1.8.18Electromagnetism

Kirchhoff's current law (KCL), Kirchhoff's voltage law (KVL)

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WHY do these laws exist?

WHY KCL? Charge cannot be created or destroyed, and in steady state it cannot accumulate at a single point (a node has no capacity to store charge). So whatever current flows in must flow out.

WHY KVL? Electric potential is a property of a point. If you take any round-trip and come back to the same point, the potential is the same as when you left — so the total potential change around the loop is zero. This is just saying the electrostatic field is conservative (Edl=0\oint \vec{E}\cdot d\vec{l}=0 for steady fields).


KCL — Kirchhoff's Current Law

Derivation from first principles. Charge conservation says the rate of charge change in a tiny region equals net current flowing in: dQnodedt=IinIout.\frac{dQ_{\text{node}}}{dt} = \sum I_{\text{in}} - \sum I_{\text{out}}. In steady state (or for an idealized node with no charge storage), dQnodedt=0\dfrac{dQ_{\text{node}}}{dt}=0. Therefore Iin=IoutIk=0.\sum I_{\text{in}} = \sum I_{\text{out}} \quad\Longrightarrow\quad \sum I_k = 0. Why this step? Setting dQ/dt=0dQ/dt=0 is the whole content of KCL — a node is not a battery or capacitor; it can't hoard charge.


KVL — Kirchhoff's Voltage Law

Derivation from first principles. Potential is single-valued at each point. Start at point AA with potential VAV_A, walk through elements gaining/losing potential, and return to AA: VA+(ΔV1)+(ΔV2)++(ΔVn)=VA.V_A + (\Delta V_1) + (\Delta V_2) + \dots + (\Delta V_n) = V_A. Subtract VAV_A: kΔVk=0.\sum_k \Delta V_k = 0. Why this step? You return to the same point, so its potential hasn't changed — the trip must net to zero.

Sign conventions (the part that trips everyone)

Travel around the loop in a chosen direction:

  • Through a resistor in the direction of current → potential drops by IRIR (write IR-IR).
  • Through a resistor against the current → potential rises (+IR+IR).
  • Through a battery from − to + terminal → potential rises (+ε+\varepsilon).
  • Through a battery from + to − → potential drops (ε-\varepsilon).
Figure — Kirchhoff's current law (KCL), Kirchhoff's voltage law (KVL)

Worked Example 1 — Single loop

A loop with EMF ε=12 V\varepsilon = 12\text{ V} and two resistors R1=2 ΩR_1 = 2\ \Omega, R2=4 ΩR_2 = 4\ \Omega in series. Find the current II.

  1. Assume a current direction, say clockwise. Why? KVL needs an assumed direction; a wrong guess just gives a negative answer.
  2. Apply KVL going clockwise starting from the battery's − terminal: +εIR1IR2=0.+\varepsilon - IR_1 - IR_2 = 0. Why this step? Battery − to + is a rise; resistors in the current direction are drops.
  3. Solve: I=εR1+R2=126=2 A.I = \frac{\varepsilon}{R_1+R_2} = \frac{12}{6} = 2\text{ A}. Why this step? Algebra — and it reproduces the series-resistance result, a good sanity check.

Worked Example 2 — Node with three branches (KCL)

Currents I1=3 AI_1 = 3\text{ A} and I2=2 AI_2 = 2\text{ A} flow into a node; I3I_3 flows out. Find I3I_3.

  1. KCL: I1+I2I3=0I_1 + I_2 - I_3 = 0. Why? In-currents positive, out-current negative.
  2. I3=3+2=5 AI_3 = 3 + 2 = 5\text{ A}. Why this step? Charge in must equal charge out — none can vanish.

Worked Example 3 — Two-loop circuit (both laws together)

Battery ε=10 V\varepsilon = 10\text{ V} feeds a node that splits into R1=5 ΩR_1 = 5\ \Omega and R2=20 ΩR_2 = 20\ \Omega in parallel, then returns. Find branch currents.

