The key formulas from every finished module, grouped by lesson. Each lesson title links back to the full explanation. Symbols follow the course's SAE convention (x forward, y right, z down) unless a note says otherwise. For definitions of the terms, see the glossary.

Symbols and units

SymbolMeaningUnits
The car
\(m,\ W = mg\)Total mass and weightkg, N
\(m_s,\ m_{us}\)Sprung mass; unsprung mass (per axle)kg
\(a,\ b,\ L = a + b\)CG to front axle, CG to rear axle, wheelbasem
\(t\)Track widthm
\(h,\ h_s,\ h_{us}\)CG height; sprung-mass CG height; unsprung-mass CG heightm
\(h_{rc},\ h_{ra}\)Roll-center height (front or rear); roll-axis height under the sprung CGm
\(K_\phi\)Roll stiffness (\(K_{\phi f}\), \(K_{\phi r}\) per axle)N·m/deg
\(I_z\)Yaw moment of inertiakg·m²
Motion
\(V\) (or \(v\))Speedm/s
\(R\)Turn radiusm
\(a_x,\ a_y\)Longitudinal and lateral accelerationm/s² or g
\(a_{CG}\)Deceleration of the CG under braking (Lesson 3.3)g
\(r\)Yaw raterad/s
\(\psi,\ \theta,\ \phi\)Yaw (heading), pitch and roll anglesrad or deg
\(\delta\)Front-wheel steer anglerad or deg
\(\beta\)Sideslip angle at the CG. In Lesson 3.3 only, \(\beta\) is the front brake bias.rad or deg
\(K\)Understeer gradient (negative = oversteer)rad/(m/s²)
Tires
\(F_x,\ F_y,\ F_z\)Longitudinal, lateral and vertical (normal) tire force. \(N\) is also used for normal force on FBDs.N
\(\mu\)Peak friction coefficient (\(\mu_x\), \(\mu_y\) for each direction)—
\(\mu_0,\ F_{z0},\ s\)Load-sensitivity model: friction at the reference load, the reference load, the sensitivity—, N, —
\(\alpha,\ \kappa,\ \gamma\)Slip angle, slip ratio, camber angledeg, —, deg
\(C_\alpha,\ C_\kappa,\ C_\gamma\)Cornering stiffness, longitudinal slip stiffness, camber stiffnessN/deg, N, N/deg
\(\Omega,\ r_e,\ I_w\)Wheel spin rate, effective rolling radius, wheel inertiarad/s, m, kg·m²
\(T_b,\ p\)Brake torque; tire pressureN·m; kPa

A plain \(a\) is always the CG-to-front-axle distance; accelerations always carry a subscript (\(a_x\), \(a_y\), \(a_{CG}\)).

Unit conversions

QuantityConversion
Speedkm/h \(\div 3.6\) → m/s; mph \(\times 0.447\) → m/s
Acceleration1 g = 9.81 m/s²
Angle1 rad = 57.3°
Pressureabsolute = gauge + 101.3 kPa; 1 psi = 6.895 kPa
TemperatureK = °C + 273.15
Power1 hp ≈ 746 W

QuantityFormulaNotes
Newton's second law\(\Sigma \mathbf{F} = m\,\mathbf{a}_{CG}\)Real forces only on an FBD: no “centrifugal force”.
Yaw rotation\(\Sigma M_z = I_z\,\ddot\psi\)Steady turn: \(\Sigma M_z = 0\).
Circular motion\(a_y = \dfrac{V^2}{R} = V r\)
\(r = \dfrac{V}{R}\)
Know any two of \(V, R, r, a_y\) and you know the rest.
Steady turn, forces\(N_{\text{in}} + N_{\text{out}} = mg\)
\(F_{y,\text{in}} + F_{y,\text{out}} = m\dfrac{V^2}{R}\)
Vertical and lateral balance.
Steady turn, roll moment\((N_{\text{out}} - N_{\text{in}})\,\dfrac{t}{2} = (F_{y,\text{in}} + F_{y,\text{out}})\,h\)Moments about the CG: why the outside tires carry more load.

