Tire–Road Interaction: A Comprehensive Review of Friction Mechanisms, Influencing Factors, and Future Challenges
Abstract
1. Introduction
2. Bibliometric and Thematic Methods
- Publications related to the automotive sector, such as those mentioned above, including research articles, review papers, conference papers, and books;
- Studies published between 1968 and 2025 to capture the latest trends and advancements;
- Studies published in English.
- Articles not specifically focused on the key research direction;
- Non-peer-reviewed works and gray literature, excluded to ensure data quality and reliability;
- Papers published in languages other than English, or outside the specified publication window.
Review Questions
3. Results
- Symmetrical patterns offer a uniform design that balances performance and longevity;
- Asymmetrical patterns combine distinct inner and outer designs, with the outer shoulder enhancing dry grip and cornering stability, while the inner shoulder improves water dispersion;
- Directional patterns, often arrow-shaped, are intended to rotate in a single direction, providing superior water evacuation and traction in snow or mud.
3.1. Tire–Road Friction Process
- The coefficient of static friction is the friction force that must be overcome to be able to determine the movement of the wheel from rest. This is usually greater than the coefficient of dynamic friction. Some references reviewed in this article are [55,56,57,58]. A semi-analytical model presented in [57] predicts the normal force distribution, while a beam–spring network captures the friction force and rubber deformation during stick-to-slip transitions.
- The dynamic friction coefficient represents the friction force that acts when a wheel slides on a surface [55,57]. In [59] a hybrid physical–dynamic tire–road friction model is presented for the simulation and control of vehicle motion, extending the LuGre dynamic friction model by incorporating a stick–slip partition based on the physical model of the contact patch.
3.2. Factors That Affect the Coefficient of Friction
3.2.1. Tire Composition and Construction
3.2.2. Road Surface
3.2.3. Temperature
3.2.4. Tire Load and Pressure
3.2.5. New Tire Production Technology
3.3. Tire–Road Interactions Models and Methods
4. Discussion
- Tire Compound: Soft rubber compounds offer better grip, thus yielding a higher coefficient of friction, but they tend to wear out more quickly and are sensitive to temperature changes. In combination with temperature, the tire compound must be selected to remain sufficiently adhesive at real operating temperatures without becoming too soft or too rigid. Although softer compounds provide increased grip, they may require higher inflation pressures to compensate for excessive deformation.
- For rubber, there is a close relation between sliding friction (especially at low speeds) and viscoelastic properties. Softer rubber (or rubber at a higher temperature, and thus more compliant) shows increased friction under relevant regimes [134].
- Enhanced formulations incorporating nanomaterials can reduce rolling resistance (RR) by 5–7% while maintaining durability.
- Tread Pattern: The tread design influences how effectively water or debris is evacuated and the extent of direct contact with the road surface. Treads with numerous grooves and protrusions perform well on wet or muddy roads but may reduce actual contact on dry asphalt, especially if combined with improper inflation pressure. In terms of surface interaction, an off-road tread on smooth asphalt may significantly reduce grip compared to a slick tire designed for that specific surface. Wet-condition treads (e.g., multiple grooves and channels) increase grip on slippery surfaces but also raise rolling resistance due to increased volume and deformation.
- Road Surface: The texture and material composition of asphalt mixtures significantly affect tire grip. Smooth roads provide limited roughness, making tire composition and temperature more critical. On rough-textured or wet surfaces, tread design and inflation pressure are key to maintaining effective contact. Macroscopic roughness influences hysteresis through localized deformation. Road moisture changes the adhesion mechanism—from direct bonding on dry roads to hysteresis-dominated interaction in wet conditions.
