Chassis and suspension design: Difference between revisions

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== References ==
== References ==
<references />
 
== References ==
* [https://www.fia.com/regulation/category/110 FIA Regulations Hub]
== References ==
* [https://www.fia.com/sites/default/files/fia_2025_formula_1_technical_regulations_-_issue_01_-_2024-12-11_1.pdf 2025 FIA Technical Regulations (Issue 01)]
* FIA (2025). 2025 Formula 1 Technical Regulations (Issue 01). https://www.fia.com/sites/default/files/fia_2025_formula_1_technical_regulations_-_issue_01_-_2024-12-11_1.pdf
* [https://api.fia.com/system/files/documents/fia_2025_formula_1_sporting_regulations_-_issue_4_-_2025-02-26.pdf 2025 FIA Sporting Regulations (Issue 4)]
* FIA (2025). 2026 Formula 1 Regulations — Section C: Technical Regulations (Issue 12). https://api.fia.com/system/files/documents/fia_2026_f1_regulations_-_section_c_technical_-_iss_12_-_2025-06-10.pdf
* [https://www.fia.com/sites/default/files/fia_2026_formula_1_technical_regulations_issue_8_-_2024-06-24.pdf 2026 FIA Technical Regulations (Issue 8)]
* Milliken, W. F., & Milliken, D. L. (1995). *Race Car Vehicle Dynamics*. SAE International. ISBN 978-0768001216
* [https://www-control.eng.cam.ac.uk/foswiki/pub/Main/MalcolmSmith/cued_control_859.pdf Smith (2002): “Synthesis of Mechanical Networks: The Inerter” — IEEE (author PDF)]
* Park, J., Guenther, D., & Heydinger, G. (2003). “Kinematic Suspension Model Applicable to Dynamic Full Vehicle Simulation.” *SAE Technical Paper* 2003-01-0859. https://saemobilus.sae.org/papers/kinematic-suspension-model-applicable-dynamic-full-vehicle-simulation-2003-01-0859  (doi:10.4271/2003-01-0859)
* [https://asmedigitalcollection.asme.org/dynamicsystems/article-pdf/131/1/011001/5493020/011001_1.pdf Papageorgiou & Smith (2009): “Experimental Testing and Analysis of Inerter Devices” — ASME PDF]
* Edara, R. (2004). “Effective Use of Multibody Dynamics Simulation in Vehicle Development.” *SAE Technical Paper* 2004-01-1547. https://www.sae.org/publications/technical-papers/content/2004-01-1547/  (doi:10.4271/2004-01-1547)
* [https://ep.liu.se/ecp/124/004/ecp16124004.pdf Sundström (2016): “Virtual Vehicle Kinematics & Compliance Test Rig” Modelica Conference PDF]
* Singh, R. (2005). “A Downforce Optimization Study for a Racing Car Shape.” *SAE Technical Paper* 2005-01-0545. https://www.sae.org/publications/technical-papers/content/2005-01-0545/  (doi:10.4271/2005-01-0545)
* [https://publications.lib.chalmers.se/records/fulltext/219391/219391.pdf Danielsson (2014): “Influence of Body Stiffness on Vehicle Dynamics” — Chalmers PDF]
* Smith, M. C. (2002). “Synthesis of Mechanical Networks: The Inerter.” *IEEE Trans. Automatic Control*, 47(10), 1648–1662. https://www-control.eng.cam.ac.uk/foswiki/pub/Main/MalcolmSmith/cued_control_859.pdf (doi:10.1109/TAC.2002.803532)
* [https://www.sae.org/publications/technical-papers/content/2003-01-0859/ Park et al. (2003): “Kinematic Suspension Model Applicable to Dynamic Full Vehicle Simulation” — SAE]
* Papageorgiou, C., & Smith, M. C. (2009). “Experimental Testing and Analysis of Inerter Devices.” *ASME J. Dynamic Systems, Measurement, and Control*, 131(1), 011001. https://asmedigitalcollection.asme.org/dynamicsystems/article/131/1/011001/466043  (doi:10.1115/1.2969253)
* [https://search.worldcat.org/title/Race-car-vehicle-dynamics/oclc/31288484 Milliken & Milliken (1995): ''Race Car Vehicle Dynamics'' — WorldCat record]
* Sundström, P. (2016). “Virtual Vehicle Kinematics and Compliance Test Rig.” *1st Japanese Modelica Conference*. https://ep.liu.se/ecp/124/004/ecp16124004.pdf
* Danielsson, O. (2014). *Influence of Body Stiffness on Vehicle Dynamics Modeling and Validation*. Chalmers University of Technology. https://publications.lib.chalmers.se/records/fulltext/219391/219391.pdf
* Singh, K. B. (2019). “Literature Review and Fundamental Approaches for Vehicle and Tire State Estimation.” *Vehicle System Dynamics*, 57(10), 1463–1512. https://www.tandfonline.com/doi/abs/10.1080/00423114.2018.1544373  (doi:10.1080/00423114.2018.1544373)
* Miloradović, D. (2022). “Identification of Vehicle System Dynamics from the Aspect of Steering–Suspension Interaction.” *Machines*, 10(1), 46. https://www.mdpi.com/2075-1702/10/1/46  (doi:10.3390/machines10010046)
* Multimatic. “DSSV Damping Technology (motorsport applications).” https://www.multimatic.com/motorsports/multimatic-racing-dampers
* Morse Measurements. “A Case Study in K&C Testing.” https://www.morsemeasurements.com/a-case-study-in-kc-testing/


[[Category:Chassis Design]]
[[Category:Chassis Design]]

Latest revision as of 06:16, 6 August 2025

Formula One chassis and suspension design defines the vehicle’s mechanical grip envelope, vertical load control, and its interaction with aerodynamic structures. The system is not merely structural; it governs pitch, ride, and roll behaviour under aerodynamic and tyre-dominated force regimes at frequencies up to 20 Hz.

