When Are Impedance Choices Irrelevant? Equivalence Conditions for Hansen-Style Access Metrics

1. Questions

Hansen (1959) established the weighted-sum structure of generalized cost components (e.g., time, money, operating costs) that underlies many access indices. In practice, analysts must pick an impedance $f$ (e.g., a cumulative threshold (all opportunities within $T$ equally counted), an exponential decay ($e^{-\theta t}$), or an inverse power ($1/t^p$)).

We ask:

1. When do different impedances yield the same percentage changes in access under uniform changes in land use, speed, or time budget?

2. When are cross-place rankings independent of the impedance?

3. How do these conditions relate to the frequent empirical finding that cumulative and gravity-type metrics are highly correlated?

Empirically, many studies report that common access measures often yield similar rankings or conclusions under typical parameter choices (Santana Palacios and El-Geneidy 2022; Kapatsila et al. 2023; Vale and Pereira 2017). This motivates the hypothesis that, under mild conditions, impedance choice may be irrelevant in specific senses. However, the precise reasons for this robustness have not been formally established. This paper sharpens and extends earlier insights by deriving general analytic results. We provide explicit elasticity formulas for accessibility with respect to uniform changes in land-use density, travel speed, and time budget, showing how these sensitivities compare across impedance functions (building on the qualitative trade-offs noted by Levine et al. (2012)). We also introduce a new decomposition of Hansen’s index into discrete distance-band contributions, which offers a clearer interpretation of how different decay functions weight near vs. far opportunities. Finally, we identify a simple dominance condition – proportional cumulative opportunity curves across locations – under which any impedance choice will yield identical cross-place accessibility rankings. This theoretical condition helps explain the empirical findings of prior work that different accessibility metrics often lead to the same conclusions. In these ways, our paper formalises and generalises scattered observations from the literature, providing a stronger foundation for when impedance choices are truly irrelevant and when they might matter.

2. Methods

Note: A complete nomenclature table is provided in Table 1.

We work with travel cost or time, denoted $t$ or $T$ for arguments and budgets, respectively. Here, ‘budget’ means a time or generalised cost limit or threshold, not monetary expenditure. Let $c_{ij}$ be generalised cost from origin $i$ to opportunity $j$, and $O_j \ge 0$ the size of opportunity $j$.

Hansen’s primal accessibility with budget $T$ is given by

$$A_i(T; f) = \sum_{j: c_{ij}\le T} O_j f(c_{ij}). \tag{1}$$

We use this budgeted form for all impedances. While an unbudgeted sum exists when $\int_0^\infty t f(t) \mathrm{d}t<\infty$ in the uniform–plane benchmark, which assumes constant speed across space (no congestion or signals), discrete sums are typically budgeted in practice, using the cumulative curve $N_i(t)$ defined as the sum of opportunities that can be reached from $i$ within travel cost $t$:

$$N_i(t) = \sum_{j: c_{ij}\le t} O_j. \tag{2}$$

Discrete jump-sum identity. The jump–sum identity says that accessibility can be computed as the sum, over each travel-time threshold, of the cumulative number of reachable opportunities at that threshold multiplied by the drop in the impedance weight at that point. Formally: Assume $f$ is non–increasing, bounded, and right–continuous with $f(\infty) = 0$, so $\Delta f_k \ge 0$ is well defined. Let $t_1 < \cdots < t_m$ be the strictly increasing ordering of the distinct costs $\{c_{ij}\}$ where $N_i(t)$ jumps, with jumps $J_i(t_k) = \sum_{j: c_{ij}=t_k} O_j$, and set $t_{m+1} = \infty$. Define $\Delta f_k := f(t_k) - f(t_{k+1})$ with $f(\infty) = 0$. Then

$$A_i(T; f) = \sum_{k: t_k\le T} N_i(t_k) \,\Delta f_k. \tag{3}$$

Note: Any tie–breaking that preserves the cumulative steps yields the same $A_i$, since only $N_i(t_k)$ and $\Delta f_k$ enter Equation (3). The jump-sum identity is shown in Appendix A.

Because $f$ is non-increasing, the framework excludes cases where being closer is undesirable (e.g., noise/safety next to certain stops).

Uniform-plane benchmark. The uniform-plane benchmark assumes opportunities are spread evenly across space and travel occurs at constant speed, so accessibility reduces to integrating opportunity density over concentric circles around an origin. Formally: for a uniform planar density $\rho$ and speed $v$, the marginal annulus area at time $t$ is proportional to $t$, so

$$A_i(T; f) = 2\pi\rho v^2 \int_{0}^{T} t\,f(t)\,\mathrm{d}t. \tag{4}$$

This gives the elasticities

$$E_\rho = 1,\qquad E_v = 2,\qquad E_T(T; f) = \frac{T^2 f(T)}{\displaystyle\int_{0}^{T} t\,f(t)\,\mathrm{d}t}. \tag{5}$$

Ranking invariance across impedances. If the cumulative opportunity curves for two places are proportional at all travel times, then their accessibility rankings will be the same no matter which impedance function is used. More precisely: if cumulative curves are proportional across places, $N_i(t) = \alpha_i N^\star(t)$ for all $t$, then for any non-increasing $f$ with $f(\infty) = 0$,

$$A_i(T; f) = \alpha_i \sum_{k: t_k\le T} N^\star(t_k) \,\Delta f_k, \tag{6}$$

so $A_i > A_{i'}$ if and only if $\alpha_i > \alpha_{i'}$, independent of $f$.

