The units of electrical resistance quantify how strongly a material opposes the flow of electric current, with the ohm (Ω) serving as the base SI unit. If you picture electricity like water flowing through a plumbing system, resistance is the equivalent of a narrowed pipe: the narrower the pipe (higher resistance), the harder the pump (voltage) must work to push the same volume of water (current) through it. While the ohm is the standard baseline, real-world electronics and electrical installations require us to scale this unit across several orders of magnitude—from the microohms of a copper busbar to the megaohms of motor winding insulation.
The Core Units of Electrical Resistance
According to the National Institute of Standards and Technology (NIST), the ohm is defined by the fixed numerical value of the elementary charge and the Planck constant in the revised SI system. However, on the workbench, we rarely deal with exactly 1 Ω. We use metric prefixes to handle the vast range of resistive values encountered in modern design. Below is the definitive reference table for the units you will actually measure and specify.
| Unit Name | Symbol | Multiplier | Measurement Tool | Real-World Component Example |
|---|---|---|---|---|
| Microohm | µΩ | 10-6 | Micro-ohmmeter | PCB copper trace (1 oz, 10mm length) |
| Milliohm | mΩ | 10-3 | 4-wire Kelvin DMM | Battery internal ESR, current shunt resistor |
| Ohm | Ω | 100 | Standard Multimeter | LED current limiter, nichrome heater element |
| Kiloohm | kΩ | 103 | Standard Multimeter | I2C pull-up resistor, voltage divider network |
| Megaohm | MΩ | 106 | Insulation tester (Megger) | Motor winding insulation, ESD floor mat |
Worked Example: Sizing a Shunt Resistor for Current Sensing
Let’s move from theory to the workbench with a concrete numeric example. Suppose you are designing a battery management system (BMS) and need to measure a continuous 20A DC load using a microcontroller’s ADC. Your ADC has a 0–3.3V input range, but to minimize parasitic power loss and heat, you want to limit the maximum voltage drop across your shunt resistor to 100mV (0.1V) at peak current.
Step 1: Calculate the Required Resistance
Using Ohm’s Law (R = V / I):
- R = 0.100V / 20A
- R = 0.005 Ω (or 5 milliohms)
Step 2: Calculate Power Dissipation
Now we must ensure the physical component won't melt. Using Joule’s Law (P = I²R):
- P = (20A)² × 0.005 Ω
- P = 400 × 0.005
- P = 2.0 Watts
Step 3: Component Selection and Derating
A 2W dissipation means a standard 2W resistor will run at 100% capacity, likely overheating and drifting in value due to its temperature coefficient of resistance (TCR). Engineering best practice dictates derating power resistors to at least 50% of their rated capacity. Therefore, you need a minimum 4W or 5W rated shunt resistor.
The Part: You would specify a 5mΩ, 5W metal strip shunt resistor, such as the Vishay WSL3637 or Bourns CSS series. As detailed in All About Circuits' guide on shunt design, you must layout your PCB with dedicated Kelvin sense pads located directly at the resistor's inner edges to avoid measuring the voltage drop of the PCB copper traces themselves.
Where You Meet These Units in Practice
Understanding the units of electrical resistance is only half the battle; knowing where each scale physically manifests in a system separates novices from experienced builders.
Milliohms (mΩ): The Parasitics and the Power
In power electronics, milliohms are the domain of unintended losses and intentional sensing. A typical 18650 lithium-ion cell has an internal equivalent series resistance (ESR) of about 15 to 30 mΩ when new, which climbs past 100 mΩ as it degrades. In home wiring, a 50-foot run of 12 AWG copper wire has a loop resistance of roughly 160 mΩ. While that sounds tiny, pushing 20A through it results in a 3.2V drop and 64W of heat dissipated inside your walls—exactly why NEC-style voltage drop calculations matter for long feeder runs.
Ohms (Ω) and Kiloohms (kΩ): Signal Control and Logic
This is the comfort zone for most hobbyists. You use ohms to limit current to an LED (e.g., a 220 Ω resistor for a 20mA red LED on a 5V rail). You use kiloohms to set logic states without drawing excessive current. An I2C bus, for instance, requires pull-up resistors to hold the SDA and SCL lines high. A standard value is 4.7 kΩ, which provides enough current to overcome bus capacitance for fast rise times, but limits the sinking current when a device pulls the line low to just over 1mA.
Megaohms (MΩ): Isolation and Safety
When resistance reaches the megaohm scale, we are no longer controlling current; we are preventing it from flowing where it shouldn't. According to Fluke's insulation testing guidelines, a healthy 120V/240V residential branch circuit should exhibit an insulation resistance of at least 1 MΩ (and ideally >50 MΩ) between the current-carrying conductors and the equipment grounding conductor when tested with a 500V or 1000V Megger. If a motor winding reads 0.5 MΩ, the dielectric insulation is breaking down, and the motor is a shock hazard waiting to fail.
Common Confusions: Resistance vs. Resistivity vs. Impedance
When discussing the units of electrical resistance, people frequently conflate three distinct but related concepts. Clearing up these confusions will save you from critical design errors.
| Concept | Unit | Definition | What People Get Wrong |
|---|---|---|---|
| Resistance (R) | Ohms (Ω) | The total opposition to DC current flow of a specific physical object. | Assuming a material is inherently 'high resistance' without considering its physical dimensions. |
| Resistivity (ρ) | Ohm-meters (Ω·m) | An intrinsic material property defining how strongly a bulk material opposes current. | Confusing the material property (copper's resistivity) with the object property (a copper wire's resistance). |
| Impedance (Z) | Ohms (Ω) | The total opposition to AC current, combining DC resistance with frequency-dependent reactance. | Measuring a speaker or motor coil with a DC multimeter (yielding 4Ω) and assuming it will draw 30A from a 120V AC source (it won't, due to inductive reactance raising the impedance to ~100Ω). |
The Geometry Factor: Why Resistivity Matters
Resistivity explains why a massive copper busbar has lower resistance than a tiny carbon film resistor, even though copper's intrinsic resistivity (1.68 × 10-8 Ω·m) is vastly lower than carbon's. Resistance is calculated as R = ρ(L/A), where L is length and A is cross-sectional area. You can make a high-resistance component out of low-resistivity copper simply by making it very long and very thin (like the fine wire inside a 10 Ω wirewound resistor).
The AC Factor: Why Impedance Trumps Resistance
In DC circuits, resistance is the only opposition you face. In AC circuits, inductors and capacitors introduce reactance (X), which shifts the phase of the current. Impedance (Z) is the vector sum of resistance and reactance (Z = √(R² + X²)). This is why an 18 AWG wire might have a DC resistance of 0.02 Ω, but at high radio frequencies (RF), the skin effect forces current to the outer edge of the conductor, effectively reducing the cross-sectional area and drastically increasing its AC impedance.






