4. Probability and statistics foundations for UQ

Uncertainty quantification (UQ) for occupant injury prediction rests on a simple premise: every quantity we care about — peak head acceleration, HIC15, chest deflection, femur force, AIS severity — is treated as a random variable rather than a single deterministic number. A finite element (FE) crash model with a nominal input set produces one response value; a UQ workflow acknowledges that material properties, restraint timing, occupant posture, and impact conditions vary, and it asks how the response is distributed as a consequence. This chapter establishes the probabilistic vocabulary and the specific distributional choices that recur throughout occupant safety analysis.

Random variables and their two flavors

A random variable (RV) is a measurable function mapping outcomes in a sample space to real numbers. In occupant injury work we encounter both types constantly. Continuous RVs include HIC15, peak chest acceleration (g), chest deflection (mm), and femur axial force (kN) — quantities that can, in principle, take any value in an interval. Discrete RVs include AIS level (0–6), airbag deployment stage (single-stage, dual-stage, adaptive), and the count of rib fractures. The distinction matters because it dictates which distribution family, density function, and estimation procedure apply.

Each RV is characterized by a cumulative distribution function (CDF), F(x) = P(X ≤ x), and — for continuous variables — a probability density function (PDF), f(x) = dF/dx. In injury prediction, the CDF is often the more useful object: the probability that HIC15 exceeds a regulatory or injury-reference threshold is simply 1 − F(threshold).

Expectation and variance: the first two moments

The expectation E[X] (mean, μ) is the probability-weighted average of the RV. For a continuous response it is E[X] = ∫ x f(x) dx; for a discrete response, E[X] = Σ xi p(xi). The variance Var(X) = E[(X − μ)²] = E[X²] − μ² measures dispersion around the mean, and its square root σ is the standard deviation in the same units as the response — far more interpretable when reporting, say, chest deflection in millimetres.

Two properties are used constantly in UQ propagation. First, expectation is linear: E[aX + bY] = aE[X] + bE[Y] regardless of dependence. Second, variance is not linear in general: Var(aX + bY) = a²Var(X) + b²Var(Y) + 2ab·Cov(X,Y). The covariance term is the reason correlated inputs — for example, belt stiffness and belt pretensioner timing that are tuned together — can produce response variance far larger than a naive independent-input assumption would suggest. Higher moments (skewness, kurtosis) matter when injury responses are strongly asymmetric or heavy-tailed, which is common for severe-injury tails.

Common injury response distributions

Choosing a distribution family is a modelling decision with physical consequences. The table below summarizes the families most frequently used for occupant injury responses, with the rationale for each.

DistributionSupportTypical injury applicationWhy it fits
Normal (Gaussian)(−∞, ∞)Material modulus, peak acceleration near nominalSymmetric, additive errors; convenient but can assign probability to non-physical negative values
Lognormal(0, ∞)HIC15, chest deflection, femur forcePositive, right-skewed; arises naturally from multiplicative effects
Weibull[0, ∞)Time-to-injury, tolerance thresholdsFlexible hazard shape; standard in injury-risk and reliability modelling
Beta[0, 1]Normalized injury probability, restraint effectiveness fractionBounded; ideal for probabilities and fractions
Bernoulli / Binomial{0,1} / {0,…,n}AIS ≥ 3 occurrence, rib fracture countDiscrete event outcomes
Uniform[a, b]Poorly characterized inputs (posture angle range)Maximum-entropy choice when only bounds are known

For HIC15 specifically, the lognormal is a defensible default: HIC is strictly positive, its distribution across a population of crash pulses is right-skewed, and log-transforming it yields an approximately normal variable suitable for standard statistical inference. A useful practical check is to plot the empirical CDF of HIC on lognormal probability paper; if the points fall near a straight line, the lognormal assumption is reasonable. If the tail bends upward, a Weibull or a mixture may be warranted.

From distributions to injury risk: the tolerance curve

Injury criteria are frequently expressed as risk functions. A common form is the lognormal risk curve, P(injury) = Φ[(ln(x) − μ)/σ], where Φ is the standard normal CDF and μ, σ are fitted to biomechanical tolerance data. This is the same lognormal family introduced above, now used as a risk model rather than a response model. The distinction is important: the response distribution describes what the model predicts; the risk curve describes the probability of injury given a response value. UQ combines the two by integrating the response distribution against the risk curve — a step developed in later chapters but whose foundation is the CDF machinery introduced here.

Response distribution: HIC₁₅ (lognormal) HIC₁₅ f(x) μ (mean) x* threshold P(X > x*) Injury risk curve: P(injury | x) HIC₁₅ P 1.0 risk at x* map x → risk UQ integrates the response PDF against the risk curve: P(injury) = ∫ P(injury | x) · f(x) dx

Estimating moments from simulation output

In practice, the response distribution is not known analytically; it is estimated from a sample of simulation runs. Given N runs with HIC values x1,…,xN, the sample mean and variance are:

mu_hat    = (1/N) * sum(x_i)
var_hat   = (1/(N-1)) * sum((x_i - mu_hat)^2)
sigma_hat = sqrt(var_hat)
cv        = sigma_hat / mu_hat          # coefficient of variation

The coefficient of variation (CV) is particularly useful for comparing dispersion across responses with different units. A CV of 0.15 on HIC15 indicates moderate scatter; a CV above 0.30 usually signals that a dominant input is poorly characterized and should be prioritized in sensitivity analysis. Note the (N−1) denominator: it yields an unbiased variance estimate, which matters when N is small (tens of runs, typical for FE-based UQ).

Practical check: Before fitting any parametric family, inspect the empirical CDF and a histogram of the response. If the sample is small, prefer moment-based summaries (mean, SD, CV, percentiles) over distribution fitting — a lognormal fitted to 20 points can badly misrepresent the tail that governs severe-injury probability.

Correlation and dependence

Occupant injury responses are rarely independent across outputs. Chest deflection and rib fracture count are driven by overlapping physics; peak head acceleration and HIC15 are functionally linked. The covariance matrix Σ captures these relationships, and its off-diagonal entries encode the linear dependence structure. When inputs are correlated, sampling must respect Σ — naive independent sampling of a multivariate normal with the wrong covariance will understate or overstate response variance. The Pearson correlation coefficient ρ = Cov(X,Y)/(σXσY) is the normalized version; values near ±1 indicate strong linear dependence, while ρ near 0 does not preclude nonlinear dependence.

Common pitfall: Applying a normal distribution to a strictly positive injury metric such as femur force can assign non-trivial probability to negative values when the mean is small relative to the standard deviation (CV > ~0.3). Truncate the distribution, switch to lognormal, or use a shifted family — and document the choice, because it changes the tail probabilities that drive risk estimates.

What this foundation enables

With random variables defined, moments understood, and distribution families selected on physical grounds, the UQ workflow gains its basic currency: a response is a distribution, a threshold comparison is a CDF evaluation, and a risk estimate is an integral of a risk curve against a response density. The next steps — sampling design, surrogate modelling, and sensitivity analysis — all operate on exactly these objects. Getting the distributional assumptions right at this stage prevents the more expensive errors that surface later when tail probabilities are extrapolated from a mis-specified model.