Advanced design must account for:

  • Torsional and bending stiffness of the monocoque
  • Multibody suspension kinematics and compliance
  • Ride height–aerodynamic coupling in ground-effect flows
  • Inerter-tuned heave response
  • Tyre load sensitivity and contact patch stability

Torsional Rigidity and Structural Dynamics[edit | edit source]

Torsional stiffness is critical for preserving kinematic integrity. Twist under cross-axle torque alters suspension angles and misaligns aerodynamic reference planes.

Where:

  • = applied torque (Nm)
  • = angular displacement (rad)

Benchmark targets: - F1 monocoque: ≥ 35,000 Nm/deg - Deviations under load: < 0.1° at 3.5 kNm - GP2 monocoques: ~18,000–22,000 Nm/deg

Typical FIA torsional test uses a load fixture with two lateral beams at front and rear bulkheads. Displacement is measured with ±0.01 mm tolerances.

Suspension Kinematics and Load Vector Decomposition[edit | edit source]

All teams use double wishbone suspension at each corner. Rod orientation, pivot height, and triangle length define instantaneous centres and vertical load reaction geometry.

Anti-Dive Model[edit | edit source]

During braking, the front suspension compresses due to weight transfer. Anti-dive resists this using suspension geometry.

Where:

  • = vertical distance from ground to Instantaneous Centre (typically 120–150 mm)
  • = CG height (~310 mm for 2024 cars)
  • = longitudinal deceleration (1.7–2.0 g)

Effective range: 30–45% Higher values reduce pitch but can reduce front load feel and exacerbate tyre flat-spotting under longitudinal lock.

Anti-Squat[edit | edit source]

Applied at the rear to limit squat under traction. Geometry is defined similarly, with slightly reduced height leverage.

Typical value range: 20–30% Measured via pitch rate differential at 80% throttle, 3rd gear, with DRS closed.

Ride Height Sensitivity and Platform Control[edit | edit source]

2022–2025 F1 cars exploit floor-generated downforce via venturi tunnels. Platform control is critical for diffuser efficiency and vortex sealing.

Static targets:

  • Front ride height: 25–30 mm
  • Rear ride height: 45–55 mm
  • Rake: 1.5° (Red Bull), <1.0° (Mercedes)

Aero model output (CFD correlation):

Change Aero Impact
+1 mm front ride height –0.8% downforce, +1.4% balance rearward
+1° pitch forward –2.2% aero balance forward, +3% yaw sensitivity
+2 mm heave stroke mid-corner diffuser stall risk ↑ 18%

Teams simulate with pitch-sweep and heave oscillation modes under fuel load variation and rear wing DRS closure. 1 mm pitch instability can cause >0.1s/lap penalty on aero-sensitive tracks (e.g., Silverstone).

Inerter Systems and Heave Mode Response[edit | edit source]

Inerters ("J-dampers") generate force as a function of vertical acceleration:

Where:

  • = inertance (kg), usually 3.5–6.5 kg
  • = suspension vertical acceleration

Heave resonance tuning targets:

  • Frequency: 9–13 Hz (above floor oscillation frequency)
  • RMS displacement: <2.5 mm at max velocity (60 mm/s)
  • Damping ratio (ζ): 0.65–0.75 for vertical critical damping

Disallowed if hydraulically linked across axles under 2016–2021 FIA interpretations.

Tyre Load Sensitivity and Vertical Compliance[edit | edit source]

Suspension compliance affects contact patch consistency. Tyre grip scales with vertical load until saturation, but lateral grip is highly load-sensitive.

Where:

  • = load sensitivity coefficient (0.07–0.12)
  • = load variation

Target load variation over a lap:

- High-load corner (e.g., Copse): ΔFz < 8% peak-to-peak

- Kerb strike (e.g., Monza T1): 3–5 mm damper compression, 20–25 g peak shock

Suspension Compliance and K&C Mapping[edit | edit source]

K&C rigs measure hardpoint movement under applied loads.

Parameter Target Value Comments
Toe compliance < 0.08°/kN lateral Controls oversteer/understeer behaviour during cornering loads
Bump steer gradient ~0.12° per 10 mm bump Affects stability and steering response at high slip angles
Roll centre migration < 2 mm/° roll Maintains aero platform and balance during lateral loading
Camber gain ~0.2° per 25 mm compression Preserves tyre contact patch under heave and roll
Compliance steer < 0.05°/kN lateral Ensures predictable handling at 3–5 g lateral acceleration
Scrub radius 10–15 mm Influences steering feedback and kickback under braking
Caster trail 18–22 mm Governs self-aligning torque and yaw sensitivity

Simulation and Rig Validation Process[edit | edit source]

Development cycle:

  • Geometry defined in CAD → kinematic hardpoint solver
  • Simpack/Dymola model for transient lap input simulation
  • K&C test rig used to validate:
 - Vertical displacement vs load
 - Bump steer & toe curve
 - Roll gradient under 2g cornering
  • 7-post rig simulation:
 - Damper settings for energy control
 - Ride energy profile from full lap replay

Track correlation:

  • Laser ride height sensors at all corners
  • Linear poten

tiometers on dampers

  • Infrared tyre surface sensors

Further Reading[edit | edit source]

References[edit | edit source]