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Speakers Guru
Installers pulling cable before drywall closes or before a door card goes back on, who need to know whether 16 AWG is enough for this specific run and this specific load.9 min read · Updated July 2026

Speaker Wire Gauge by Run Length and Load: A 5% Power-Loss Chart

Hold total round-trip wire resistance under about 5% of the load impedance and you lose 0.22 dB, which is inaudible. For a 4 ohm load that means 16 AWG stops at roughly 26 ft, 14 AWG at 42 ft and 12 AWG at 66 ft. Double all three figures for an 8 ohm home run, and cut them by a third for copper-clad aluminium.

By the Speakers Guru Editorial Team

Wire gauge arguments go in circles because nobody states the loss threshold they are arguing about. Fix it at 5% of amplifier power dumped as heat in the cable and the whole thing becomes arithmetic: keep round-trip conductor resistance below about one twentieth of the nominal load impedance.

At 4 ohms that ceiling is 0.21 ohms, which 16 AWG copper reaches at 26 ft, 14 AWG at 42 ft and 12 AWG at 66 ft. At 8 ohms every one of those numbers doubles. And here is the part that ends most of the arguments: 5% power loss is 0.22 dB. You will not hear it. What you may hear, on a long run into a low load, is what the same resistance does to damping factor.

  1. Setting the threshold before running the numbers

    Cable and driver form a voltage divider. The wire has resistance, the speaker has impedance, and they share the amplifier's output in proportion. Power reaching the driver is the load's share of the total: R_load divided by (R_load plus R_wire).

    Round-trip matters, not one-way. Current goes out on one conductor and comes back on the other, so a 25 ft run is 50 ft of copper. Halve that and every table on the internet is wrong by a factor of two, which is exactly how thin wire gets defended.

    The 5% figure is a convention, not a law of physics. It is roughly where the loss stops being measurable in any way that matters and starts being an accounting entry. Below 2% you are buying copper for reassurance. Above 10% you are heating a wall cavity with amplifier power you paid for.

  2. Round-trip resistance, gauge by gauge

    Figures below are solid annealed copper at 20 degrees C. Stranded cable runs about 2% higher because the strands take a slightly longer helical path, which is inside the noise of everything else here.

    GaugeOhms per 1000 ft10 ft run25 ft run50 ft run75 ft run100 ft run150 ft run
    18 AWG6.3850.1280.3190.6390.9581.2771.916
    16 AWG4.0160.0800.2010.4020.6020.8031.205
    14 AWG2.5250.0510.1260.2530.3790.5050.758
    12 AWG1.5880.0320.0790.1590.2380.3180.476
    10 AWG0.9990.0200.0500.1000.1500.2000.300
    All cells are total round-trip resistance in ohms for the stated one-way run length. Compare the number against 5% of your nominal load: 0.11 ohms at 2 ohms, 0.21 at 4, 0.32 at 6, 0.42 at 8.
  3. Maximum run length at the 5% line

    Same maths, turned around. Pick your load, pick your gauge, and this is where the run stops passing.

    Nominal loadResistance ceiling18 AWG16 AWG14 AWG12 AWG10 AWG
    2 ohm0.105 ohm8 ft13 ft21 ft33 ft53 ft
    4 ohm0.211 ohm16 ft26 ft42 ft66 ft105 ft
    6 ohm0.316 ohm25 ft39 ft63 ft99 ft158 ft
    8 ohm0.421 ohm33 ft52 ft83 ft133 ft211 ft
    16 ohm (100V line taps aside)0.842 ohm66 ft105 ft167 ft265 ft421 ft
    Find your load row, read across to the longest gauge that covers your run. Anything to the left of that column passes the 5% rule; anything to the right of your run length is copper you did not need to buy.

    Two things fall straight out of this table. A 4 ohm car door on 16 AWG is fine at any realistic in-vehicle length, because no door run is 26 ft. And a 2 ohm subwoofer on 18 AWG is out of budget at 8 ft, which is shorter than most boot runs.