- Temperature: Temperature directly affects the elasticity of rubber: too cold and a compound becomes rigid; too hot and it becomes excessively soft. Increased temperature softens the rubber (reducing its viscoelasticity), which in turn lowers internal hysteresis and therefore the coefficient of friction. Proper inflation can help the tire reach and maintain its optimal operating temperature more efficiently. Temperature is interdependent with wheel load: excessive load increases heat buildup and accelerates wear. Theory predicts that under isothermal conditions the coefficient of friction decreases with load, which is more pronounced for the adhesion than for the hysteresis contribution. This result is found to be in fair agreement with the measured friction curves confirming the contact mechanical approach of the theory [138]. Temperature significantly influences tire–road interaction through complex thermo-viscoelastic mechanisms. As temperature increases, the rubber’s modulus decreases, allowing greater conformity to pavement micro-texture and enhancing adhesive friction at moderate levels. Elevated thermal conditions also promote molecular mobility, facilitating interfacial bonding and improving grip within an optimal viscoelastic range. However, excessive heating causes over-softening of the tread rubber, reducing shear stiffness and promoting slip. Frictional heating at asperity contacts, flash temperature, further amplifies local softening, diminishing the hysteretic component of friction and potentially inducing frictional instability [139]. At high temperatures, the viscoelastic hysteresis losses decline because the difference between storage and loss moduli narrows, reducing energy dissipation and overall friction efficiency. This thermal–mechanical feedback loop between heat generation, deformation, and slip can destabilize traction. Consequently, an optimum temperature window exists in which grip is maximized; outside this range, either excessive stiffness at low temperatures or over-softening at high temperatures leads to reduced traction, accelerated wear, and potential thermal degradation of the tread compound.
- Wheel Load: A higher wheel load generally increases the contact patch area, thereby enhancing grip—up to a certain point. When high load is combined with low inflation pressure, it can lead to excessive deformation and performance degradation. Load distribution must be analyzed in conjunction with vehicle type and road conditions. Increased load often requires higher pressure to control deformation and manage friction. Electric vehicle (EV) tires, subject to higher weights, may experience accelerated wear and contribute to particulate emissions. The use of biomaterials is being explored to mitigate these impacts.
- Tire Pressure: Inflation pressure is one of the most critical and easily adjustable parameters. It affects the size and shape of the contact patch, thus influencing the effectiveness of the tread and grip. The ideal pressure depends on temperature, load, and road surface; for instance, in racing, pressure is adjusted based on the expected track temperature. Tire wear increases with pressure, load, and friction, especially under high speed and load conditions. Higher pressure reduces lateral deformation and the contact area, leading to lower rolling resistance but potentially also to a reduced coefficient of friction due to smaller contact footprints.
| Factor | Typical Effect | Notes | References |
|---|---|---|---|
| Tire compound | Softer rubber, softer viscoelastic compounds offer higher friction coefficients, especially at low slip speeds | Softer rubber conforms better to surface asperities and has higher hysteretic and adhesive contribution; compound glass transition controls temperature sensitivity. | [10,62,63,64,65,66,67,68,69,90,144,146] |
| Tire temperature | TRFC typically increases with moderate warming toward optimal tread temperature, then can decreases if overheated | Temperature changes rubber viscoelasticity and adhesion; there is an optimal window near which hysteretic loss and adhesion produce maximum grip. | [77,78,79,90,142,143,147,148] |
| Tread pattern | Pattern that evacuates water and provides biting edges offers higher wet friction coefficient | Tread channels control water evacuation, prevent hydroplaning; tread blocks provide mechanical interlocking on rough surfaces; depth affects contact and aquaplaning threshold. | [10,48,70,146,149,150] |
| Road surface/texture | Coarser texture and high micro-roughness offer higher friction coefficient (up to a point); polished and/or contaminated surfaces offer lower friction coefficient | Tread rubber compound in the lower slip region is most prominent, which is also where vehicles operate most of the time. | [42,50,52,54,55,71,72,73,74,145,151] |
| Tire inflation pressure | Higher pressure offers smaller contact patch and often lower grip (reduced hysteretic contribution); very low pressure may generate weak lateral guidance of a vehicle | Surface roughness determines hysteretic friction (rubber deformation) and real contact area; aggregate type (porous or dense) and contamination with ice or oil change this coefficient dramatically. | [50,60,80,81,82,83,84,151] |
| Wheel load (vertical force) | Friction coefficient often decreases with increasing normal load (contact area/pressure nonlinearity); peak friction force increases, but friction coefficient often falls | Pressure changes contact area, contact pressure distribution, and tread block stiffness; both under- and over-inflation hurt effective grip vs. optimum. | [80,81,82,138,142,144,147,151,152] |
- Tire Formula (e.g., rubber type, tread, and composition): This factor establishes the intrinsic viscoelastic properties of the material. It dictates the base level of adhesion (molecular forces) and hysteresis (energy dissipation). Tires designed for lower rolling resistance, for example, typically trade off some grip due to their material composition.
