<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">TEL</journal-id><journal-title-group><journal-title>Theoretical Economics Letters</journal-title></journal-title-group><issn pub-type="epub">2162-2078</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/tel.2012.23062</article-id><article-id pub-id-type="publisher-id">TEL-21508</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Business&amp;Economics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Water Resource and Power Generation: An Alternative Formulation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ack</surname><given-names>Robles</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>School of Economics and Finance, Victoria University of Wellington, Wellington, New Zealand</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Jack.Robles@vuw.ac.nz</email></corresp></author-notes><pub-date pub-type="epub"><day>02</day><month>08</month><year>2012</year></pub-date><volume>02</volume><issue>03</issue><fpage>341</fpage><lpage>343</lpage><history><date date-type="received"><day>March</day>	<month>6,</month>	<year>2012</year></date><date date-type="rev-recd"><day>April</day>	<month>8,</month>	<year>2012</year>	</date><date date-type="accepted"><day>May</day>	<month>10,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Crampes and Moreaux [1] provide a two period model of competition between a hydrostation and a thermal station for the generation of electricity. We modify this model to make it more directly comparable with an infinite horizon model. The closed loop equilibrium is characterized.
 
</p></abstract><kwd-group><kwd>Water Resource; Hydroelectricity; Cournot Competition; Closed Loop Equilibrium</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Crampes and Moreaux [<xref ref-type="bibr" rid="scirp.21508-ref1">1</xref>] (CM) provide a two period model of competition between a thermal station and a hydrostation for the production of electricity. CM’s analysis is both broad and illuminating. However, their model contains implicit assumptions which make it difficult to compare with an infinite horizon model. In this paper, we modify CM’s model to facilitate such comparisons, and solve for the closed loop equilibrium.</p><p>An appropriately written finite horizon model is essential to the understanding of infinite horizon models. Robles [<xref ref-type="bibr" rid="scirp.21508-ref2">2</xref>] analyzes an infinite horizon model and shows that one can characterize Markov Perfect Equilibria by finding the appropriate closed loop equilibrium to a one year finite horizon model.</p><p>A thermal station acts much like any firm. The hydrostation produces energy with (essentially) no variable cost. However, it’s output is constrained by the quantity of water in it’s reservoir. It can mitigate this constraint by passing water through time, but this ability as well is subject to constraint.</p><p>Our model has two main departures from CM’s: we allow for an over abundance of water as well as scarcity, and we allow water inflows in all periods rather than just the first. The second departure requires a third; our scarcity constraints are per period rather than global. We observe that in an infinite horizon model: no reservoir is large enough to prevent a firm from forcing it to overflow eventually, and water inflows must occur in more than one period. Consequently, an infinite horizon model must have all the constraints that we have added to the model. For the comparisons carried out in Robles (2009) to be meaningful, a finite horizon model must have these constraints as well. In addition, our departures from CM’s model: clarify the role of the various constraints, and allow the possibility of multiple equilibria.</p></sec><sec id="s2"><title>2. Model</title><p>The model runs over two periods labelled<img src="20-1500119\5b707f93-2610-4322-9c57-9c5dcd1daa59.jpg" />. There is no discounting between periods. In each period, the thermal station produces <img src="20-1500119\2c623bd0-d317-4e83-9e6f-b467dd053924.jpg" /> and the hydrostation produces <img src="20-1500119\9ede5236-08ad-42b6-845d-1f376f5b788b.jpg" /> electricity. The per period (inverse) demand is denoted<img src="20-1500119\70fc0e58-d3be-4920-a5ea-8f6730ecee97.jpg" />. The per period cost function for the thermal plant, denoted<img src="20-1500119\79086b91-f413-4a77-92a1-69b861a5e70e.jpg" />, is increasing and convex:</p><p><img src="20-1500119\f9038e23-9a06-4c8d-a51d-d6f7c0eeb842.jpg" /></p><p>The thermal plant’s installed capacity is large enough that no constraint is imposed.