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This article summarizes the essential elements of SAE J212-2008, a recommended practice that establishes a uniform laboratory dynamometer method for testing passenger car brake systems. Although the document has been cancelled and replaced by SAE J2784, its procedures remain a foundational reference for evaluating brake system performance, including deceleration versus input, system integrity, and stopping ability under emergency or power-assist failure.
The standard applies to all classes of passenger car brakes and requires specific equipment to simulate real-world conditions:
Accurate measurement and recording are vital. Required instruments include recording devices for hydraulic line pressure, brake torque, lining temperature, and shaft speed, as well as cooling air temperature indicators and a revolutions-to-stop indicator for equivalent stopping distance. Optional instruments include cooling air velocity indicators, drum/disc temperature recorders, fluid displacement indicators, and stopping time indicators.
To ensure data quality, the overall system accuracy for recording or indicating instruments must be ±2% of full-scale or better. Control parameters must meet the following tolerances:
| Parameter | Tolerance |
|---|---|
| Line pressure, torque, temperature | ±5% of desired value |
| Speed | ±2% of desired value |
| Test moment of inertia | ±2.03 kg·m² (±1.5 slug·ft²) of calculated value |
Brake drums or discs should be new and within manufacturer specifications. Plug-type thermocouples are installed per SAE J79 at the center of the most heavily loaded shoe, one per brake, to capture representative lining temperatures.
Calculation of Test Moment of Inertia: The moment of inertia required to simulate the vehicle is calculated as I = (W × r²) / (2g), where W is the vehicle test weight (normally curb weight + 2669 N (600 lb)) multiplied by 0.86 to account for parasitic losses, r is the effective tire radius, and g is gravity (9.8 m/s² or 32.2 ft/s²). Test rpm is derived from rpm = (22.56 × km/h) / r or rpm = (14.02 × mile/h) / r, and deceleration is converted to torque using T = (W × r × a) / (2g).
The test sequence includes multiple phases to evaluate brake performance under varying conditions. The table below summarizes key parameters for each major phase.
| Test Phase | Stop Speed | Deceleration | Initial Temp | Number of Stops | Cycle |
|---|---|---|---|---|---|
| Preburnish Check | 48.3 km/h | 3.05 m/s² | Any | 10 | 90 s |
| First Effectiveness | 48.3, 96.6 km/h | Variable | 93 °C | Multiple increments | — |
| Burnish | 64.4 km/h | 3.7 m/s² | ≤121 °C | 200 | ≤90 s |
| High-Speed Stop | Up to 160.9 km/h | 4.6 m/s² | 66 °C | 1 | — |
| First Fade | 96.6 km/h | 4.6 m/s² | 66 °C | 10 | 35 s |
| Recovery | 48.3 km/h | 3.1 m/s² | — | 12 | 2 min |
| Emergency/No-Power | 96.6 km/h | Constant pressure | 66 °C | As needed | — |
Throughout all phases, unusual performance characteristics (noise, roughness) must be recorded. Cooling air speeds must be controlled to produce temperatures normally experienced on the specific vehicle, with calibration based on baseline vehicle data.
It compensates for parasitic losses that absorb energy in a real vehicle (e.g., drivetrain friction, tire rolling resistance). Without it, the dynamometer would overestimate the inertia the brakes must absorb, leading to unrealistic loading.
Per SAE J79, plug-type thermocouples are installed at the approximate center of the most heavily loaded brake shoe, one per brake. This location provides a representative lining temperature relative to the high-energy zone and ensures consistent readings across tests.
Pressure, torque, and temperature must be within ±5% of desired; speed within ±2%; and inertia within ±2.03 kg·m² of the calculated value. Instrument accuracy must be ±2% of full-scale or better. Adhering to these tolerances is essential for repeatable and comparable results.