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Inductance Converter

Convert between inductance units including henry, microhenry, millihenry, nanohenry, and weber per ampere.


L

Inductor Circuit Symbol (L = Inductance)


Understanding Inductance

What is Inductance?

Inductance is the property of an electrical conductor that opposes changes in current. When current through an inductor changes, it creates a magnetic field that induces a voltage opposing that change (Lenz's Law). The SI unit is the henry (H).

1 H = 1 Wb/A = 1 V·s/A = 1 kg·m²/(A²·s²)

Named after Joseph Henry, who discovered self-inductance independently of Michael Faraday.

Faraday's Law of Induction

The voltage induced across an inductor is proportional to the rate of change of current.

V = L × (dI/dt)

Where V is voltage (volts), L is inductance (henrys), and dI/dt is the rate of current change (amperes per second).

Energy Stored in an Inductor

An inductor stores energy in its magnetic field. The energy depends on inductance and current.

E = ½ L I²

Where E is energy (joules), L is inductance (henrys), and I is current (amperes).

Inductive Reactance

In AC circuits, inductors have impedance that depends on frequency.

XL = 2πfL = ωL

Where XL is inductive reactance (ohms), f is frequency (hertz), and ω is angular frequency (radians/second). Higher frequency → higher impedance.

Self-Inductance

Self-inductance is the inductance of a single coil due to its own magnetic field. For a solenoid (long coil):

L = μ₀ μr N² A / l

Where μ₀ is permeability of free space, μr is relative permeability of core material, N is number of turns, A is cross-sectional area, and l is length.

Mutual Inductance

When two coils are near each other, current change in one induces voltage in the other. This mutual inductance (M) is the basis for transformers.

V₂ = M × (dI₁/dt)

The coupling coefficient k relates mutual inductance to self-inductances: M = k√(L₁L₂), where 0 ≤ k ≤ 1.

Inductors in Series and Parallel

Series (no mutual coupling)

Formula: Ltotal = L₁ + L₂ + L₃ + ...

Parallel (no mutual coupling)

Formula: 1/Ltotal = 1/L₁ + 1/L₂ + 1/L₃ + ...

Note: With mutual coupling, these formulas become more complex and must account for the coupling coefficient.

Abhenry (abH)

The abhenry is the CGS electromagnetic unit of inductance.

1 abH = 10⁻⁹ H = 1 nH

One abhenry equals one nanohenry. The abhenry is rarely used in modern practice.

Stathenry (statH)

The stathenry is the CGS electrostatic unit of inductance.

1 statH ≈ 8.98755 × 10¹¹ H ≈ 898.755 GH

The stathenry is extremely large and practically never used.

Types of Inductors

Air Core Inductors

  • Construction: Coil wound without magnetic core
  • Advantages: No core losses, linear behavior, high Q-factor
  • Disadvantages: Lower inductance per size
  • Applications: RF circuits, high-frequency oscillators

Ferrite Core Inductors

  • Construction: Coil wound on ferrite (ceramic magnetic material)
  • Advantages: High inductance, compact size
  • Disadvantages: Non-linear at high currents, temperature sensitive
  • Applications: Power supplies, EMI filters, transformers

Iron Core Inductors

  • Construction: Coil wound on laminated iron core
  • Advantages: Very high inductance, handles high power
  • Disadvantages: Heavy, core losses at high frequency
  • Applications: Power transformers, low-frequency chokes

Toroidal Inductors

  • Construction: Coil wound on donut-shaped core
  • Advantages: Self-shielding, high efficiency, compact
  • Disadvantages: Harder to wind, more expensive
  • Applications: Power supplies, audio equipment

SMD/Chip Inductors

  • Construction: Ceramic or ferrite with thin-film or multilayer winding
  • Advantages: Tiny size, suitable for automated assembly
  • Disadvantages: Limited current capacity, lower Q
  • Applications: Smartphones, portable electronics, RF circuits

Quality Factor (Q)

The quality factor measures inductor efficiency—the ratio of energy stored to energy dissipated.