</p><p>The hydrostation has no variable costs, but faces a number of constraints. Let <img src="20-1500119\8250335b-02c2-4eb5-84cf-e001373ba97b.jpg" /> denote the stock of water available at the beginning of period<img src="20-1500119\b28e5b26-420c-48fd-b72b-69be680c3f6e.jpg" />. CM impose the resource constraint<img src="20-1500119\02f08aa6-ff8c-4f29-9ccb-a70b9a1e91b3.jpg" />.</p><p>Like CM, we assume that <img src="20-1500119\a6874d99-cd79-4ea2-8e8a-4b0b0b1ca315.jpg" /> is set exogenously. However, we allow for an additional exogenous inflow of water between periods which we denote by<img src="20-1500119\c4e5362f-055d-4e76-aa8a-4c5a70dcc025.jpg" />. Hence,</p><p><img src="20-1500119\25e3721b-2b9c-4daf-8a3a-104c38aee0a2.jpg" /></p><p>Consequently, we need a resource constraint for each period. We also include a constraint on the hydrostation’s storage; the hydrostation must end the period with no more than <img src="20-1500119\005131b7-870e-4d95-8024-d12b63f21f6e.jpg" /> water. We assume that <img src="20-1500119\4e265c82-1def-4f92-8844-e1e1fba8734c.jpg" /> is sufficiently large that if<img src="20-1500119\56f21168-4336-4b38-b4f8-b24fddcf02ec.jpg" />, then the second period resource constraint can not bind in equilibrium. Further, we require that water is either used or passed to the future; there is no “spilling”. This implies the per period hydroconstraints 1 and 2:</p><disp-formula id="scirp.21508-formula68249"><label>(1)</label><graphic position="anchor" xlink:href="20-1500119\40e2e13d-d0fd-4c7e-9ffc-feece85ea712.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.21508-formula68250"><label>(2)</label><graphic position="anchor" xlink:href="20-1500119\632552ba-993c-4a1c-9c10-7fbfabb6a4e6.jpg"  xlink:type="simple"/></disp-formula><p>Finally, we include a non-negativity constraint. For comparison CM: have no overflow constraints, and use a single resource constraint.</p></sec><sec id="s3"><title>3. Equilibrium</title><p>We solve for the closed loop or subgame perfect equilibrium. In each period, firms set output. Demand, <img src="20-1500119\0e71a250-1c83-4d22-8c39-906887f8fe9c.jpg" />, is downward sloping and such that each firm’s per period revenue function is concave in that firm’s own output. We denote the period <img src="20-1500119\1522fe47-bfce-4aad-afd7-6af006d763a5.jpg" /> revenue function for the hydrostation (resp. thermal station) by <img src="20-1500119\22fa33be-ca31-475d-92dd-bdd57a1bb3b5.jpg" /> (resp.<img src="20-1500119\02e3a3b4-f00b-442b-a393-d4eef8e5c759.jpg" />.)</p><p>In each period the thermal plant acts to maximize profits within that period,<img src="20-1500119\4c12a869-d208-4d87-b2c4-e3360ab69254.jpg" />. In each period<img src="20-1500119\e0557947-e6a7-4ed5-af72-a43938f73fb0.jpg" />, he satisfies</p><p><img src="20-1500119\95fccc4b-c15c-40d2-a063-1e1a7d7b4c0e.jpg" /></p><p>Here <img src="20-1500119\6b562c9f-446a-41e2-b8ff-bbccd02f6db1.jpg" /> is the multiplier on the thermal station’s period <img src="20-1500119\92d43d4a-616e-477a-b031-eb95cd03cecd.jpg" /> non-negativity constraint and the relevant complimentary slackness condition holds. Let <img src="20-1500119\cb7c885c-96d5-4b21-885f-3137013e0979.jpg" /> denote the thermal station’s period <img src="20-1500119\1e211fdb-d6c8-46f0-8035-771e9aa5005a.jpg" /> reaction function.</p><p>Because of his constraints, the hydrostation’s optimal choice depends upon the stock of water<img src="20-1500119\9c75d4cd-b6a9-4101-b7c3-414293262f31.jpg" />. Let <img src="20-1500119\bf6bc329-f4b2-4bd8-8341-4cb09483a8b4.jpg" /> denote the hydrostation’s optimal choice.</p><p>In the second period, the hydrostation’s problem is non-dynamic as well. However, he faces no variable costs, but must satisfy the hydro-constraints. The resulting first order condition is</p><disp-formula id="scirp.21508-formula68251"><label>(3)</label><graphic position="anchor" xlink:href="20-1500119\0894e50e-3965-44ce-9f98-ef60d47905e8.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="20-1500119\67540485-8773-409a-8792-8b7cd4aa7cd1.jpg" />, <img src="20-1500119\a0068042-bde1-473f-8a2c-0e79abcc03ff.jpg" />, and <img src="20-1500119\7fa8dbdf-6dbe-49ea-a0d6-f2d44ed4036d.jpg" /> are (respectively) the multipliers on the period <img src="20-1500119\2455f86a-574b-4026-80ad-b2f7dacf92a6.jpg" /> resource, overflow, and nonnegativity constraints.