The metal with the lowest electrical resistivity at room temperature is silver ($1.59 \times 10^{-8} \Omega\cdot m$), but copper ($1.68 \times 10^{-8} \Omega\cdot m$ for pure, $1.72 \times 10^{-8} \Omega\cdot m$ for standard ETP) is the definitive practical choice for 95% of electrical wiring due to its superior cost-to-conductivity ratio. When sizing wire or designing traces, relying solely on a 20°C baseline chart will result in undersized conductors for real-world operating temperatures. You must apply temperature derating to the base resistivity value to calculate true voltage drop and ampacity limits.
The Resistivity of Metals Chart (20°C Baseline)
The following table provides the baseline DC resistivity for common electrical metals. Source Standard: Values are aligned with ASTM B193 (Standard Test Method for Resistivity of Electrical Metallic Materials) and referenced against the International Annealed Copper Standard (IACS).
| Metal / Alloy | Resistivity ($\rho$) at 20°C ($\Omega\cdot m \times 10^{-8}$) |
Conductivity (% IACS) |
Temp Coefficient ($\alpha$) per °C |
Primary Application |
|---|---|---|---|---|
| Silver (Pure) | 1.59 | 105% | 0.0038 | RF contacts, aerospace, high-end audio |
| Copper (Pure / OFHC) | 1.68 | 102% | 0.00393 | PCB traces, magnet wire, precision shunts |
| Copper (ETP / Standard) | 1.72 | 100% | 0.00393 | THHN/NM-B building wire, busbars |
| Gold (Pure) | 2.44 | 70% | 0.0034 | Corrosion-proof edge connectors, IC bonding |
| Aluminum (Pure) | 2.65 | 61% | 0.00429 | High-voltage transmission lines |
| Aluminum (AA-8000 Series) | 2.85 | 57% | 0.00400 | NEC-compliant branch/feeder building wire |
| Tungsten | 5.60 | 31% | 0.0045 | Incandescent filaments, high-temp probes |
| Nichrome 80 (80% Ni, 20% Cr) | 110.0 | 1.5% | 0.0004 | Toaster elements, 3D printer hotends, dummy loads |
How to Read This Table
The Resistivity ($\rho$) column is your raw physics value, measured in ohm-meters. For practical wire math, you will usually convert this to ohms per circular mil-foot or ohms per 1000 feet based on AWG cross-sections. The % IACS column is the industry shorthand for conductivity; standard annealed copper is defined as exactly 100% IACS. If a material is 61% IACS (like pure aluminum), it means it has 61% of the conductance of standard copper, requiring a larger cross-sectional area to carry the same current. The Temp Coefficient ($\alpha$) is the multiplier used to adjust the baseline resistivity when the conductor heats up under load.
Applying Temperature Derating to Base Values
A common mistake on the workbench and in CAD software is using the 20°C resistivity value to calculate voltage drop for a wire that will actually operate at 60°C or 75°C. As a metal heats up, atomic lattice vibrations increase, scattering electrons and raising resistance.
To find the true operating resistivity ($\rho_T$), use this formula:
$\rho_T = \rho_{20} \times [1 + \alpha(T - 20)]$
Worked Example: 12 AWG Copper at 75°C
Suppose you are running a 12 AWG ETP copper branch circuit in a hot attic, and the terminations are rated for 75°C.
- Baseline: 12 AWG copper at 20°C is 1.588 $\Omega$ / 1000 ft.
- Temp Coefficient ($\alpha$): 0.00393 (from the chart above).
- Delta T: $75°C - 20°C = 55°C$.
- Calculation: $1.588 \times [1 + (0.00393 \times 55)] = 1.588 \times 1.216 = $ 1.93 $\Omega$ / 1000 ft.
Bench Insight: If you sized your wire based on the 20°C chart (1.588 $\Omega$), your calculated voltage drop would be nearly 18% lower than reality. Always use the 75°C or 90°C column from NEC Table 310.16 for ampacity, and derate your resistivity math to match that same temperature ceiling.
Decision Tree: Which Metal for Your Installation?