  1. KCL at top node: I=I1+I2I = I_1 + I_2 where I1I_1 through R1R_1, I2I_2 through R2R_2. Why? Total current splits between the branches.
  2. KVL, loop through R1R_1: εI1R1=0I1=10/5=2 A\varepsilon - I_1 R_1 = 0 \Rightarrow I_1 = 10/5 = 2\text{ A}.
  3. KVL, loop through R2R_2: εI2R2=0I2=10/20=0.5 A\varepsilon - I_2 R_2 = 0 \Rightarrow I_2 = 10/20 = 0.5\text{ A}. Why? Both branches see the same voltage ε\varepsilon across them (parallel).
  4. Back to KCL: I=2+0.5=2.5 AI = 2 + 0.5 = 2.5\text{ A}. Check: Req=(520)/(25)=4 ΩR_{\text{eq}} = (5\cdot20)/(25) = 4\ \Omega, so I=10/4=2.5 AI = 10/4 = 2.5\text{ A}. ✓


Recall Feynman: explain to a 12-year-old

Think of wires as water pipes. KCL: at a T-junction, all the water flowing in must flow out — water doesn't disappear or pile up. KVL: imagine the voltage is height on a hilly path. The battery is a pump lifting you up; resistors are slides taking you down. Walk a full loop around the hill and you end where you started — so all the ups and downs must cancel to exactly zero. That's it: water is conserved, and a round trip on a hill brings you back to the same height.


Flashcards

What physical conservation law underlies KCL?
Conservation of electric charge (no charge accumulates at a node).
What physical conservation law underlies KVL?
Conservation of energy (potential is single-valued; a round trip returns to the same potential).
State KCL mathematically.
kIk=0\sum_k I_k = 0 at any node (in-currents positive, out negative); equivalently Iin=Iout\sum I_{in}=\sum I_{out}.
State KVL mathematically.
kVk=0\sum_k V_k = 0 around any closed loop (rises positive, drops negative).
Through a resistor in the direction of current, does potential rise or fall?
It falls by IRIR (a drop, IR-IR).
Through a battery from − to + terminal, rise or fall?
Potential rises by ε\varepsilon (+ε+\varepsilon).
If KVL gives a negative current, what does it mean?
Your assumed current direction was backward; magnitude is correct, just reverse the arrow.
Does current get "used up" in a resistor?
No — KCL keeps current the same in series; only energy (voltage) is dissipated.
For two resistors in parallel across an EMF, what is shared and what differs?
Same voltage across both; currents differ inversely with resistance.

Connections

  • Ohm's Law — supplies V=IRV=IR, combined with KCL/KVL solves any DC network.
  • Series and Parallel Resistors — derived directly from KCL + KVL.
  • Conservation of Charge — the basis of KCL.
  • Conservation of Energy — the basis of KVL.
  • Electric Potential — single-valuedness justifies KVL.
  • Wheatstone Bridge — application requiring both laws simultaneously.
  • Mesh and Nodal Analysis — systematic algorithms built on KVL and KCL.

Concept Map

justifies

justifies

applies at

applies around

no charge storage

gives

equivalent

single-valued potential

equivalent

needs

resistor & battery

combined with laws

combined with laws

combined with laws

Charge conservation

KCL node rule

Energy conservation

KVL loop rule

Node junction

Closed loop

dQ/dt = 0

sum Ik = 0

sum Vk = 0

Sign conventions

Ohm's law

DC circuit analysis

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Dekho, Kirchhoff ke do laws basically do simple conservation ideas hain. Pehla, KCL (Current Law): kisi bhi junction (node) par jitna current andar aata hai, utna hi bahar jaana chahiye — kyunki charge na to bante hai na khatam hota hai, aur node par charge jama nahi ho sakta. Isliye Iin=Iout\sum I_{in} = \sum I_{out}. Bas itni si baat hai — charge conserved hai.

Dusra, KVL (Voltage Law): kisi bhi closed loop ke charo taraf ghoom kar wapas usi point pe aao, to total voltage change zero hona chahiye. Soch lo voltage ek "height" hai pahaad par — battery tumhe upar uthata hai (pump), aur resistors tumhe neeche giraate hai (slide). Pura round maaro to wapas same height pe aa jaate ho, to saare ups aur downs cancel ho jaate hai: V=0\sum V = 0.

Sabse bada confusion hota hai signs mein. Ek loop direction choose karo (clockwise/anticlockwise), phir rule fix rakho: current ke direction mein resistor se guzro to voltage girta hai (IR-IR), battery ke − se + jao to voltage badhta hai (+ε+\varepsilon). Aur ek aur common galti — "resistor current ko kha jaata hai" — yeh galat hai. Resistor sirf energy (voltage) consume karta hai, current to series mein same rehta hai. Agar answer mein current negative aaye to ghabrao mat, sirf tumhara assumed direction ulta tha — magnitude sahi hai.

Yeh dono laws plus Ohm's law (V=IRV=IR) se tum koi bhi DC circuit solve kar sakte ho. Isliye yeh foundation hai — exam mein bhi aur real circuits design karne mein bhi.

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Connections