- Road Surface (micro- and macro-texture): Surface texture determines the available contact points and the deformation frequency of the rubber. Micro-texture influences adhesion, while macro-texture is key to hysteresis (due to bulk deformation) and also affects water drainage, which critically reduces adhesion on wet surfaces.
- Load and Pressure: These mechanical factors define the contact patch area and the nominal contact stress. Pressure primarily controls stiffness and contact shape. Load is the vertical force. The dynamic interplay means an increase in load can increase contact but simultaneously accelerate frictional heating, leading to a complex, nonlinear effect on the final TRFC.
- Temperature: The friction mechanism itself generates heat, making temperature a dynamic output that instantly becomes a key input:
- ○
- Frictional Heat Generation: When a tire slips or deforms on the road, the energy dissipated by hysteresis generates heat.
- ○
- Thermo-Viscoelastic Change: This heat raises the temperature within the contact patch, causing a change in the rubber’s viscoelastic properties (softening or stiffening), which in turn modifies the loss modulus and thus the hysteresis component of friction.
- ○
- Feedback Loop: This change in rubber properties alters the rate of heat generation and the resulting friction coefficient, creating a constant, closed-loop feedback mechanism that determines the final friction coefficient and wear rate.
4.1. Addressing RQ1: TWP Emission Reduction Strategies to Meet Euro 7 Regulations
- Restrictions on tire wear—to be assessed through standardized measurement methods (e.g., drum testing and real-world driving conditions).
- Optimization of tire composition and design—aimed at minimizing particle emissions without compromising safety or energy efficiency.
- Rigorous testing—involving validated methodologies in both real-traffic and laboratory environments.
4.2. Addressing RQ2: Technical Pathways and Challenges for Real-Time TRFC Estimation
- Reliance on fitted parameters: Models like the Magic Formula achieve high accuracy in fitting real data. However, this accuracy is attained through a large number of empirical fitting parameters (e.g., stiffness factor, peak factor, and curvature factor) These coefficients must be determined experimentally for every specific tire–road combination, making the model a function of the experimental data rather than a universal predictor.
- Degradation and lack of generalization: Traditional analytical models depend heavily on accurate physical parameters and well-defined slip conditions. Their performance degrades significantly when environmental factors, like surface wetness, temperature variation, or uneven road textures, introduce uncertainties at the tire–road interface. Consequently, they struggle to generalize outside of the specific, well-controlled conditions under which their parameters are derived.
- Computational cost for high fidelity: Highly detailed physical models, such as the FTire model or high-fidelity FEA models, offer comprehensive realism, including thermal effects and dynamic wear modeling. However, this fidelity comes at the cost of being extremely resource-intensive and having a high computational cost, which limits their utility for real-time control applications in vehicles.
- AI-driven estimators can advance beyond conventional model-based observers by learning complex, nonlinear relationships between tire, vehicle, and environmental variables directly from noisy sensor data. This capability allows them to adaptively infer friction levels, making them superior to traditional methods that struggle with uncertainties introduced by combined environmental effects.
- The ability of AI models to learn these “complex, nonlinear relationships” leads to the “black box” problem, where the decision-making process is opaque and lacks transparency. A variant could be moving towards hybrid systems, combining data-driven learning with physical modeling constraints, producing estimators that are both adaptive and interpretable. This necessity for interpretability points directly to the lack of transparency in purely data-driven models.
- AI models, especially those using external sensors like cameras for TRFC estimation, face significant challenges in generalization across varying lighting and weather conditions.
- The need for large, labeled datasets is a continuous challenge in development. Furthermore, their robustness is highly susceptible to sensor failures, highlighting their reliance on continuous, clean data streams.
