---
## Energy basics
##### *Energy transformations/transfers*
- Energy *transformations* **are changes of energy with a system from one form to another**.
- Energy *transfers* are different. They are the **exchange of energy between a system and its environment.**
- **Work** describes the process of transferring energy to or from a system to an environment through **mechanical motion** *(kinetic energy)*.
- **Heat** describes the process of transferring energy to or from a system via a **nonmechanical** means.
- Since work allows us to change the energy of a system we can relate the total energy of a system to the amount of work done on it with the following proportional relationship. *This is known as the work energy equation.*
$\newline$
$W=\Delta E=E_f-E_i\;\;\;\;\text{\color{grey}\small where}\;\;\;\;\Delta E=\sum\Delta E_{type}$
$\newline$
- *This equation illustrates why isolated systems have their energy conserved: without work, the total energy in a system cannot change.*
##### *Types of energy*
- **Kinetic energy** is the energy of motion. All objects that are moving are said to have some kinetic energy. The **heavier an object is and the faster it moves, the more kinetic energy it is said to have.**
- **Gravitational potential energy**, is *stored energy* that is associated with an object's **height above the ground.** The higher up an object is moved, the greater its gravitational potential energy.
- When an object with *gravitational potential energy* is released it will convert that energy **into kinetic energy** as it accelerates towards the ground.
- **Elastic potential energy** is the energy *stored* when a spring or other elastic object is **stretched out or compressed inwards past its equilibrium position.**
- When an object with elastic potential energy is released the potential energy will transform into **kinetic energy** as the spring/elastic object works to move it back towards the equilibrium position.
- **Thermal energy** is the sum of the **kinetic and potential energies** of all the molecules that make up an object. In other words, its a measure of **heat**, which is just itself, a type of energy.
- **Chemical energy** is the energy stored by the strong and weak nuclear forces between atoms. This energy can be released when bonds between these atoms **are broken/re-arranged**.
- **Nuclear energy** is the energy created due to the strong/weak nuclear forces that hold [[Electrons]] [[Protons]] and [[Neutrons]] together to form **atoms.** When these bonds are broken *(nuclear fission)* a huge amount of this *nuclear energy* is released.
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## Kinetic energy
- **Translational kinetic energy** is the energy associated with an object that is moving from one location to another. This kind of kinetic energy is denoted using the variable: $\small K$.
- If an object is moving at **a constant velocity its kinetic energy will also be constant**.
- Kinetic energy ==is always measured in units of joules $J$==
- **Rotational kinetic energy** is the energy associated with an object that is **rotating** around an axis that lies **within itself**. This kind of kinetic energy is denoted using the variables and subscript: $K_{rot}$
- Both rotational and translational kinetic energy **increase exponentially** as the velocity *(or angular velocity)* of their associated object increases.
$\text{Kinetic energy equations: }\;\;\Huge\boxed{\color{LightCyan}\large K=\frac{1}{2}mv^2\;\;\;\;\;\;K_{rot}=\frac{1}{2}I\omega^2}$
$\newline$
$\text{Change in kinetic energy: }\;\Delta K=\frac{1}{2}m\Big(v_{\small f}^2-v_{\small i}^2\Big)$
>[!tip]
>##### *Interesting fact:*
>- From these equations you should be able to see that the **overall kinetic energy of a *rolling object* will always be greater than that of a nonrotating object that is moving at the same speed**.
---
## Potential energy
- Potential energy is the term we use to describe the **energy that is stored in an object due to its position relative to other object within a system**. We call this kind of energy potential energy because it has the ***potential* to be converted into other forms of energy** when the object it is associated with is released and allowed to return to its ideal state.
- You can only gain potential energy through positive work. *Also* in order to store potential energy you need to continue exerting positive work on the system.
##### *Gravitational potential energy*
- Gravitational potential energy is the energy that is associated with the height of an object.
