Potential Energy Equation

A

PE = mgh

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9
Q

Total Mechanical Energy is:

A

The sum of an object’s potential and kinetic energies.

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10
Q

Total Mechanical Energy (E) Equation

A

E = PE + KE

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11
Q

The First Law of Thermodynamics states:

A

Energy is never created or destroyed. It is merely transferred from one system to another.

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12
Q

When the work done by nonconservative forces is zero (when there are no nonconservative forces acting on the system), the total mechanical energy of the system:

A

remains constant. (E = PE + KE = Constant)

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13
Q

When nonconservative forces such as friction and air resistance are present, total mechanical energy:

A

is not conserved

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14
Q

Work Done by Nonconservative Forces (W’) Equation

A

W’ = ΔE = ΔKE + ΔPE

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15
Q

The work done by nonconservative forces such as air resistance and friction is exactly equal to:

A

the amount of energy ‘lost’ from the system. NOTE: the energy was not ‘lost’, it was just transferred out of the system and into another.

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16
Q

Mechanical Energy is conserved when:

A

No nonconservative forces (friction, air resistance, etc. are present).

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17
Q

Work is:

A

a process in which energy is transferred from one system to another when something exerts forces on or against something else.

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18
Q

Work (W) Equation

A

W = FdcosΘ

(F = force applied; d = displacement through which the force is applied; Θ = the angle between the applied force vector and the displacement vector)

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19
Q

In the Work equation, Θ is:

A

the angle between the displacement and force vectors

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20
Q

Power

A

The rate at which energy is transferred from one system to another.

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21
Q

Power (P) Equation

A

P = W / t (where W = work and t = time)

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22
Q

SI Unit of Power

A

Watts (W)

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23
Q

The Work-Energy Theorem states:

A

the net work done on or by an object will result in an equal change in the object’s kinetic energy.

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24
Q

Work-Energy Theorem Equation

A

Wnet = ΔK = Kf - Ki

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25
Momentum is defined as:
a quality of objects in motion. It is defined as the product of an object's mass times its velocity. Therefore, it is a vector quantity.
26
Momentum (p) Equation
p = mv (where m = mass and v = velocity)
27
For two or more objects, the total momentum is equal to:
the vector sum of the individual momenta
28
Inertia
the tendency of objects to resist changes in their motion and momentum
29
Impulse is defined as:
the change in an object's momentum. It is a vector quantity.
30
For a constant force applied through a period of time, impulse and momentum are related by this equation:
I = FΔt = Δp = mvf - mvi (where I = impulse, t = time; p = momentum; m = mass; v = velocity)
31
The longer the time of change in momentum (Impulse), the smaller the:
Force necessary to achieve the impulse. (Example - Crush zones in cars. The longer amount of time the car crushes, the smaller the force felt on the occupancy zone by the change in momentum - the change in momentum occurs over a longer period of time, and thus the force felt is smaller)
32
Conservation of momentum means that:
the momentum after a collision is the same as the momentum before the collision.
33
Conservation of momentum occurs when:
No nonconservative forces (friction, air resistance, etc. are present).
34
Conservation of Momentum Equation for elastic and inelastic collisions
mavai + mbvbi = mavaf + mbvbf
35
The three types of collisions for which momentum is conserved:
Completely Elestic Collisions; Inelastic Collisions; Completely Inelastic Collisions
36
Completely Elastic Collisions occur when:
Two or more objects collide in such a way that both kinetic energy and momentum are conserved. They do not stick together.
37
Conservation of Kinetic Energy in a Completely Elastic Collision Equation
½mavai2 + ½mbvbi2 = ½mavaf2 + ½mbvbf2
38
In completely elastic collisions:
kinetic energy and momentum are BOTH conserved
39
Inelastic Collisions occur when:
a collision results in the decrease of kinetic energy of the system through the production of sound, heat, light, etc.
40
In inelastic collisions:
momentum is conserved, but the final kinetic energy is LESS THAN the initial kinetic energy
41
Inelastic Collision Equation
½mavai2 + ½mbvbi2 \> ½mavaf2 + ½mbvbf2
42
Completely Inelastic Collisions occurs when:
objects collide and stick together rather than bouncing off each other and moving apart.
43
In completely inelastic collisions:
momentum is conserved, but the final kinetic energy is LESS THAN the initial kinetic energy
44
Conservation of Momentum Equation for completely inelastic collisions
mavai + mbvbi = (ma + mb)(vf)
45
In completely elastic collisions, what is conserved?
KE and momentum
46
In completely inelastic collisions, what is conserved?
momentum; KE is lost
47
In inelastic collisions, what is conserved?
momentum; KE is lost
48
Mechanical Advantage
Any device (such as an inclined plane) that allows for work to be accomplished through a reduced applied force is said to provide mechanical advantage.
49
Mechanical Advantage Equation
Mechanical Advantage = Fout / Fin (Fout = the force exerted on an object by a simple machine; Fin = the force actually applied on the simple machine)
50
Mechanical Advantage is the ratio of:
the force exerted on an object by a simple machine (Fout) to the force actually applied on the simple machine (Fin)
51
Mechanical Advantage comes at the expense of:
increasing the distance over which the work is done
52
Mechanical Advantage: load
the load is the weight of an object (mg) in a mechanical advantage situation
53
Mechanical Advantage: effort
the force applied to the simple machine in mechanical advantage
54
Mechanical Advantage: Load Distance
the distance an object is moved by a simple machine in mechanical advantage
55
Mechanical Advantage: Effort Distance
In a pulley system, the length of rope that must be pulled in order to move the object the load distance. Effort distance is longer than load distance.
56
Efficiency of a Simple Machine Equation
Efficiency = Wout / Win = (load)(load distance) / (effort)(effort distance)
57
Efficiencies are expressed as:
Percentages
58
The efficiency of a machine gives a measure of:
the amount of work put into the system that "comes out" as useful work
59
The six devices considered to be classic simple machines:
inclined planes, wedges, pulleys, axle and wheel, lever, and screws
60
In an idealized pulley (one that is massless and frictionless), the work put into the system is equal to:
the work that comes out of the system. Thus, the pulley has a 100% efficiency.
61
Center of Mass
The point that acts as if the entire mass was concentrated at that point.
62
Center of Mass Equation
X = m1x1 + m2x2 + m3x3 + .. / m1 + m2 + m3 .. (where m1, m2, and m3 are the masses of three different objects and x1, x2, and x3 are there positions along the x-axis)
63
Center of Gravity Equation
X = w1x1 + w2x2 + w3x3 + .. / w1 + w2 + w3 .. (where w1, w2, and w3 are the weights of three different objects and x1, x2, and x3 are there positions along the x-axis)