1.1.12Electricity & Charge Basics

Understand inductance and the henry

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WHAT is inductance?


WHY does a coil oppose current change? (Derive from first principles)

Step 1 — Current makes a magnetic field. Any current II produces magnetic flux ΦI\Phi \propto I. Wind the wire into NN turns and the flux links all NN turns, so the total flux linkage is λ=NΦ\lambda = N\Phi.

Why this step? More turns and more current both mean more magnetic field, so flux linkage scales with both.

Step 2 — Define LL as the proportionality constant. Because flux linkage is proportional to current for a fixed geometry: λ=NΦ=LIL=NΦI\lambda = N\Phi = L\,I \quad\Rightarrow\quad L = \frac{N\Phi}{I}

Why this step? LL bundles all the geometry (turns, area, core material) into one number so we don't recompute the field every time.

Step 3 — Faraday's law: changing flux makes voltage. Faraday says an induced EMF equals the rate of change of flux linkage: ε=dλdt\varepsilon = -\frac{d\lambda}{dt}

Substitute λ=LI\lambda = LI (with LL constant):   ε=LdIdt  \boxed{\;\varepsilon = -L\,\frac{dI}{dt}\;}

Why the minus sign? Lenz's law — the induced voltage opposes the change that made it. That's the "electrical inertia."


WHY is energy 12LI2\tfrac{1}{2}LI^2? (Derive it)

Power delivered to the inductor: P=VI=(LdIdt)IP = VI = \left(L\dfrac{dI}{dt}\right)I.

Energy is power integrated over time as current rises from 00 to II: E=Pdt=0ILIdI=12LI2E=\int P\,dt = \int_0^I L\,I\,dI = \tfrac{1}{2}LI^2

Why this step? We swapped dtdt for dIdI using dIdtdt=dI\frac{dI}{dt}\,dt = dI, turning a time integral into a clean current integral. The energy lives in the magnetic field, not in heat — it comes back when current falls.

Figure — Understand inductance and the henry

HOW does geometry set LL? (Solenoid derivation)

For a long solenoid of NN turns, length \ell, cross-section area AA, core permeability μ\mu:

  • Field inside: B=μNIB = \mu \frac{N}{\ell} I
  • Flux per turn: Φ=BA=μNAI\Phi = BA = \mu \frac{N A}{\ell} I
  • Flux linkage: NΦ=μN2AIN\Phi = \mu \frac{N^2 A}{\ell} I

Divide by II: L=μN2AL = \mu\,\frac{N^2 A}{\ell}

Why it matters: LN2L \propto N^2doubling turns quadruples inductance. Iron cores raise μ\mu hugely, so a small iron-core coil beats a big air coil.


Worked Examples


Common Mistakes (Steel-manned)


Flashcards

What is inductance in one sentence?
A measure of how strongly a component opposes a change in the current through it (via its magnetic field).
Define the henry.
1 H is the inductance where a current changing at 1 A/s induces 1 V; equivalently 1 Wb/A = 1 V·s/A.
Voltage across an inductor formula?
V=LdI/dtV = L\,dI/dt — proportional to the rate of change of current.
Why the minus sign in ε=LdI/dt\varepsilon=-L\,dI/dt?
Lenz's law: the induced EMF opposes the change in current that produces it.
Energy stored in an inductor?
E=12LI2E=\tfrac12 LI^2, stored in the magnetic field.
Inductance of a solenoid?
L=μN2A/L=\mu N^2 A/\ell.
If you double the turns, what happens to L?
It quadruples, because LN2L\propto N^2.
What does an ideal inductor do in steady DC?
Nothing — dI/dt=0dI/dt=0 so V=0V=0; it behaves like a plain wire.
Capacitor vs inductor duals?
Capacitor resists voltage change (E-field, 12CV2\tfrac12CV^2); inductor resists current change (B-field, 12LI2\tfrac12LI^2).
Flux-linkage definition of L?
L=NΦ/IL=N\Phi/I (flux linkage per unit current).

Recall Feynman: explain to a 12-year-old

Imagine pushing a heavy merry-go-round. It's hard to get it spinning, and once it's spinning fast it's hard to stop — it "wants" to keep going. A coil of wire is like that for electricity. When you turn the current on, the coil fights you at first; when you try to switch it off, the coil fights again and can even give a nasty spark, because it wants to keep the current flowing. The henry is just how we measure how stubborn a coil is: a big henry number means a very stubborn coil.


Connections

  • Faraday's Law of Induction — the parent principle giving ε=dλ/dt\varepsilon=-d\lambda/dt.
  • Lenz's Law — source of the opposing minus sign.
  • Capacitance and the Farad — the electrical dual of inductance.
  • Magnetic Field of a Solenoid — where B=μNI/B=\mu NI/\ell comes from.
  • RL Circuits and Time Constant — where τ=L/R\tau = L/R governs current rise.
  • Energy Storage in Fields12LI2\tfrac12LI^2 vs 12CV2\tfrac12CV^2.

Concept Map

produces

link flux

scales with I

L as constant

measured in

Faraday's law

Lenz's law opposes change

defines

integrate power

stored in

acts like

Current I

Magnetic flux

N turns

Flux linkage N-Phi

Inductance L

Henry H

Induced EMF

V equals L dI/dt

Energy half L I squared

Magnetic field

Electrical flywheel

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Dekho, inductance ka matlab hai ki ek coil current ke change ko oppose karti hai. Jab aap coil mein current bhejte ho, wo apne aas-paas ek magnetic field bana leti hai. Ye field ek tarah ki "inertia" jaisi hoti hai — jaise heavy pankha (flywheel) ghumana mushkil hota hai, waise hi coil mein current ko badalna mushkil hota hai. Iska unit hai henry (H): agar current 1 amp per second ke rate se badle aur us se 1 volt induce ho, to inductance 1 henry hai.

Sabse important baat: inductor ke across voltage current par nahi, balki current ke rate of change par depend karta hai — yaani V=LdI/dtV = L\,dI/dt. Isliye steady DC mein (dI/dt=0dI/dt=0) inductor bas ek simple taar jaisa behave karta hai, koi voltage drop nahi. Lekin jab current suddenly change karo, to bada voltage aa sakta hai (isiliye switch off karte time spark dikhta hai).

Energy bhi store hoti hai magnetic field mein: E=12LI2E=\tfrac12 LI^2. Ye formula hum khud derive karte hain power VIVI ko time ke saath integrate karke. Aur geometry se: L=μN2A/L=\mu N^2 A/\ell — matlab turns double karo to inductance 4 guna ho jaata hai kyunki N2N^2 aata hai. Ye concept RL circuits, transformers aur power supplies mein har jagah kaam aata hai, isliye ache se samajhna zaroori hai.

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