QuantityFormulaNotes
Vehicle axesSAE: \(x\) forward, \(y\) right, \(z\) downISO 8855: \(x\) forward, \(y\) left, \(z\) up.
Rotationsroll \(\phi\) about \(x\), pitch \(\theta\) about \(y\), yaw \(\psi\) about \(z\)Right-hand rule.
Course angle\(\psi + \beta\)Direction of travel = heading + sideslip.
Slip angles\(\alpha_f = \beta + \dfrac{a\,r}{V} - \delta\)
\(\alpha_r = \beta - \dfrac{b\,r}{V}\)
SAE signs, small angles.
Tire lateral force\(F_y = -C_\alpha\,\alpha\)SAE: a negative slip angle gives a positive (rightward) force.

QuantityFormulaNotes
Force to turn\(F_y = m\,\dfrac{V^2}{R}\)Supplied entirely by the tires.
Maximum corner speed\(V_{\max} = \sqrt{\mu\, g\, R}\)No aerodynamic downforce.
Friction circle (one tire)\(\sqrt{F_x^2 + F_y^2} \le \mu F_z\)Grip is shared between braking/driving and cornering.
g-g circle (whole car)\(\sqrt{a_x^2 + a_y^2} \le \mu\)Accelerations in g.
Friction ellipse\(\left(\dfrac{a_y}{\mu_y}\right)^2 + \left(\dfrac{a_x}{\mu_x}\right)^2 \le 1\)Forward acceleration is also capped by the drive (power) limit.

QuantityFormulaNotes
Critical speed\(U_{\text{crit}} = \sqrt{\dfrac{L}{|K|}}\)Oversteering car (\(K < 0\)) is unstable above it. An understeering car has none.

QuantityFormulaNotes
Cornering stiffness\(C_\alpha = \left.\dfrac{dF_y}{d\alpha}\right|_{\alpha = 0}\)Slope of the tire curve at zero slip.
Linear tire\(F_y \approx C_\alpha\,\alpha\)Small slip angles only.
Peak lateral force\(F_{y,\max} = \mu(F_z)\,F_z\)Reached near the peak slip angle.
Load sensitivity\(\mu(F_z) = \mu_0\left[1 - s\,\dfrac{F_z - F_{z0}}{F_{z0}}\right]\)\(\mu\) falls as load rises.
Pair of tires, load transfer \(\Delta F\)\(F_{y,\text{pair}} = 2\mu_0 F_{z0} - \dfrac{2\mu_0\, s\, \Delta F^2}{F_{z0}}\)Load transfer always costs an axle grip.
Magic Formula\(F_y = D \sin\!\big(C \arctan \Phi\big)\)
\(\Phi = B\alpha - E\,(B\alpha - \arctan B\alpha)\)
\(D\) = peak force, \(C\) = shape, \(E\) = curvature; slope at the origin \(BCD = C_\alpha\).

QuantityFormulaNotes
Slip ratio\(\kappa = \dfrac{\Omega r_e - V}{V}\)\(\kappa > 0\) driving, \(\kappa < 0\) braking, locked wheel \(\kappa = -1\).
Linear tire\(F_x \approx C_\kappa\,\kappa\)Small slip ratios only.
Peak longitudinal force\(F_{x,\max} = \mu_x F_z\)Typically at 5–15% slip, depending on the tire.
Wheel spin dynamics\(I_w\,\dot\Omega = F_x\,r_e - T_b\)Past the peak, lock-up runs away.
Stopping distance\(d = \dfrac{V^2}{2\mu g}\)Use the peak \(\mu\) for ABS, the sliding \(\mu\) for a locked wheel.

QuantityFormulaNotes
Friction ellipse (tire)\(\left(\dfrac{F_x}{F_{x,\max}}\right)^2 + \left(\dfrac{F_y}{F_{y,\max}}\right)^2 \le 1\)Combined braking/driving and cornering.
Lateral force left while braking\(F_y = F_{y,\max}\sqrt{1 - \left(\dfrac{F_x}{F_{x,\max}}\right)^2}\)On the ellipse boundary.
Normalized combined slip\(n = \sqrt{\left(\dfrac{\kappa}{\kappa_{\text{peak}}}\right)^2 + \left(\dfrac{\alpha}{\alpha_{\text{peak}}}\right)^2}\)\(n = 1\) is the combined peak. A sliding tire's force points along its sliding direction.