- ==Gravitational potential energy depends only on the height of an object and not on the path the object took to get to that position.== When the object is allowed to fall downwards, the potential energy is converted to kinetic energy. We denote gravitational potential energy using the variable: $\small U_g$
- Since it always takes some amount of force to change the gravitational potential energy of an object we can derive a very simple relationship between the gravitational potential energy of an object and the amount of work done on that object:
- ==Potential energy is always measured in units of joules $J$==
$\newline$
$\text{Change in gravitational PE: }\;\Huge\boxed{\large\color{LightCyan}\Delta U_g=mg\Delta y}$
$\color{darkgrey}-=================================-$
$\text{Relationship between gravitational PE and work: }\;(U_g)_f=(U_g)_i+W\;\;\;\text{-or-}\;\;\;\;\color{lightcyan}\Delta U_g=W$
$\text{}$
>[!quote]
>##### *Gravitational potential energy*
>![[gravitationalpotentialenergyvisual.png|850]]
##### *Elastic potential energy*
- Energy can also be stored in a *compressed* or *extended* spring as **elastic potential energy** which is denoted using the variable: $\small U_s$
- Elastic potential energy is gained when an object is moved **against the restoring force of a spring or *other elastic object***. When this object is released the spring will exert a restoring force on the object converting the potential energy to kinetic energy.
- The amount of elastic potential energy that is stored in a spring that is at some **stretched/compressed position is equal to the amount of work done to get the spring to that position**.
- ==Potential energy is always measured in units of joules $J$==
$\newline$
$\text{Change in elastic PE: }\;\;\Huge\boxed{\large\color{LightCyan}\Delta U_s=\frac{1}{2}k\cdot x^2}$
$\newline$
- Since it takes work to compress or stretch a spring we can also derive a very simple relationship between the change in the elastic potential energy of an object and the **work** done on that object:
$\newline$
$\text{Relationship between elastic PE and work: }\;\Delta U_s=W$
---
## Thermal energy
- Thermal energy is the sum of the individual **kinetic and potential energies of all the atoms/molecules that make up an object**. Colloquially, we often call this quantity temperature, or heat.
- *Note that thermal energy is note the **average** of the KE of the atoms that make up a substance, it is the **summation of their KE's***.
- Friction between two objects **always increases their thermal energy**. If there is friction between an object and a surface the greater the **displacement of that object along that surface** the greater the amount of thermal energy that will be created.
- Drag between an object and a medium also always increases the thermal energy of the object.
- ==Thermal energy is always measured in units of joules $J$==
$\newline$
$\text{Change in thermal energy due to friction: }\;\Huge\boxed{\color{LightCyan}\normalsize\Delta E_{th} = f_k\cdot\Delta x}$
$\text{Change in thermal energy due to drag: }\;\Huge\boxed{\color{LightCyan}\normalsize\Delta E_{th} = D\cdot\Delta x}$
$\newline$
---
## Conservation of energy
- Just like with [[Impulse|momentum]] energy is **a property that is conserved**. This means that the total energy within that system will **==never change, it will only ever transfer from one form to another== *(potential to thermal ...)*** Unlike with conservation of momentum **when using conservation of energy to perform calculations you can choose a non-isolated system** so long as you know the amount of work **done by or done on that system.**
- If gravity is involved in any situation you must remember to always include **the earth in your system**.
- To use the property of conservation of energy in our equations we just set the initial and final **energies equal to each other**. This allows us to solve for any unknown values. See the example below:
$\newline$
$\text{Conservation of energy: }\;\color{LightCyan}E_i=E_f$
$\color{darkgrey}-===================================-$
$\text{Example conservation of energy equation: }$
$K_f+U_f+\Delta E_{th}=K_i+U_i+W=\Huge\boxed{\color{LightCyan}\normalsize \frac{1}{2}mv_f^2+mgy_f+\Delta E_{th}=\frac{1}{2}mv_i^2+mgy_i+W}$
$\newline$
- The **total energy** of a system is the sum of all the different types of energies within that system. If the system is isolated *(meaning that it does not interact with any outside objects/forces)* this value should **never change**. ==Therefore, the total energy of an isolated system is always conserved==.
- The heat transfer $\small Q$ and the work done $\small W$ must be equal to zero for a system to be **truly isolated**.
- Since energy can only transfer **in/out of a system through work or heat transfer we can create the following equation** that relates the change in energy *(of a system)* and the work/heat transfer done on a system.
- This equation shows that in isolated systems *(that have 0 work done on them and 0 heat transfer)* also have 0 change in energy.
$\text{Change of energy equation: }\;\Huge\boxed{\color{LightCyan}\large\Delta E=W+Q}$
$\newline$
>[!quote]
>##### *Conservation of energy visual*
>![[conservation of energy.png|850]]
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