Ohmic Audio

⚙️ ENGINEER LEVEL: Acoustic Optimization Theory

Cabin Transfer Function Modeling

The vehicle cabin is not a rigid piston but a complex resonant cavity. The transfer function from driver volume velocity to cabin pressure involves:

Modal analysis — each cabin dimension supports standing wave modes:

f_lmn = (c/2) × √[(l/Lx)² + (m/Ly)² + (n/Lz)²]

For a sedan (Lx=1.2m, Ly=1.5m, Lz=4.0m interior dimensions):

f_100 = (343/2) × (1/1.2) = 143 Hz (width mode)
f_010 = (343/2) × (1/1.5) = 114 Hz (height mode)
f_001 = (343/2) × (1/4.0) = 43 Hz (length mode)

At 40-50 Hz, the wavelength (7-8.5m) is longer than cabin length. The cabin pressurizes uniformly — this is ideal for SPL. No nodes or antinodes to worry about. Pure pressure gain.

Cabin gain formula (simplified for low frequencies):

G_cabin = 10 × log₁₀[(4π × V_cabin) / λ²]

At 50 Hz, λ = 6.86m, V_cabin = 3 m³:

G_cabin = 10 × log₁₀[(4π × 3) / 6.86²] = 10 × log₁₀(0.801) = -0.96 dB

Wait, that's a loss, not gain. Let me reconsider the cabin gain model.

Correct approach — pressure doubling from boundary loading:

In a sealed cabin at frequencies well below first mode, pressure increases because the air cannot escape. The effective radiation impedance seen by the driver increases, causing more mechanical-to-acoustic power conversion.

Practical cabin gain: 10–20 dB depending on vehicle size and sealing quality. Smaller, well-sealed vehicles exhibit more gain.

Thermal Power Compression in Competition

Voice coil temperature during burping:

Assume 15-second burp at 10,000W into a driver with Re = 1Ω (cold).

Power dissipation in voice coil:

P_heat = I² × Re = (√(10000/1))² × 1 = 10,000W

All 10,000W becomes heat in the voice coil (100% conversion to thermal at DC and low frequencies).

Temperature rise (using thermal mass of typical 3" voice coil):

Thermal mass ≈ 50 J/°C (aluminum former, copper wire)

ΔT = (P × t) / C_thermal = (10000 × 15) / 50 = 3000°C theoretical

Obviously impossible — the coil would vaporize. What actually happens:

  1. Voice coil heats rapidly to 300-500°C
  2. Resistance increases (Rhot = Rcold × [1 + α×ΔT])
  3. Current decreases for same voltage
  4. Power decreases (power compression)
  5. After ~5-10 seconds, thermal equilibrium at reduced power

Competition strategy: Burp duration kept under 15 seconds. Cooling between runs (forced air, liquid cooling on extreme builds).

Liquid-cooled voice coils (exotic competition tech):

Some championship builds use subwoofers with hollow voice coil formers. Coolant (water or glycol) circulates through the former, removing heat directly. Allows sustained high power. Adds complexity and cost.


13.2 Sound Quality Competition Strategy