QuantityFormulaNotes
Camber thrust (linear)\(F_y \approx C_\alpha\,\alpha + C_\gamma\,\gamma\)\(C_\gamma \ll C_\alpha\).
Camber at the limit\(\gamma_{\text{at limit}} = \gamma_{\text{static}} + \Delta\gamma_{\text{roll}}\)Aim near the tire's optimum camber.
Contact patch area\(A \approx \dfrac{F_z}{p}\)Membrane model, \(p\) gauge.
Hot pressure\(p_{2,\text{abs}} = p_{1,\text{abs}}\,\dfrac{T_2}{T_1}\)Absolute pressure and absolute temperature (K).
Normalized tire curve\(F_y / F_z\)Curves that don't collapse onto one show load sensitivity.

QuantityFormulaNotes
Static axle loads\(W_f = W\,\dfrac{b}{L}\)
\(W_r = W\,\dfrac{a}{L}\)
Each wheel carries half its axle's load.
Longitudinal load transfer\(\Delta F_{z,\text{long}} = \dfrac{m\,a_x\,h}{L}\)Change in each axle's load; to the front under braking.
Total lateral load transfer\(\Delta F_{z,f} + \Delta F_{z,r} = \dfrac{m\,a_y\,h}{t}\)\(\Delta F_{z}\) = load gained by each outside wheel (lost by each inside wheel).
Front share (simple model)\(\dfrac{\Delta F_{z,f}}{\Delta F_{z,f} + \Delta F_{z,r}} = \dfrac{K_{\phi f}}{K_{\phi f} + K_{\phi r}}\)The axle with more load transfer saturates first.

QuantityFormulaNotes
Unsprung transfer\(\Delta F_{z,us} = \dfrac{m_{us}\,a_y\,h_{us}}{t}\)Per axle, using that axle's unsprung mass.
Geometric transfer\(\Delta F_{z,geo} = \dfrac{m_{s,\text{axle}}\,a_y\,h_{rc}}{t}\)Through the links, immediately, with no body roll needed.
Roll-axis height under the CG\(h_{ra} = h_{rc,f} + (h_{rc,r} - h_{rc,f})\,\dfrac{a}{L}\)Straight line between the two roll centers.
Roll moment\(M_\phi = m_s\,a_y\,(h_s - h_{ra})\)\(h_s - h_{ra}\) is the roll moment arm.
Elastic transfer\(\Delta F_{z,el} = \dfrac{K_{\phi,\text{axle}}}{K_\phi}\,\dfrac{M_\phi}{t}\)Through the springs and anti-roll bars.
Body roll\(\phi = \dfrac{M_\phi}{K_\phi}\)\(K_\phi\) in N·m/deg. Roll gradient \(\phi / a_y\) in deg/g.
Totalunsprung + geometric + elasticSame total as Lesson 3.1: the paths only redistribute it.

QuantityFormulaNotes
Axle loads under braking\(\dfrac{N_f}{W} = \dfrac{b}{L} + a_{CG}\,\dfrac{h}{L}\)
\(\dfrac{N_r}{W} = \dfrac{a}{L} - a_{CG}\,\dfrac{h}{L}\)
\(a_{CG}\) in g.
Brake force split\(F_{xf} = \beta\,W a_{CG}\)
\(F_{xr} = (1-\beta)\,W a_{CG}\)
\(\beta\) = front brake bias (front share of brake force).
Ideal brake bias\(\beta_{\text{ideal}} = \dfrac{b}{L} + a_{CG}\,\dfrac{h}{L}\)At the limit \(a_{CG} = \mu\); moves rearward when grip falls.
Front lock-up\(a_{CG}^{\text{front lock}} = \dfrac{\mu\,b/L}{\beta - \mu h/L}\)The front never locks if \(\beta \le \mu h/L\).
Rear lock-up\(a_{CG}^{\text{rear lock}} = \dfrac{\mu\,a/L}{1 - \beta + \mu h/L}\)Maximum deceleration is the smaller of the two lock values.
Set-up rule\(\beta\) slightly forward of \(\beta_{\text{ideal}}\)Fronts lock first and the car stays stable.