The concept of a hyperuniformity disorder length h was recently introduced for analyzing volume fraction fluctuations for a set of measuring windows [Chieco et al. (2017)]. This length permits a direct connection to the nature of disorder in the spatial configuration of the particles, and provides a way to diagnose the degree of hyperuniformity in terms of the scaling of h and its value in comparison with established bounds. Here, this approach is generalized for extended particles, which are larger than the image resolution and can lie partially inside and partially outside the measuring windows. The starting point is an expression for the relative volume fraction variance in terms of four distinct volumes: that of the particle, the measuring window, the mean-squared overlap between particle and region, and the region over which particles have non-zero overlap with the measuring window. After establishing limiting behaviors for the relative variance, computational methods are developed for both continuum and pixelated particles. Exact results are presented for particles of special shape, and for measuring windows of special shape, for which the equations are tractable. Comparison is made for other particle shapes, using simulated Poisson patterns. And the effects of polydispersity and image errors are discussed. For small measuring windows, both particle shape and spatial arrangement affect the form of the variance. For large regions, the variance scaling depends only on arrangement but particle shape sets the numerical proportionality. The combined understanding permit the measured variance to be translated to the spectrum of hyperuniformity lengths versus region size, as the quantifier of spatial arrangement. This program is demonstrated for a system of non-overlapping particles at a series of increasing packing fractions as well as for an Einstein pattern of particles with several different extended shapes.The structural uniformity of a many-body system may be studied in terms of fluctuations in the number [1,2] and volume fraction [3-5] of objects inside measuring windows of equal size but different locations. At one extreme, a totally random arrangement exhibits large fluctuations that are Poissonian, such that the volume fraction variance for largewhere L is the width of the measuring windows and d is dimensionality. By contrast, a "hyperuniform" [1] or "superhomogeneous" [2] arrangement exhibits smaller sub-Poissonian fluctuations that decay more rapidly as σ φ 2 (L) ∼ 1/L d+ with 0 < ≤ 1. At the = 1 extreme, two straightforward hyperuniform arrangements are "shuffled lattice" [2] and "Einstein" [6] patterns, where particles are effectively bound by square-well and harmonic potentials, respectively, to fixed crystalline lattice sites and are independently displaced as though by thermal energy. If the root mean square displacement is large compared to the lattice spacing, then the arrangement appears quite random to the eye. In such cases, the underlying crystalline order is well hidden.There has been gro...