3. Findings

We next discuss the Findings in order.

Three results explain when impedance choice matters:

• First, in a uniform planar benchmark, density and speed elasticities are invariant across impedances.

• Second, cumulative opportunities is the only such impedance function with a constant time elasticity. See Eq. (7).

• Third, if cumulative curves are proportional across places, cross–place rankings do not depend on the impedance.

F1. Elasticity equivalence for land use and speed. On the uniform plane (see Methods, Section 2), the marginal annulus area at time $t$ is proportional to $t$, implying E${\mathstrut}_{\rho}=1$, E${\mathstrut}_v=2$ (see Eq. (5)).

These invariances rely on the uniform-plane benchmark; strong spatial non-uniformity or network effects can break them.

F2. Constant time elasticity. Among the canonical impedances shown here, only the cumulative opportunities has $E_T \equiv$ constant. For cumulative opportunities $f(t)=\mathbf{1}\{t\le T\}$,

$$A=\pi\rho v^2 T^2,\qquad E_T={2} \,\, \forall \,\,T. \tag{7}$$

Other impedances have $E_T(T;f)$ that varies with $T$, determined by the tail of $f$.

F3. Ranking invariance across impedances. If cumulative curves are proportional across places, $N_i(t) = \alpha_i N^\star(t)$ for all $t$, then for any non-increasing $f$ with $f(\infty) = 0$,

$$A_i(T; f) = \alpha_i \sum_{k: t_k\le T} N^\star(t_k)\,\Delta f_k, \tag{8}$$

so $A_i > A_{i'}$ if and only if $\alpha_i > \alpha_{i'}$, independent of $f$.

To diagnose whether this holds: plot $N_i(t)/N_i(T)$ for competing places over $t \in [0, T]$; nearly parallel curves indicate ranking stability across impedances, while crossings signal possible ranking flips as $\theta$ or $T$ varies.

F4. Practical indifference in narrow bands. When relevant travel times concentrate near a typical $t^\ast$, many impedances are nearly flat on that band, so percentage responses and rankings are often locally similar.

Illustration on the uniform plane. Three canonical impedances give closed forms with compact displays. Cumulative $f(t)=\mathbf{1}\{t\le T\}$:

$$A=\pi\rho v^2 T^2,\qquad E_T=2. \tag{9}$$

Exponential $f(t)=e^{-\theta t}$, where $\theta$ denotes the exponential decay parameter:

$$\begin{aligned} A &= \frac{2\pi\rho v^2}{\theta^2}\Bigl[1-(1+\theta T)e^{-\theta T}\Bigr],\\ E_T(T; e^{-\theta\cdot}) &= \frac{\theta^{2}T^{2}e^{-\theta T}}{1-(1+\theta T)e^{-\theta T}}. \end{aligned}\tag{10}$$

The micro-cutoff $t_0$ is the smallest practical time considered, used to avoid singularities at $t=0$. Inverse–square with micro–cutoff $f(t)=\mathbf{1}\{t\ge t_0\}\,(t_0/t)^2$:

$$A=2\pi\rho v^2\,t_0^2 \ln\!\frac{T}{t_0},\qquad E_T(T;f)=\frac{1}{\ln(T/t_0)}. \tag{11}$$

In all three cases $E_\rho=1$ and $E_v=2$ (see Eq. (5)).

When equivalence fails. See Supplemental Information for worked examples. Ranking invariance requires $N_i(t) = \alpha_iN^\star(t)$ for all $t$. If curves cross, weights on near versus far thresholds matter and different $f$ can reverse rankings, and thus interpretations. Time–elasticity invariance relies on the planar annulus area being proportional to $t$, so non-uniform density or network effects can break it.

Figure 1.Illustration of the discrete jump–sum identity (Equation (3)) with three cost thresholds $t_1 < t_2 < t_3 \leq T$. Top panel: cumulative opportunities $N_i(t)$. Middle panel: impedance $f(t)$ with baselines $f(t_k)$. Bottom panel: contributions $N_i(t_k) \Delta f_k$. Red segments $f(t_1)$, $f(t_2)$, and $f(t_3)$ determine the baselines of $\Delta f_k$. Green bars $N_i(t_k) \Delta f_k$ at bottom add to $A_i(T;f)$ under the budget $T$.