feat: archive electricity

Resources/dev/tmux.md

@@ -0,0 +1,5 @@
+# TMUX
+
+| ShortCut      | Action     |
+|---------------|------------|
+| Prefix+Ctrl+O | Swap Panes |

Resources/electricity/ac.md

@@ -1,7 +1,7 @@
 # AC (Alternating Current)
 
 
-![](./assets/wave.gif)
+![](wave.gif)
 
 
 A few important characteristics of an AC Signal:
@@ -21,7 +21,7 @@ The difference between the highest and lowest peak.
 ## Root Mean Square Values
 This helps calculating the current an equivalent DC Signal would need to provide the same amount of power.
 
-![](./assets/rms.gif)
+![](rms.gif)
 
 $$
 \begin{flalign}

Resources/electricity/assets/open-drone-map-arch.md

@@ -31,7 +31,7 @@ Browser ^8G0ZtAAK
 
 
 # Embedded files
-7f38f53feb6c797675e3f24fa22a89a899ceaddc: [[Areas/electricity/assets/Pasted Image 20220330151250_777.png]]
+7f38f53feb6c797675e3f24fa22a89a899ceaddc: [[Pasted Image 20220330151250_777.png]]
 
 %%
 # Drawing

Resources/electricity/circuits/rc-low-pass.md

@@ -10,7 +10,7 @@ We can also see that for the RL LowPass Filter the positions of the resistor and
 
 **Example:**
 
-Lets design a RC LowPass Filter with a [[glossary#Cutoff Frequency|Cutoff Frequency]] of $15.9kHz$. The Formular for calculating the cutoff frequency is the following:
+Lets design a RC LowPass Filter with a [[Resources/electricity/glossary#Cutoff Frequency|Cutoff Frequency]] of $15.9kHz$. The Formular for calculating the cutoff frequency is the following:
 
 ![[formulas#Cutoff Frequency for RC Filters]]
 

Resources/electricity/formulas.md

@@ -50,7 +50,7 @@ $$
 
 **Example:**
 
-![](./assets/kirchhoffs-law-01.svg)
+![](kirchhoffs-law-01.svg)
 
 For this circuit kirchhoffs law states that:
 

Resources/electricity/formulas/kirchhoffs-law.md.md

@@ -3,7 +3,7 @@
 ### Example 1
 **Example:**
 
-![](../assets/kirchhoffs-law-02.svg)
+![](kirchhoffs-law-02.svg)
 
 For this circuit this means.
 

Resources/electricity/impedance.md

@@ -17,7 +17,7 @@ We can also represent these impedances as seperated things:
 
 
 
-# [[glossary#Input Impedance Z_ in|Input Impedance]]
+# [[Resources/electricity/glossary#Input Impedance Z_ in|Input Impedance]]
 
 Input impedance is the impedance seen by anything connected to the input of a circuit. It is the combined effect of all resistance, capacitance and inductance connected to the input side of the circuit.
 
@@ -49,7 +49,7 @@ We can use the voltage divtider equation to calculate the voltage that is availa
 
 ![[voltage-dividers#Simple Voltage Divider#Equation]]
 
-# [[glossary#Output Impedance Z_ out|Output Impedance]]
+# [[Resources/electricity/glossary#Output Impedance Z_ out|Output Impedance]]
 
 The output impedance is the combined effect of all resistors, capacitors and inductors connected to the output inside the circuit.
 

Resources/electricity/index.md

@@ -1,7 +1,7 @@
 # Learning Analog Hardware
 
-[Glossary](./glossary.md)
-[Formulas](./formulas.md)
+[Glossary](Resources/electricity/glossary.md)
+[Formulas](formulas.md)
 
 ## Building Blocks
 - [LED](./led)

Resources/electricity/passive-components/capacitors.md

@@ -1,6 +1,6 @@
 # Capacitors
 
-Capacity is measured in [[glossary#Farad|Farads]].
+Capacity is measured in [[Resources/electricity/glossary#Farad|Farads]].
 
 Capacity is calculated as follows:
 
@@ -15,7 +15,7 @@ $$
 $$
 
 
-![](../assets/Parallel_plate_capacitor.svg)
+![](Parallel_plate_capacitor.svg)
 
 ### Important Metrics
 
@@ -70,7 +70,7 @@ The capacity is not always exact, the tolerance describes how much it could vary
 - low current leakage and ESR
 - best for high frequency coupling
 
-![](../assets/ceramic-capacitor.webp)
+![](ceramic-capacitor.webp)
 
 
 ## Aluminium and Tantalum Electrolytic
@@ -78,7 +78,7 @@ The capacity is not always exact, the tolerance describes how much it could vary
 - Capacity usuially $1\micro F - 1mF$
 - Good for high voltage
 
-![](../assets/tantalum-capacitor.jpg)
+![](tantalum-capacitor.jpg)
 
 ## Super Capacitors
 

Resources/electricity/passive-components/capacitors/impedance-reactance.md

@@ -10,7 +10,7 @@ $Xc = \textit{Capacity in } \ohm$
 f = Frequency in Hertz
 C = Capacitance in Farads
 
-![](../../assets/graphXC.gif)
+![](graphXc.gif)
 
 Higher Frequence $\Rightarrow$ Lower Current Flow
 Higher Capacitance $\Rightarrow$ Lower Current Flow
@@ -74,7 +74,7 @@ $$
 
 ## Reality
 In reality capacitors are not perfect, they are more like:
-![](../../assets/rlc-capacitor.svg)
+![](rlc-capacitor.svg)
 
 So the have a $ESR$ and $X_{C}$ and $X_{L} / ESL$
 
@@ -84,8 +84,8 @@ $$
 
 Due to this the frequency to impedance curve of real capacitors look something like this.
 
-![](../../assets/EMC-9_graf_01.gif)
+![](EMC-9_graf_01.gif)
 
 When we add multiple capacitors we can get a curve looking like this
 
-![](../../assets/rlc-capacitor-multiple.png)
+![](rlc-capacitor-multiple.png)

Resources/electricity/passive-components/capacitors/rc-time-constant.md

@@ -41,9 +41,9 @@ In words this means after 47 seconds the capacitor will be at 63% of the input v
 
 We can use capacitors to filter out any signal above a certain frequency in a signal. This is called a low pass filter. This is usefull to filter out noise in a signal for example.
 
-![](../../assets/low-pass-filter.png)
+![](low-pass-filter.png)
 
-![](../../assets/low-pass-cutoff.png)
+![](low-pass-cutoff.png)
 
 We can see here that the high frequencies are reduced, while the low frequencies keep their strength. Above a certain frequency the signal is reduced by 70%, that point is called the cutoff frequency. We can calculate that point like this:
 $$