[1] We appreciate the comments of Chen and Liu [2007] regarding our paper [Walker and Roberts, 2003] and are grateful for the opportunity for further discussion regarding interpreting the flow dimension of a hydraulic test. The comments of Chen and Liu (hereinafter referred to as CL) indicate that some aspects of Walker and Roberts (hereinafter referred to as WR) were unclear, and we hope to use this reply to reduce the confusion we have apparently caused. [2] We should first note that the flow dimension as a parameter of the generalized radial flow (GRF) model differs somewhat from our use of the apparent flow dimension as a diagnostic tool for hydraulic test interpretation. The GRF interpretive model fits the flow dimension as a parameter to account for the radial change in the crosssectional area of flow through an irregular network of homogeneous fractures [Barker, 1988]. The GRF estimates of hydraulic conductivity (KGRF) and specific storage (SGRF) are applicable to only that part of the domain conducting flow. That is, the GRF estimates depend on the fitted value of the flow dimension, similar to the parameters of any other interpretive model, e.g., the leakance parameter is specific to the leaky aquifer model and its value constrains the estimates of storage coefficient and transmissivity. In contrast, the apparent flow dimension is a diagnostic statistic that may be estimated from the late time slope of any observed hydraulic test. System geometry, heterogeneity [Doe, 1991; Walker et al., 2006], boundary conditions, and leakage [Walker and Roberts, 2003] have specific effects on the apparent flow dimension, thus it is a useful diagnostic for inferring conceptual models. In this sense, the apparent flow dimension is an extension of the use of the slope of the drawdown derivative as a diagnostic [Acuna and Yortsos, 1995; Horne, 1995]. The apparent flow dimension is not necessarily unique to a particular conceptual model [Doe, 1991;Walker and Roberts, 2003], thus all conceptual models producing the apparent flow dimension of a hydraulic test should be considered plausible until eliminated on the basis of other site characteristics. Using the apparent flow dimension as a diagnostic does not require using the GRF approach to interpret a hydraulic test, and the GRF model of homogeneous fractures is not necessarily a plausible conceptual model for an aquifer. Therefore we respectfully disagree with initial premise of CL that ‘‘if the apparent flow dimensions obtained are appropriate for the idealized systems, their application to [the GRF model] ought to reproduce the drawdown variations of these idealized systems.’’ We regret that that WR was not more explicit in this regard, and apologize for the confusion that this has created. [3] CL present useful calculations illustrating the ambiguities of forcing a site into the GRF model, and we would like to here add several comments. Much of the ambiguity of the GRF model arises from the definition of the extent of the flow zone, b, which Barker [1988] noted was difficult to describe for nonintegral flow dimensions, n. The extent of the flow zone cannot be separated easily from the GRF estimates, thus the estimates are sometimes reported as a generalized parameters, e.g., the generalized transmissivity is KGRF b 3 n [L /T] [Barker, 1988; Geier et al., 1996; Marechal et al., 2004]. We do not know how CL treated the flow zone in their analysis, but as we noted above, KGRF is the hydraulic conductivity of the space occupied by flow, so that KGRF should not be expected to match the hydraulic conductivity estimated using an interpretive model that assumes flow covers the entire Euclidean space. [4] For our analyses, we use a radial finite difference approach for interpreting hydraulic tests in fractured media. Recall that the flow area (A) in Barker’s [1988] formulation is given by