====== Block 02 — Electric charge, current, voltage ====== ===== Learning objectives ===== After this 90-minute block, you can * Define electric charge $Q$ and explain its quantization in multiples of the elementary charge $e$. * Distinguish positive and negative charges, their interactions, and typical carriers (electrons, ions). * Define electric current $I$ as rate of charge flow; relate $I$ to moving charge via $I = \frac{{\rm d}Q}{{\rm d}t}$. * Apply the unit check for $1~\rm A = 1~C/s$ and recall typical current magnitudes (pA … kA). * Explain and consistently use the **conventional current direction**. * Define electric voltage $U$ as potential difference and relate it to energy per unit charge: $U=W/Q$. * Distinguish potential reference (ground) and explain why only voltage differences are measurable. ===== 90-minute plan ===== - Warm-up (5–10 min): - Recall of SI units from Block 01; estimate “How many electrons per second flow at $1~\rm A$?” - Quick quiz – “What is larger: voltage of a lightning strike or mains outlet?” - Core concepts & derivations (60–70 min): - Electric charge: definition, elementary charge, Coulomb’s law (overview only). - Charge carriers in metals vs. electrolytes. - Electric current: definition, instantaneous and average values, unit check. - Typical magnitudes; conventional vs. electron flow. - Practice (10–20 min): Quick calculations and sim-based exercises. - Wrap-up (5 min): Summary and pitfalls. ===== Conceptual overview ===== - **Charge $Q$** is the fundamental “substance” of electricity, always in multiples of the elementary charge. - **Like charges repel, unlike charges attract**; forces are described by Coulomb’s law (detail in Block 09). - **Current $I$** quantifies *how fast* charge moves: $1~\rm A$ = $1~C/s$. - Convention: we follow **conventional current direction** (positive charge motion, from $+$ to $-$), even though in metals electrons move oppositely. - This block connects Block 01 (units) to Block 03 (voltage and resistance), and prepares for Kirchhoff’s laws in Block 04. ~~PAGEBREAK~~ ~~CLEARFIX~~ ===== Core content ===== ==== Electric charge ==== {{drawio>Atommodell.svg}} * Electric charge $Q$ is a physical quantity indicating the amount of excess or deficit of electrons or ions. * the charge is based on the electron shell and the atomic nucleus, see the atomic model of Bohr and Sommerfeld in * Due to the electrons and protons it is **quantized** in multiples of the elementary charge: \begin{align*} e &= 1.602 \cdot 10^{-19}~\rm C \\ Q &= n \cdot e \end{align*} with $n \in \mathbb{Z}$. * Positive charge: deficiency of electrons generates an excess of positive charges (e.g. ionized atoms). * Negative charge: excess electrons overcompensates the positive charges. * charges with different signs attract each other. Charges with similar sign repell each other \begin{align*} [Q] = 1~\rm C = 1~A \cdot s \end{align*} How many electrons correspond to a charge of $1~\rm C$? \begin{align*} n = \frac{Q}{e} = \frac{1~\rm C}{1.602\cdot 10^{-19}~\rm C} \approx 6.24 \cdot 10^{18} \end{align*} ==== Electric current ==== An **electric current** arises when charges move in a preferred direction, e.g. by attraction and repulsion. The current is defined as \begin{align*} I = \frac{Q}{t} \end{align*} The instantaneous current is defined as \begin{align*} i(t) = \frac{{\rm d}Q}{{\rm d}t} \end{align*} Unit check: \begin{align*} [i] &= \frac{[Q]}{[t]} = \frac{1~\rm C}{1~\rm s} = 1~\rm A \end{align*} Charge transport can take place through * In metals: flow of electrons. * In electrolytes: movement of ions. * In semiconductors: electrons and holes. In this course, we generally use the **conventional current direction**: positive from $+$ to $-$. The electron flow is opposite. * $10~\rm pA$ — control current in a FET gate * $10~\rm \mu A$ — sensitive sensor output * $10~\rm mA$ — LED or small sensor supply * $10~\rm A$ — heating device * $10~\rm kA$ — large generator output ==== Electrodes ==== An electrode is a connection (or pin) of an electrical component. \\ Looking at a component, the electrode is characterized as the homogenous part of the component, where the charges come in / move out (usually made out of metal). \\ The name of the electrode is given as follows: * **A**node: Electrode at which the current enters the component. * Cathode: Electrode at which the current exits the component. (in