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| electrical_engineering_and_electronics_1:block05 [2025/10/10 21:41] – [Learning objectives] mexleadmin | electrical_engineering_and_electronics_1:block05 [2026/01/10 13:23] (current) – mexleadmin | ||
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| - | ====== Block 05 — Resistive | + | ====== Block 05 — Resistive |
| - | ===== Learning objectives | + | ===== 5.0 Intro ===== |
| + | |||
| + | ==== 5.0.1 Learning Objectives | ||
| < | < | ||
| After this 90-minute block, you can | After this 90-minute block, you can | ||
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| </ | </ | ||
| - | ===== Preparation at Home ===== | + | ==== 5.0.2 Preparation at Home ==== |
| And again: | And again: | ||
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| ~~PAGEBREAK~~ ~~CLEARFIX~~ | ~~PAGEBREAK~~ ~~CLEARFIX~~ | ||
| - | ===== 90-minute | + | ==== 5.0.3 90-minute |
| * 0–10 min — Recap KCL/KVL; sign conventions. | * 0–10 min — Recap KCL/KVL; sign conventions. | ||
| * 10–30 min — Series & parallel; quick numeric checks. | * 10–30 min — Series & parallel; quick numeric checks. | ||
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| ~~PAGEBREAK~~ ~~CLEARFIX~~ | ~~PAGEBREAK~~ ~~CLEARFIX~~ | ||
| - | ===== Core Content ===== | + | ===== 5.1 Core Content ===== |
| - | ==== Unloaded | + | ==== 5.1.1 Unloaded |
| The series circuit of two resistors $R_1$ and $R_2$ shall be considered now. \\ | The series circuit of two resistors $R_1$ and $R_2$ shall be considered now. \\ | ||
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| ~~PAGEBREAK~~ ~~CLEARFIX~~ | ~~PAGEBREAK~~ ~~CLEARFIX~~ | ||
| - | ==== The loaded Voltage Divider ==== | + | ==== 5.1.2 The loaded Voltage Divider ==== |
| If - in contrast to the abovementioned, | If - in contrast to the abovementioned, | ||
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| $ U_1 = \LARGE{{U} \over {1 + {{R_2}\over{R_L}} + {{R_2}\over{R_1}} }}$ | $ U_1 = \LARGE{{U} \over {1 + {{R_2}\over{R_L}} + {{R_2}\over{R_1}} }}$ | ||
| - | or on a potentiometer | + | An alternative representation of the formula sticks more to the application. \\ |
| + | It uses: | ||
| + | - the position | ||
| + | - the sum of resistors $R_{\rm s} = R_1 + R_2$. | ||
| + | Both are more often used in real setups. | ||
| - | $ U_1 = \LARGE{{k \cdot U} \over { 1 + k \cdot (1-k) \cdot{{R_{\rm s}}\over{R_{\rm L}}} }}$ | + | Mathematically, |
| + | When these tyo relations are included in rhe the formula above, we get: | ||
| + | |||
| + | $ U_1 = U \cdot k \cdot \LARGE{{1} \over { 1 + k \cdot (1-k) \cdot{{R_{\rm s}}\over{R_{\rm L}}} }}$ | ||
| <imgref BildNr65> | <imgref BildNr65> | ||
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| ~~PAGEBREAK~~ ~~CLEARFIX~~ | ~~PAGEBREAK~~ ~~CLEARFIX~~ | ||
| - | ==== Bridge | + | ==== 5.1.3 Bridge |
| A four-resistor bridge can be seen as **two voltage dividers in parallel**. The detector (bridge branch) sees the **difference** of the two divider node voltages. The **balance condition** (zero detector current) is | A four-resistor bridge can be seen as **two voltage dividers in parallel**. The detector (bridge branch) sees the **difference** of the two divider node voltages. The **balance condition** (zero detector current) is | ||
| \begin{align*} | \begin{align*} | ||
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| ~~PAGEBREAK~~ ~~CLEARFIX~~ | ~~PAGEBREAK~~ ~~CLEARFIX~~ | ||
| - | ==== Strategy for network reduction ==== | + | ==== 5.1.4 Strategy for network reduction ==== |
| * Reshape (without changing node connections), | * Reshape (without changing node connections), | ||
| - | * If blocked by a three-terminal cluster, apply **Δ–Y** (or **Y–Δ**), | + | * (If blocked by a three-terminal cluster, apply **Δ–Y** (or **Y–Δ**), |
| * Repeat until a simple ladder remains; finish with KCL/KVL if needed. | * Repeat until a simple ladder remains; finish with KCL/KVL if needed. | ||
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| | | ||
| ~~PAGEBREAK~~ ~~CLEARFIX~~ | ~~PAGEBREAK~~ ~~CLEARFIX~~ | ||
| - | ===== Exercises ===== | + | ===== 5.2 Exercises ===== |
| <panel type=" | <panel type=" | ||
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