  4. What the loss actually sounds like

    Converting percentage loss into decibels is where the folklore dies. Ten log of the surviving fraction, and the numbers are small.

    Round-trip wire resistancePower lost at 4 ohmLevel dropDamping factor at the driver
    0.05 ohm1.2%0.05 dB40
    0.10 ohm2.4%0.11 dB27
    0.20 ohm4.8%0.21 dB16
    0.40 ohm9.1%0.41 dB8.9
    0.80 ohm16.7%0.79 dB4.7
    1.60 ohm28.6%1.46 dB2.4
    Damping factor assumes an amplifier output impedance of 0.05 ohm. Read the last column, not the third: level drop stays trivial long after damping factor has collapsed.

    Below a damping factor of about 20 the amplifier stops controlling cone motion cleanly at resonance, and what you hear is a loose, one-note quality in the bottom two octaves. That is the honest reason to run heavier cable to a woofer. Not the 0.4 dB.

  5. Copper-clad aluminium costs you two gauges

    CCA is an aluminium conductor with a thin copper skin. Aluminium carries about 61% of copper's current for the same cross-section, and a typical CCA blend lands around 60 to 65%, so multiply every resistance figure above by roughly 1.55.

    That multiplier happens to be almost exactly two AWG steps. So the rule is simple and easy to remember at the counter: CCA behaves like copper two sizes thinner. Twelve gauge CCA is 14 gauge copper. Sixteen gauge CCA is 18 gauge copper.

    Marked gauge (CCA)Copper ohms/1000 ftCCA ohms/1000 ftBehaves likeMax 4 ohm run at 5%
    18 AWG CCA6.385approx 9.920 AWG copper10 ft
    16 AWG CCA4.016approx 6.218 AWG copper17 ft
    14 AWG CCA2.525approx 3.916 AWG copper27 ft
    12 AWG CCA1.588approx 2.514 AWG copper43 ft
    10 AWG CCA0.999approx 1.612 AWG copper68 ft
    If the reel does not say OFC, oxygen-free copper or 100% copper, assume CCA and read this table instead of the copper one. Weigh a 100 ft reel if you are unsure - CCA comes in at roughly a third of the weight.
  6. Where the extra copper is money burnt

    Twelve gauge to a pair of 8 ohm bookshelf speakers 12 ft away is 0.038 ohms of round-trip resistance against a 0.42 ohm budget. You used a tenth of your allowance. Fourteen would have been ten times better than necessary and sixteen would still have been five times inside the line.

    The runs that genuinely justify heavy cable are the long ones into low loads: a 2 ohm sub in a boot, a 4 ohm in-ceiling pair at the far end of a 60 ft home run, a passive PA top on a 100 ft trunk from an amp rack at the back of a hall. Those are the cases where the table above turns red, and they are also the cases where damping factor is doing something audible.

    Terminations matter more than most people expect on long runs. A dirty spade or a barely-tightened binding post can add more resistance than 20 ft of 14 gauge. Strip clean, twist tight, and if you crimp, crimp with a ratchet tool rather than pliers.

  7. Two rules the calculator does not cover

    In-wall and in-ceiling runs need cable with a CL2 or CL3 jacket rating. That is a cable listing requirement, and it applies to the low-voltage speaker run itself.

    Amplifier power leads are a different calculation entirely and do not belong on this chart. Those are sized on current draw and fused within about 18 inches of the battery terminal, and the gauge comes from the amplifier's fuse rating, not from a 5% audio loss rule.

  8. Feeding the Gauge Calculator

    Enter run length, nominal load and conductor material. Output is round-trip resistance, percentage loss, level drop in dB, resulting damping factor and a pass, marginal or fail verdict against the 5% line.

    One habit worth adopting: enter the load your amplifier will actually see, not the number on the speaker. Two 4 ohm drivers in parallel on one channel is a 2 ohm run, and that halves every length in the table above.

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