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Location in a Disk City with Consumer Concentration Around the Center

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Abstract

The paper studies a two-stage location-price duopoly game in a disk city with consumer concentration around the city center. When consumers are uniformly distributed over the plane, unconstrained firms locate outside of the city. Consumer concentration, however, induces firms to locate nearer to each other and, when the degree of concentration is sufficiently high, inside of the city. Prices and firm profits decrease in the degree of consumer concentration. We explicitly solve the model for classes of cone-shaped, dome-shaped, and bell-shaped consumer densities. In all cases we identify a loss of welfare due to the strategic effect which causes the firms’ spatial differentiation being too large.

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Notes

  1. The disk area on the right side of the vertical line \(\tilde{x}\) is \(2\int_{\tilde{x}}^{1}r\arccos(\tilde{x}/r)dr\). Multiply at each point in this area by the local consumer density \(f(r)\) to obtain the demand function \(D(\tilde{x})\).

  2. This is a two-dimensional extension inter alia of the triangular density function as used by Tabuchi and Thisse (1995). A corresponding specification can be found in Mazalov and Sakaguchi (2003).

  3. If the city border is binding, firms locate on the disk’s perimeter at maximal distance. Substituting \(x_{1}=-x_{2}=1\), \(D(\tilde{x}=0)=1/2\), and \(D^{\prime}(\tilde{x}=0)=-2/\pi\) into the price equations (4) shows that the firms charge the prices \(p=\pi<p^{*}\) and hence realize the profits \(\Pi=(1/2)\pi<\Pi^{*}\). This solution is the constrained optimum as it was derived by Mazalov and Sakaguchi (2003) and Feldin (2012).

  4. This is a two-dimensional counterpart to the one-dimensional beta density function as used by Stadler (2012).

  5. Note that \(\Gamma(1/2)=\sqrt{\pi}\), \(\Gamma(1)=1\), and \(\Gamma(n+1)=n\Gamma(n)\) for \(n=\{1/2,1\}\).

  6. Note that the tiny area differential \(dA\) for the polar coordinates (\(r,\phi\)) is \(dA=rdrd\phi\).

  7. Additionally, the population of the city – an alternative measure of the “city size” – does not have to be restricted to the mass of 1. An increasing mass would leave the location and price decisions of the firms unchanged but would proportionally increase their profits.

  8. In case of finite support, a rectangular (or a quadratic) product space would certainly be preferable to a disk space. A quadratic product space, however, is not tractable for an analysis of demand concentration since the property of polar-symmetry is not satisfied. In the case of infinite support, the geometrical difference between a disk and a square diminishes such that this problem is resolved.

  9. As pointed out e.g. by Ansari et al. (1994), the distribution of consumer preferences in many markets is unlikely to be uniform.

  10. Note that \(\arccos(0)=\pi/2\) and \(2\pi\int_{0}^{1}rf(r)dr=1\) for all feasible polar-symmetric consumer densities.

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Correspondence to Manfred Stadler.

Additional information

Paper presented at the 18th annual GEABA conference at the University of Hohenheim. The author gratefully acknowledges comments of the participants, especially of the discussant Karl Morasch, as well as the helpful suggestions of two anonymous referees.

Appendix

Appendix

As described in the main text, the demand function of firm 1 reads

$$D(\tilde{x})=2\int_{\tilde{x}}^{1}f(r)r\arccos(\tilde{x}/r)dr$$
(18)

and the demand of firm 2 is \(1-D(\tilde{x})\). By using Leibniz’s rule and integrating by parts, we obtain the derivatives

$$D^{\prime}(\tilde{x})=-2\int_{\tilde{x}}^{1}\frac{f(r)}{\sqrt{1-(\tilde{x}/r)^{2}}}dr =-2\left[f(1)\sqrt{1-\tilde{x}^{2}}-\int_{\tilde{x}}^{1}f^{\prime}(r)\sqrt{r^{2}-\tilde{x}^{2}}dr\right]$$
(19)

and

$$D^{\prime\prime}(\tilde{x})=2\tilde{x}\left[\frac{f(1)}{\sqrt{1-\tilde{x}^{2}}}-\int_{\tilde{x}}^{1}\frac{f^{\prime}(r)}{\sqrt{r^{2}-\tilde{x}^{2}}}dr\right].$$
(20)

In the case of \(\tilde{x}=0\) (symmetric firm location around the city center), one obtainsFootnote 10

$$D(\tilde{x}=0)=1/2.$$
(21)

The first two derivatives amount to

$$D^{\prime}(\tilde{x}=0)=-2\int_{0}^{1}f(r)dr<0$$
(22)

and

$$D^{\prime\prime}(\tilde{x}=0)=0.$$
(23)

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Stadler, M. Location in a Disk City with Consumer Concentration Around the Center. Schmalenbach Bus Rev 71, 35–50 (2019). https://doi.org/10.1007/s41464-018-0064-0

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