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diff --git a/Areas/upv/classes/electricidad/index.md b/Archive/electricidad/index.md
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diff --git a/Resources/dev/tmux.md b/Resources/dev/tmux.md
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index 0000000..bcab30d
--- /dev/null
+++ b/Resources/dev/tmux.md
@@ -0,0 +1,5 @@
+# TMUX
+
+| ShortCut      | Action     |
+|---------------|------------|
+| Prefix+Ctrl+O | Swap Panes |
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@@ -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}
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index 1775daf..72a1d8a 100644
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+++ b/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
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+++ b/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]]
 
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diff --git a/Areas/electricity/datasheets/1N4148.pdf b/Resources/electricity/datasheets/1N4148.pdf
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diff --git a/Areas/electricity/datasheets/lm741.pdf b/Resources/electricity/datasheets/lm741.pdf
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diff --git a/Areas/electricity/datasheets/tlur6400.pdf b/Resources/electricity/datasheets/tlur6400.pdf
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diff --git a/Areas/electricity/formulas.md b/Resources/electricity/formulas.md
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index 66e4770..84603d3 100644
--- a/Areas/electricity/formulas.md
+++ b/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:
 
diff --git a/Areas/electricity/formulas/kirchhoffs-law.md.md b/Resources/electricity/formulas/kirchhoffs-law.md.md
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index 087601e..f7fe250 100644
--- a/Areas/electricity/formulas/kirchhoffs-law.md.md
+++ b/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.
 
diff --git a/Areas/electricity/glossary.md b/Resources/electricity/glossary.md
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diff --git a/Areas/electricity/impedance.md b/Resources/electricity/impedance.md
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index d174404..e164326 100644
--- a/Areas/electricity/impedance.md
+++ b/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.
 
diff --git a/Areas/electricity/index.md b/Resources/electricity/index.md
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index 3430e84..00a530e 100644
--- a/Areas/electricity/index.md
+++ b/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)
diff --git a/Areas/electricity/passive-components/capacitors.md b/Resources/electricity/passive-components/capacitors.md
similarity index 92%
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index 18b5097..d705266 100644
--- a/Areas/electricity/passive-components/capacitors.md
+++ b/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
 
diff --git a/Areas/electricity/passive-components/capacitors/coupling.md b/Resources/electricity/passive-components/capacitors/coupling.md
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diff --git a/Areas/electricity/passive-components/capacitors/impedance-reactance.md b/Resources/electricity/passive-components/capacitors/impedance-reactance.md
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index 3befab8..71b834a 100644
--- a/Areas/electricity/passive-components/capacitors/impedance-reactance.md
+++ b/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)
\ No newline at end of file
+![](rlc-capacitor-multiple.png)
\ No newline at end of file
diff --git a/Areas/electricity/passive-components/capacitors/rc-time-constant.md b/Resources/electricity/passive-components/capacitors/rc-time-constant.md
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--- a/Areas/electricity/passive-components/capacitors/rc-time-constant.md
+++ b/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:
 $$
diff --git a/Areas/electricity/passive-components/capacitors/smoothing.md b/Resources/electricity/passive-components/capacitors/smoothing.md
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diff --git a/Areas/electricity/passive-components/diodes.md b/Resources/electricity/passive-components/diodes.md
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diff --git a/Areas/electricity/passive-components/diodes/example.md b/Resources/electricity/passive-components/diodes/example.md
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diff --git a/Areas/electricity/passive-components/filters.md b/Resources/electricity/passive-components/filters.md
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index 045974f..1fd260d 100644
--- a/Areas/electricity/passive-components/filters.md
+++ b/Resources/electricity/passive-components/filters.md
@@ -27,7 +27,7 @@ Aktive filters use active components like op-amps or transistors, active filters
 ## Notch Filter
 
 
-# [[glossary#Cutoff Frequency|Cutoff Frequency]]
+# [[Resources/electricity/glossary#Cutoff Frequency|Cutoff Frequency]]
 