Use this decision path to terminate your material selection. Do not default to 'it depends'—match your specific physical constraints to the concrete pick below.
| If your primary constraint is... | And the environment is... | Then your concrete pick is... |
|---|---|---|
| High-Frequency RF / Skin Effect | Aerospace, ham radio, or high-end audio interconnects where surface conductivity dictates signal loss. | Silver-plated copper wire (e.g., MIL-W-16878 / PTFE insulated). Pure silver is too soft; plating gives the RF surface benefit with copper's tensile strength. |
| Standard Branch Circuits / Mains | Residential or commercial walls, conduit, NM-B, or THHN in standard ambient temperatures. | ETP Copper (THHN/THWN-2). It is the undisputed baseline. Size according to NEC 310.16 75°C column. |
| Heavy Feeders / Weight & Cost | Service entrance conductors, long underground feeder runs (200A+), where copper cost or weight is prohibitive. | AA-8000 Series Aluminum (XHHW-2). Never use pure aluminum for building wire. Size exactly two AWG sizes larger than the equivalent copper (e.g., 2/0 Al for 100A instead of 3 AWG Cu). |
| Intentional Heat Generation | Toasters, 3D printer hotends, kiln elements, or high-wattage dummy loads. | Nichrome 80 (80% Ni, 20% Cr). Its high resistivity (110 $\times 10^{-8} \Omega\cdot m$) and stable $\alpha$ prevent thermal runaway and oxidation at red-hot temperatures. |
| Corrosion Resistance / Micro-Signals | Low-voltage edge connectors, PCB contacts, or marine environments where copper oxide would cause data errors. | Gold-flashed contacts (minimum 30 $\mu$in thickness). Gold does not oxidize, ensuring reliable low-current mating cycles. |
What This Chart Cannot Tell You (The Blind Spots)
A DC resistivity chart is a physics baseline, not a complete engineering specification. Here is what the numbers above hide:
1. The AC Skin Effect
This chart lists DC resistivity. At 60 Hz (mains power), the skin effect in standard AWG wire is negligible. However, at high frequencies (e.g., 100 kHz+ in switch-mode power supplies or RF transmitters), current migrates to the outer skin of the conductor. The effective cross-sectional area shrinks, drastically increasing AC resistance. For high-frequency builds, you must use Litz wire or hollow copper tubing, regardless of the base DC resistivity.
2. Alloy Impurities and Mechanical Creep
The chart lists 'Pure Aluminum' at 2.65 $\times 10^{-8} \Omega\cdot m$. But pure aluminum (1350 series) suffers from severe mechanical creep and galvanic oxidation at screw terminals, which historically caused house fires. Modern electrical codes require AA-8000 series aluminum alloys. These alloys add trace iron and copper to stop creep, but they slightly increase resistivity to ~2.85 $\times 10^{-8} \Omega\cdot m$. Always use the alloy value for voltage drop calculations, not the pure metal value.
3. Contact Resistance
Resistivity measures the bulk material. It does not account for the micro-ohms of resistance introduced at a crimp, a solder joint, or a mechanical lug. A poorly torqued aluminum lug will introduce more resistance than 50 feet of the wire itself. Always follow manufacturer torque specs (e.g., 25 in-lbs for a standard 12 AWG copper terminal).
Quick-Jump Reference: The Most Queried Metals
Bookmark this section for fast lookups when ordering materials or debugging a circuit.
- Copper (ETP): The 100% IACS baseline. $\rho = 1.72 \times 10^{-8} \Omega\cdot m$. Use for 99% of DIY electronics, home wiring, and motor windings. If you are unsure, use copper.
- Aluminum (AA-8000): $\rho = 2.85 \times 10^{-8} \Omega\cdot m$. Use strictly for heavy feeders (>100A) to save money and weight. Requires anti-oxidant paste (Noalox) and specific AL/CU rated lugs.
- Silver: $\rho = 1.59 \times 10^{-8} \Omega\cdot m$. Only 6% more conductive than copper but 50x more expensive. Justifiable only for RF skin-effect plating or critical aerospace contacts.
- Nichrome 80: $\rho = 110 \times 10^{-8} \Omega\cdot m$. The standard for heating. If you need a 10-ohm heating element, you need a very long, thin piece of copper, but just a short, manageable coil of Nichrome.
For further reading on standard testing methods and material properties, consult the Georgia State University HyperPhysics wire properties database or review the NEC Chapter 9, Table 8 for the practical translation of these resistivity values into AWG ohms-per-thousand-feet.






