Introduction: A 200A relay can turn a 1mΩ contact resistance into real heat; this guide follows current, resistance, and time to explain the effect.
When an electrical design engineer first sees a contact resistance rating of ≤1mΩ, it can look too small to matter. A milliohm is easy to dismiss next to a 200A current rating. But high current changes the scale: the same tiny resistance that is harmless at a few amps becomes a steady heat source at hundreds of amps. The useful way to understand a 200A high voltage relay is to follow the load current through the contact interface, watch the power loss, and then see how time, terminals, and cooling decide the actual temperature rise. The focus stays on that cause-and-effect chain and separates it from coil power, which is a different circuit with a different job.
Why Contact Resistance Turns Into Heat in High Current Paths
Every closed contact still has resistance. Two metal surfaces never touch over their full apparent area; they meet at microscopic high points, and current squeezes through those small spots. That squeezing is called constriction resistance, and it sits in series with the load current. Surface films, oxide layers, and the quality of the contact interface add to the effect. At low current the voltage drop is tiny, so the heat is negligible. At 200A the same interface carries a much denser current, and the local resistance becomes a real power loss. The contact is not a perfect switch; it is a short, narrow bridge in a high current path.
1. Joule Heating Scales With Current Squared and Resistance
The basic relationship is P = I²R. Power loss rises with the square of current and in direct proportion to resistance. At 1mΩ and 100A, the contact path produces 10W as a worst-case calculation from the maximum resistance specification. At 200A, the same 1mΩ produces 40W. Doubling the current quadruples the heat. That is why a rating that looks negligible on paper becomes a design issue in a 200A relay. The heat is concentrated near the contact spots, then spreads into the contact bridge, terminals, busbars, and housing. Joule heating is power; temperature rise is the result of that power flowing through a thermal path over time. A short pulse may be absorbed by thermal mass, while a long or repeated load lets the temperature settle toward a higher steady state.
2. Contact Resistance Is Separate From Coil Power Loss
The coil and the contacts are different circuits. The coil converts electrical energy into a magnetic field that pulls the contact mechanism closed. In the YongNeng YE706 example, the coil power is DC 3W. That 3W is coil heat, and it exists whenever the coil is energized, whether the load current is zero or 200A. The contact path loss depends on load current and contact resistance; at 200A and 1mΩ, the worst-case contact loss is about 40W. Low contact resistance does not reduce coil power, and coil temperature tells you little about the contact-path temperature. The two heat sources share a package and can warm each other, but they come from different electrical paths and should be calculated separately.
Why Milliohm Ratings Matter at 200A
A 1mΩ maximum contact resistance is a small number, but at 200A it sets a clear power-loss scale. The calculation is simple: 200A squared is 40,000A², and 40,000A² × 0.001Ω = 40W. That figure is an electrical loss estimate; actual temperature rise depends on the thermal path. The actual contact resistance can be lower, and the heat does not stay inside the contact spot. It spreads through metal terminals and busbars, which have their own resistance and their own temperature coefficient. Most conductor metals increase resistivity as they get hotter, so a warm contact path can have slightly higher resistance than a cold one, which adds a small feedback effect. The design question is therefore not only “what is the contact resistance? ” but “how much current flows, for how long, and where does the heat go? ” The difference between maximum switching current and rated resistive load matters here. The YE706 lists a 200A maximum switching current and a 100A/1000VAC resistive load rating. The 200A figure describes the switching capability limit; the 100A/1000VAC figure describes a resistive load condition. A designer should not read 200A as a continuous current rating or assume that a 200A switching event and a 100A continuous load produce the same temperature rise. Contact loss at 100A with 1mΩ is about 10W, while the 200A case is 40W. That four-to-one difference is the reason current level, load profile, and duty cycle belong in the same discussion as the milliohm rating.
Reading a 1mΩ Rating Against Real Current and Duty Cycle
A contact resistance specification becomes useful when it is placed against the real current waveform. Continuous current, short overloads, motor starting, capacitor charging, and repetitive switching all create different heating patterns. A relay that looks comfortable in a brief 200A event may run much hotter in a long 100A load if the terminals are undersized or the enclosure traps heat. The contact path is only one part of the thermal network. Terminal screws, PCB traces, busbar joints, wire lugs, ambient temperature, airflow, and mounting orientation all change how quickly heat leaves the relay. That is why a single temperature-rise number without test conditions would be misleading; the practical engineering approach is to calculate the loss, then evaluate the thermal path. Time is the other half of the story. Joule heating is instantaneous, but temperature rise is not. A short pulse raises the contact temperature a little and then the heat spreads into the surrounding metal. A repeated pulse train can build heat if the off time is too short for the thermal mass to recover. A continuous load drives the path toward a steady state where heat generation equals heat removal. For a 200A-class relay, the practical reading of ≤1mΩ is this: it is a maximum specification, not a guaranteed field measurement, and it gives a worst-case loss estimate that helps compare current levels and duty cycles. The design should leave margin for terminal resistance, contact aging, ambient heat, and enclosure conditions rather than treating the milliohm figure as the whole thermal answer.
Conclusion
Contact resistance becomes heat through a simple chain: load current flows through a small contact interface, resistance creates P = I²R loss, and time plus the thermal path decide the temperature rise. At 200A, a 1mΩ maximum contact resistance corresponds to about 40W of worst-case contact loss; at the 100A/1000VAC resistive rating, it is about 10W. Those numbers explain why milliohm ratings deserve attention in high current relay circuits. They also show why the coil’s DC 3W power is a separate matter. Designers get the clearest picture by calculating contact loss from the actual current profile, then checking terminals, ambient, cooling, and duty cycle as one thermal system.
FAQ
Q: Why does 1mΩ contact resistance matter at 200A?
A: Because power loss follows I²R. At 200A, 1mΩ gives 40W of worst-case contact-path loss, which is large enough to affect temperature rise and terminal design. At lower current the same resistance produces much less heat, so the 200A case is where the milliohm value becomes visible.
Q: Does low contact resistance mean the relay coil runs cooler?
A: No. The coil is a separate circuit that consumes power to create a magnetic field. The YE706 lists DC 3W coil power, and that heat is present whenever the coil is energized. Contact resistance affects the load path, not the coil circuit, so a low-resistance contact does not by itself reduce coil temperature.
Q: How is contact resistance different from coil power consumption?
A: Contact resistance is a property of the closed load path, and its loss depends on load current squared. Coil power consumption is the power used by the coil to actuate the relay, and it depends on coil voltage and coil resistance. In the YE706 example, the coil is rated at DC 3W, while a 200A load through 1mΩ would create about 40W of worst-case contact loss.
Sources / References
Resistivity and Conductivity - Temperature Coefficients Common Materials
Relay Switch Circuit and Types of Relay Switching Circuits