 ![[cutoff-frequency.png]]
 
@@ -45,7 +45,7 @@ We have a RC LFP which looks like this:
 
 ![[lfp-example.png|200]]
 
-First lets calculate the [[glossary#Cutoff Frequency|Cutoff Frequency]] with the specified formula:
+First lets calculate the [[Resources/electricity/glossary#Cutoff Frequency|Cutoff Frequency]] with the specified formula:
 
 ![[formulas#Cutoff Frequency for RC LowPass]]
 
diff --git a/Areas/electricity/passive-components/inductors.md b/Resources/electricity/passive-components/inductors.md
similarity index 94%
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index 77220ff..617c6b4 100644
--- a/Areas/electricity/passive-components/inductors.md
+++ b/Resources/electricity/passive-components/inductors.md
@@ -6,7 +6,7 @@ Inductors are similar to capacitors, but there are a few key differences:
 2. **They resist to changes in current**
 3. 
 
-![[../assets/inductor_schematic.png]]
+![[inductor_schematic.png]]
 
 **Inductance:**
 $$
@@ -70,7 +70,7 @@ r 96 128 240 128 0 200
 o 1 64 0 4099 5 0.025 0 2 1 3
 ```
 
-Calculate the [[glossary#Impedance Z|Impedance]] in this Circuit:
+Calculate the [[Resources/electricity/glossary#Impedance Z|Impedance]] in this Circuit:
 
 $$
 \begin{flalign}
diff --git a/Areas/electricity/passive-components/inductors/back-emf.md b/Resources/electricity/passive-components/inductors/back-emf.md
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--- a/Areas/electricity/passive-components/inductors/back-emf.md
+++ b/Resources/electricity/passive-components/inductors/back-emf.md
@@ -9,7 +9,7 @@ It is caused by a changing magnetic field around the inductor, which itself is c
 
 ### Example:
 
-![](../../assets/back_emf_curve.png)
+![](back_emf_curve.png)
 
 After switch on (A $\rightarrow$ B) we see that the voltage spikes immediately, this causes the magnetic field to change rapidly, which creates a oppositional polarity, which causes a huge resistance to current flow, so the current flowing at the start is almot zero. As soon as the voltage begins to drop, the back emf becomes weaker and current is allowed to flow.
 
diff --git a/Areas/electricity/passive-components/led.md b/Resources/electricity/passive-components/led.md
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diff --git a/Areas/electricity/passive-components/rlc-series-response.md b/Resources/electricity/passive-components/rlc-series-response.md
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+++ b/Resources/electricity/passive-components/rlc-series-response.md
@@ -19,7 +19,7 @@ At this resonance frequency the impedance from capacitor and inductor cancel eac
 
 When we graph out the impedance vs frequency in a circuit, it could look something like this:
 
-![](../assets/rlc-resonance.png)
+![](rlc-resonance.png)
 
 This could cause problems because the voltage is really high at that point, which maybe bad for some other parts.
 
diff --git a/Areas/electricity/passive-components/transformers.md b/Resources/electricity/passive-components/transformers.md
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+++ b/Resources/electricity/passive-components/transformers.md
@@ -1,12 +1,12 @@
 # Transformers
 
-![](../assets/new-transformer.jpg)
+![](new-transformer.jpg)
 
 The amount of primary and secondary windings dictate how much the voltage changes between the two. 
 
 There are two main types of transformers:
 
-![](../assets/transformer-types.jpg)
+![](transformer-types.jpg)
 
 When there are more turns on the primary winding, that means that the voltage on the secondary winding is lower, but the current is higher, and vice versa. Also this relationshop is linear, so half the amount of turns in the second winding, mean half the amount of voltage and double the amount of current. In formula this means:
 
diff --git a/Areas/electricity/passive-components/voltage-dividers.md b/Resources/electricity/passive-components/voltage-dividers.md
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