Q = ωL / R = XL / R

Where R is the series resistance (ESR - equivalent series resistance). Higher Q means lower losses. Typical values:

  • Low Q (<10): Iron core power inductors
  • Medium Q (10-100): Ferrite core inductors, typical chip inductors
  • High Q (>100): Air core RF inductors, silver wire coils

Parasitic Capacitance

Real inductors have parasitic capacitance between windings, creating a self-resonant frequency (SRF).

fSRF = 1 / (2π√(LCparasitic))

Above the SRF, the inductor behaves like a capacitor! Always check that your operating frequency is well below the SRF.

Saturation Current

Inductors with magnetic cores can saturate when the magnetic field becomes too strong. At saturation:

  • Inductance drops dramatically
  • Core may overheat
  • Circuit performance degrades

Always check the inductor's saturation current (Isat) rating—the current at which inductance drops by 10-30%. Air core inductors don't saturate.

DC Resistance (DCR)

The DC resistance of the wire winding causes power loss.

Ploss = I² × DCR

Higher inductance coils typically have more turns → more resistance → more loss. Choose an inductor with DCR appropriate for your current level.

Common Applications

Application Typical Range Purpose
RF matching networks 1-100 nH Impedance matching at GHz frequencies
LC oscillators 1 nH - 1 µH Frequency generation in RF circuits
EMI filters 1-100 µH Suppress high-frequency noise
Buck/Boost converters 1-100 µH Energy storage and voltage conversion
Audio crossovers 0.1-10 mH Frequency-dependent speaker routing
Power line filters 1-100 mH 50/60 Hz noise suppression
Power transformers 1-1000 H Voltage transformation, isolation

Lenz's Law

Lenz's Law states that the induced voltage always opposes the change in current. This is why:

  • Current through an inductor cannot change instantaneously
  • Sudden disconnection creates a voltage spike (back-EMF)
  • Inductors "smooth out" current changes
  • Flyback diodes are needed when switching inductive loads

Time Constant (τ)

In an RL circuit (resistor + inductor), the time constant describes how quickly current changes.

τ = L / R

After time τ, current reaches 63% of its final value. After 5τ, it's essentially at steady state (99%).


Most Common Conversions

Conversion Example Result
Henries to Microhenries (H to µH) 1 H = 1,000,000 µH
Microhenries to Henries (µH to H) 1,000,000 µH = 1 H
Microhenries to Millihenries (µH to mH) 1,000 µH = 1 mH
Millihenries to Microhenries (mH to µH) 1 mH = 1,000 µH
Webers per Ampere to Henries (Wb/A to H) 1 Wb/A = 1 H (equivalent by definition)
Henries to Webers per Ampere (H to Wb/A) 1 H = 1 Wb/A (equivalent by definition)

Quick Reference Cards

SI Unit
1 H = 1 Wb/A = 1 V·s/A
1 mH = 0.001 H
1 µH = 0.000001 H
Henry - standard inductance unit
Common Conversions
1 H = 1,000 mH
1 mH = 1,000 µH
1 µH = 1,000 nH
Powers of 1,000 between units
Voltage-Current Relationship
V = L × (dI/dt)
Opposes current change
Lenz's Law applies
Faraday's Law of Induction
Energy Storage
E = ½ L I²
Stored in magnetic field
Released when current drops
Inductor energy formula

Typical Inductance Values

PCB Trace
≈ 1-20 nH
≈ 0.001-0.02 µH
Per cm of trace, parasitic
RF Chip Inductor
≈ 10-100 nH
≈ 0.01-0.1 µH
High-frequency circuits
SMD Inductor
≈ 1-100 µH
≈ 0.001-0.1 mH
Surface-mount components
Power Supply Choke
≈ 100 µH - 10 mH
≈ 0.1-10 mH
DC-DC converters, filtering
Audio Crossover
≈ 1-10 mH
≈ 0.001-0.01 H
Speaker frequency separation
Power Transformer
≈ 1-100 H
≈ 1,000-100,000 mH
50/60 Hz power applications

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