- Fully coupled multi-physics wear models (thermal–mechanical–chemical): Advanced models like FTire account for thermo-mechanical effects and predict wear based on load, pressure, and road conditions. However, these models are often computationally expensive. There is a lack of computationally efficient and generalized models that fully integrate the thermal state, mechanical deformation, and chemical aspects (e.g., oxidative degradation and filler dispersion effects on wear) over a tire’s lifespan and across a wide range of operating conditions.
- Standardized, predictive models for tire wear particle generation and diffusion: The new Euro 7 regulations impose limits on non-exhaust particle emissions, highlighting the critical nature of this gap. Strategies to mitigate TWP emissions are multi-tiered (material innovation, operational measures, and environmental management). There is a particular need for harmonized methods to quantify tire abrasion and emissions. Specifically, the lack of a standardized prediction model that accurately forecasts the rate (generation) and fate (diffusion and environmental transport) of TWPs, linking them directly to complex, real-time tribological interactions, is a persistent gap.
- Real-time, adaptive TRFC estimation under combined environmental effects: Real-time friction estimation is essential for vehicle safety systems. Progress has been made using hybrid AI-enhanced estimators and sensor-based models. Despite advancements, the modeling of combined environmental factors (e.g., water, ice, dust, and temperature variations) remains insufficiently developed, preventing robust, highly accurate real-time friction prediction under all complex and transient conditions. This is particularly challenging for new systems like electric and autonomous vehicles which have distinct loading and torque patterns.
5. Conclusions
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Conflicts of Interest
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| Road | Static Friction Coefficient, μ0 | Dynamic Friction Coefficient, μ |
|---|---|---|
| Asphalt and concrete (dry) | 0.8–1.0 | 0.75 |
| Asphalt (wet) | 0.5–0.7 | 0.45–0.6 |
| Concrete (wet) | 0.8 | 0.7 |
| Gravel | 0.6 | 0.55 |
| Snow | 0.2 | 0.15 |
| Ice | 0.1 | 0.07 |
| Model | Characteristics | Typical Applications | Mathematical Description | No. of Papers in WoS | No. of Papers in Scopus | References |
|---|---|---|---|---|---|---|
| Magic Formula (Pacejka) | High accuracy; fits real data well; works for lateral, longitudinal, and combined slip | Vehicle dynamics, handling studies | Lateral force: where α—slip angle (rad) B—stiffness factor (slope near origin) C—shape factor D—peak factor (max force) E—curvature factor (asymmetry in curve) Extended versions include combined slip, camber, and longitudinal force. | 34 | 45 | [92,93,94,95,96] |
| Dugoff Model | Simple, computationally light, analytical form | Control design (ESC, path tracking); simplified dynamics | Longitudinal and lateral forces: where Fx, Fy—longitudinal and lateral forces s—longitudinal slip ratio α—sideslip angle Cs, Cα—longitudinal and lateral stiffness of tire µ—friction coefficient Fz—normal tire force λ—adhesion utilization factor f(λ)–saturation function | 31 | 36 | [97,98,99,100,101] |
| Brush Model | Good physical insight, handles combined slip, moderate complexity | Teaching. theoretical studies; control-oriented model | Lateral force: where a—half the contact length Cpy—lateral stiffness —tire model parameter σy = tan(α)—slip α—slip angle Fz—vertical load Μ—friction coefficient | 18 | 47 | [52,102,103,104,105,106] |
| LuGre Model and variants | Captures transient effects; can model stick–slip and hysteresis phenomena | Vehicle dynamics simulation; vehicle control design | Friction force: where z—internal bristle deflection v—relative velocity (slip speed) σ0—stiffness coefficient [N/m] σ1—damping coefficient [Ns/m] σ2—viscous friction coefficient [Ns/m] μs, μc—static and Coulomb friction coefficients vs—Stribeck velocity | 24 | 24 | [106,107,108,109,110,111,112] |
| Burckhardt Model | Less complex model than some others | Suitable for ABS/TCS, friction estimation, braking studies | Longitudinal force: where K—slip ratio Fz—normal tire force a1, a2, a3—fitting parameters | 11 | 13 | [110,113,114,115] |