German //**K**athode//) As a mnemonic, you can remember the diode's structure, shape, and electrodes (see ). {{drawio>Diode_Elektroden.svg}} ==== Electric voltage ==== Every rock on a mountain has a higher energy potential than a rock in the valley. As higher up and as more mass the rock has, as more energy is stored. The energy difference $\Delta W_{1,2}$ is given by the height difference $\Delta h_{1,2}$ \begin{align*} \Delta W_{1,2} = m \cdot g \cdot \Delta h_{1,2} \end{align*} Similarily, charges on the positive pin of a battery has a higher energy potential than charges on the negative pin. Similar to the transport of a mass in the gravitational field, energy is needed/released when charge is moved in an electric field. We will look at the specific electric field starting from [[block09]]. For the energy in an electric field, as higher the object is charged ($Q$), as more energy $\Delta W_{1,2}$ can be released / is needed for movements. The equivalent to the height $h$ in the mechanic picture is the potential $\varphi$ in the electric case: \begin{align*} \Delta W_{1,2} = Q \cdot \Delta \varphi_{1,2} \end{align*} It follows that: \\ \begin{align*} \boxed{{\Delta W_{1,2} \over {Q}} = \varphi_1 - \varphi_2 = U_{1,2}} \end{align*} voltage $U_{1,2}$ is the energy $W_{1,2}$ per charge $Q$ between two points $1$ and $2$. * **Units:** $[U]=[W]/[Q]=1~{\rm J}/1~{\rm C}=1~{\rm V}$. * **Reference:** We choose one node as potential zero (“ground”); only differences are meaningful. * Thermal noise: $\sim \mu{\rm V}$ * Microcontroller: supply $1.8~{\rm V}$ to $5.0~{\rm V}$ (often given as ''1V8'' and ''5V0'' or in general as ''VCC'' or ''VDD'') * Mains: $230~{\rm V}$ * Lightning: $>10^6~{\rm V}$ A charge $Q=2.0~{\rm mC}$ moves through a potential difference of $5.0~{\rm V}$. Energy transferred: \\ $W=U \cdot Q=5.0~{\rm V} \cdot 2.0~{\rm mC}=10.0~{\rm mJ}$. ==== Comparison: Mechanics vs Electrics ==== {{drawio>mechanisches_Potential.svg}} === Mechanical System === **Potential Energy** Potential energy is always related to a reference level (reference height). The energy required to move $m$ from $h_1$ to $h_2$ is independent of the reference level. $\Delta W_{1,2} = W_1 - W_2 = m \cdot g \cdot h_1 - m \cdot g \cdot h_2 = m \cdot g \cdot (h_1 - h_2)$ {{drawio>elektrisches_Potential.svg}} === Electrical System === **Potential** The potential $\varphi$ is always specified relative to a reference point. Common used are: * Earth potential (ground, earth, ground). * infinitely distant point To shift the charge, the potential difference must be overcome. The potential difference is independent of the reference potential. $\boxed{\Delta W_{1,2} = W_1 - W_2 = Q \cdot \varphi_1 - Q \cdot \varphi_2 = Q \cdot (\varphi_1 - \varphi_2)}$ ===== Common pitfalls ===== * Mixing electron flow vs. conventional current. * Misinterpreting current as “speed” rather than rate of charge flow. * Given the definition, rechargeable batteries not have a fixed cathode / anode. Here, usually discharging the battery is considered. ===== Exercises ===== {{tagtopic>chapter1_2&nodate&nouser&noheader&nofooter&order=custom}} #@TaskTitle_HTML@#1.5.1 Direction of the voltage #@TaskText_HTML@# {{drawio>BeispKonventionelleSpannungsangabe.svg}} Explain whether the voltages $U_{\rm Batt}$, $U_{12}$ and $U_{21}$ in are positive or negative according to the voltage definition. #@HiddenBegin_HTML~1,Hints~@# * Which terminal has the higher potential? * From where to where does the arrow point? #@HiddenEnd_HTML~1,Hints~@# #@HiddenBegin_HTML~2,Result~@# * ''+'' is the higher potential. Terminal 1 has the higher potential. $\varphi_1 > \varphi_2$ * For $U_{\rm Batt}$: The arrow starts at terminal 1 and ends at terminal 2. So $U_{\rm Batt}=U_{12}>0$ * $U_{21}<0$ #@HiddenEnd_HTML~1l2,Result~@# #@TaskEnd_HTML@# {{fa>pencil?32}} A flashlight bulb is supplied with $I=0.25~\rm A$. How many electrons pass through the filament in one second? Use $n=\frac{I \cdot t}{e}$ with $t=1~\rm s$. \begin{align*} n = \frac{0.25~\rm C}{1.602 \cdot 10^{-19}~\rm C} \approx 1.6 \cdot 10^{18} \end{align*} {{tagtopic>chapter1_4&nodate&nouser&noheader&nofooter&order=custom}} ===== Embedded resources ===== \\ \\ Charge in Matter {{youtube>HY_ZJTREpfU}} What is Electric Charge and How Electricity Works {{youtube>iqVtGNQAC2E}} Electric - Hydraulic Analogy: Charge, Voltage, and Current {{youtube>Lvp_a_JkD2o}}