Physics 1111: Conservation of Energy Study Notes

0.0(0)
studied byStudied by 0 people
0.0(0)
linked notesView linked note
full-widthCall with Kai
GameKnowt Play
New
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
Card Sorting

1/30

encourage image

There's no tags or description

Looks like no tags are added yet.

Study Analytics
Name
Mastery
Learn
Test
Matching
Spaced

No study sessions yet.

31 Terms

1
New cards

Work Equation

$W = extbf{F} ullet extbf{A} = F A ext{ cos}( heta)$

2
New cards

Total Work Sum Equation

$W*{ ext{total}} = extstyle extsum W$

3
New cards

Total Work Net Force Equation

$W{ ext{total}} = extbf{F}{ ext{total}} ullet extbf{A} ext{ cos}( heta)$

4
New cards

Kinetic Energy Equation

$K = rac{1}{2}mv^2$

5
New cards

Work-Kinetic Energy Theorem Equation

$W{ ext{total}} = riangle K = rac{1}{2}mvf^2 - rac{1}{2}mv_i^2$

6
New cards

Work Done by Springs Equation

$W{ ext{sp}} = - rac{1}{2}k xf^2 + rac{1}{2}k x_i^2$

7
New cards

Potential Energy Change Equation

$ riangle U = -W_{ ext{cons}}$

8
New cards

Work Done by Gravity Equation

$W_g = -mg riangle y$

9
New cards

Gravitational Potential Energy Equation

$U_g = mg riangle y$

10
New cards

Spring Potential Energy Equation

$U_s = rac{1}{2}kx^2$

11
New cards

Total Mechanical Energy Equation

$E_{ ext{mech}} = K + U$

12
New cards

Change in Mechanical Energy Equation

$ riangle E_{ ext{mech}} = riangle K + riangle U = 0$

13
New cards

Conservation of Mechanical Energy Equation

$K{ ext{before}} + U{ ext{before}} = K{ ext{after}} + U{ ext{after}}$

14
New cards

Work (W)

The net effect of a force $ \mathbf{F} $ on an object as it undergoes a displacement $ \mathbf{A} $.

15
New cards

How is work defined for a constant force?

Work is defined as $W = \mathbf{F} \cdot \mathbf{A} = F A \cos(\theta)$, where $ \mathbf{F} $ is the magnitude of the force, $ \mathbf{A} $ is the magnitude of the displacement, and $ \theta $ is the angle between $ \mathbf{F} $ and $ \mathbf{A} $.

16
New cards

How is total work calculated for multiple forces?

The total work is the sum of the work done by individual forces ($ \displaystyle \sum W$) or can be expressed using the net force: $W{\text{total}} = \mathbf{F}{\text{total}} \cdot \mathbf{A} \cos(\theta)$.

17
New cards

Kinetic Energy (K)

The energy of moving objects. It is a scalar quantity, calculated as $K = \frac{1}{2}mv^2$ where $m$ is mass and $v$ is speed.

18
New cards

Work-Kinetic Energy Theorem

States that when forces act on an object that displaces it, the net work done results in a change in kinetic energy: $W_{\text{total}} = \Delta K$.

19
New cards

How is work done by a spring determined?

Work done by a spring is determined solely by the starting and ending positions (spring lengths) and is path-independent. Springs represent a conservative force.

20
New cards

Conservative Force

A force is considered conservative if the work done depends only on initial and final positions, independent of the path taken.

21
New cards

Potential Energy (PE)

For conservative forces, it is possible to define a potential energy such that the change in potential energy equals the negative work done by the force: $ \Delta U = -W_{\text{cons}} $.

22
New cards

How is work done by gravity (Wg) defined?

The work done by gravity is defined by the height difference between starting and ending points: $W_g = -mg \Delta y$. It is positive when moving downward and negative when moving upward, and is independent of the path taken.

23
New cards

Gravitational Potential Energy (Ug)

A type of potential energy defined as $U_g = mg \Delta y$, where $m$ is mass, $g$ is the acceleration due to gravity, and $ \Delta y $ is the change in height. A reference point where $U=0$ can be chosen arbitrarily.

24
New cards

Spring Potential Energy (Us)

A type of potential energy defined as $U_s = \frac{1}{2}kx^2$, where $k$ is the spring constant and $x$ is the displacement from equilibrium.

25
New cards

Total Mechanical Energy (Emech)

The sum of kinetic energy and potential energy ($E_{\text{mech}} = K + U$). This includes gravitational potential energy ($Ug$) and spring potential energy ($Us$). It remains constant if only conservative forces do work.

26
New cards

Conservation of Mechanical Energy

States that if only conservative forces do work, the total mechanical energy of a system remains constant ($ \Delta E{\text{mech}} = 0$). This means $K{\text{before}} + U{\text{before}} = K{\text{after}} + U_{\text{after}} $.

27
New cards

What is the first step in solving problems using energy conservation?

Identify the system by drawing a picture.

28
New cards

What must be identified to solve problems using energy conservation?

The object(s) in motion and the forces acting in the system.

29
New cards

How can one determine if forces are conservative?

By observing if the work done reveals changes in potential energy, as $ \Delta U = -W $.

30
New cards

What are the mechanical energy conservation conditions?

$ \Delta E_{\text{mech}} = 0 = \Delta K + \Delta U $.

31
New cards

What is the final step in solving problems using energy conservation?

Confirm that the changes in kinetic energy align with expectations (validation step).