| Fiala Model Stretched String | Less accurate for combined slip (braking + cornering); does not capture road condition changes | Suitable for preliminary vehicle simulations; does not provide sufficient accuracy for complex vehicle handling scenarios | Lateral force: Slip angle limit: asl = arctan(3μFz/Cα) where α—slip angle Cα—cornering stiffness Fz—vertical load μ—friction coefficient | 5 | 5 | [52,116,117] |
| FEM Models | High fidelity, detailed deformation and contact patch | Tire design, material research, structural analysis | 2 | 5 | [118,119,120] |
| Low Pressure | High Pressure |
|---|---|
| Larger but uneven contact patch | Smaller contact patch, smaller friction coefficient |
| Increased grip at low speed | Low grip, risk of skidding |
| Increased wear on the edges of the belt | Increased central tread wear |
| Increased risk of overheating | Stiffer suspension, reduced comfort |
| Strong wear of the tire and weak lateral guidance |
| Components | Influence on TRFC | Advantages/Disadvantages | References |
|---|---|---|---|
| Natural rubber (NR) | Reasonable wet performance but generally outperformed by current SSBR/silica systems designed for wet grip | Faster wear at high temperatures Epoxidized Natural Rubber (ENR) improves wet grip and friction, especially under certain loads/surface roughness. The epoxidation, filler can shift the dynamic properties/hysteresis to improve grip | [10,62,63,154,159] |
| Synthetic rubber (SBR) | SBR exhibits better tire–road friction in wet conditions than NR and maintains stability at higher operating temperatures | Durable, easily customizable, but higher fuel consumption Synthetic rubbers like (functionalized) SSBR tend to give better wet grip | [63,64] |
| Silica | Increases TRFC on wet and stable surfaces in cold conditions | Low fuel consumption, good grip; “Green Tire” silica reduces consumption by ~5% The coefficient of friction of silica-filled SBR is higher than that of carbon black-filled SBR, both in dry and lubricated sliding | [63,65,66,90,160] |
| Carbon black | Good TRFC at high temperatures, but decreases in wet conditions | Excellent abrasion resistance; ideal for off-road | [67,68,161] |
| Sulfur | Stiffness increases; affects hysteresis, particularly in dynamic contact with road surfaces; higher friction coefficient | Sulfur vulcanizates are prone to oxidative aging, especially under UV or ozone exposure As sulfur content increased, the hardness and abrasion resistance increased significantly | [69,161,162,163] |
| Biomaterials and resins | TRFC increased in wet conditions; increased wear and consumption | Bio-resins often have higher softening points compared to many oils or synthetic plasticizers. This helps raise viscoelastic loss at lower temperatures, which improves wet grip Sustainable, sensitive to wear | [65,164,165] |
| Plasticizers | Increased grip in cold weather; hysteresis and slightly higher consumption | Plasticizers affect hysteresis losses Increased energy dissipation, which is good for wet grip Improved elasticity and comfort may increase fuel consumption | [161,166] |
| Accelerators/ activators | Accelerators and activators do not directly increase or decrease the friction coefficient; they modify the crosslink network, which in turn affects viscoelastic hysteresis; results influence wet grip and rolling resistance; elastic modulus/stiffness affects dry adhesion and low-speed traction | Improves structure formation and strength | [85,161,162] |
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Soica, A.; Gheorghe, C. Tire–Road Interaction: A Comprehensive Review of Friction Mechanisms, Influencing Factors, and Future Challenges. Machines 2025, 13, 1005. https://doi.org/10.3390/machines13111005
Soica A, Gheorghe C. Tire–Road Interaction: A Comprehensive Review of Friction Mechanisms, Influencing Factors, and Future Challenges. Machines. 2025; 13(11):1005. https://doi.org/10.3390/machines13111005
Chicago/Turabian StyleSoica, Adrian, and Carmen Gheorghe. 2025. "Tire–Road Interaction: A Comprehensive Review of Friction Mechanisms, Influencing Factors, and Future Challenges" Machines 13, no. 11: 1005. https://doi.org/10.3390/machines13111005
APA StyleSoica, A., & Gheorghe, C. (2025). Tire–Road Interaction: A Comprehensive Review of Friction Mechanisms, Influencing Factors, and Future Challenges. Machines, 13(11), 1005. https://doi.org/10.3390/machines13111005