</p><p>Let <img src="20-1500119\710cbbc3-df9f-4871-9a7a-a5b9af1fa1b3.jpg" /> denote the solution to</p><p><img src="20-1500119\e3518d31-4f51-44cf-9332-aaf657faf5a0.jpg" /></p><p>If neither hydro-constraint binds in period 2, then <img src="20-1500119\96452d7b-ecac-4b96-b920-125a94933315.jpg" /> has no impact on output and<img src="20-1500119\c302b53a-0b4c-468d-8b2c-1ccb1a650c69.jpg" />. That is, the two firms behave like standard Cournot Duopolists.</p><p>In period 1, the hydrostation faces a dynamic problem, and acts to maximize<img src="20-1500119\0e0e7cc7-4ccf-4ef8-b05d-4bc06083c973.jpg" />. Of course <img src="20-1500119\f9fad880-c995-46a0-bb7d-d463f482acb5.jpg" /> enters directly into<img src="20-1500119\12f75aff-a4d3-473e-b50c-5f056d2174e3.jpg" />. However, it might also determine <img src="20-1500119\78da5336-7fff-4ad8-8deb-5c113518ef35.jpg" /> by setting<img src="20-1500119\7c4fa0b9-fdff-44e7-8197-699510eee365.jpg" />. Hence, the hydrostation acts to satisfy the following first order condition:<sup>1</sup></p><disp-formula id="scirp.21508-formula68252"><label>(4)</label><graphic position="anchor" xlink:href="20-1500119\5f7eeaea-d6da-42ae-901a-fdf30bdd4690.jpg"  xlink:type="simple"/></disp-formula><p>The LHSs of the hydrostation’s two first order conditions are analogous. However, the RHS of the period 1 first order condition might not be zero. Instead, it reflects the value of water in period 2. The first term on the RHS is the second period marginal revenue, holding <img src="20-1500119\7d50e9e1-f6b8-4c7b-865d-1dbd4b57cf7a.jpg" /> constant. The second piece is the strategic effect. It is never negative. It is strictly positive if <img src="20-1500119\650f2754-0606-4e30-8881-efefbbfcc27a.jpg" /> and a second period hydro-constraint binds. In this case, an increase in <img src="20-1500119\3833b57f-92a4-499e-a31a-22a69ea5e79c.jpg" /> leads to a decrease in<img src="20-1500119\7b67bed5-6a82-4cc2-bdc5-dd6519ca4b6c.jpg" />. In response, the hydrostation will tend to move water from the first period to the second.</p><p>We turn now to a characterization of the various possible cases. First assume neither hydro-constraint binds in either period. Clearly the hydrostation sets <img src="20-1500119\c72dfb3c-20be-4990-88fb-8c09b98245bd.jpg" /></p><p>at<img src="20-1500119\62565c26-085a-4f82-bcd8-0e220d3c8aec.jpg" />. Since this output does not depend upon<img src="20-1500119\c72aa189-c744-4c5e-96e4-c9404356f65b.jpg" />, we have <img src="20-1500119\5d83d374-f199-47c8-949f-773fc12991b0.jpg" /> making the strategic term in Equation (4) zero. In addition, since the second period output is determined by<img src="20-1500119\36570265-1c99-4de1-acf3-09fd4b342da6.jpg" />, the remaining terms on the RHS sum to zero. Hence first period output is<img src="20-1500119\163ba513-791e-4796-ac8a-c6df0b02639b.jpg" />. That is, if neither hydro-constraint binds in either period, then we have period by period static Cournot competition. Our assumption that <img src="20-1500119\4ca9452f-f057-4ac7-aacc-e67a367952fb.jpg" /> is large can now be formally stated as<img src="20-1500119\793f6c5d-ea3d-466e-ac56-583bf88b0d7a.jpg" />.</p><p>The preceding paragraph implies that the second period non-negativity constraint binds in equilibrium if and only if<img src="20-1500119\9c372b04-92bc-4b77-bb52-0d449b260fee.jpg" />. This is as it should be, because the only other reason that a non-negativity constraint should bind is because of a desire to pass water to the future. However, in CM this constraint might bind because of a desire to use more than the entire resource of water in the first period. That is, CM’s second period non-negativity constraint might need to do the work that should be done by a first period resource constraint.</p><p>We consider next the possibility of a hydro-constraint binding in the first period. If this happens, and <img src="20-1500119\6486fbab-c59e-4d7f-b283-df48c47ab587.jpg" />, then the hydro station’s problem becomes static. That is, in each period t he acts as if to maximize period t profits. However, if<img src="20-1500119\fb101480-0eb3-47b1-8d66-9201e8083a35.jpg" />, then the resource constraint might bind in the first period, but with<img src="20-1500119\81dbfed2-676a-49e6-a113-22d169577bb6.jpg" />. That is, the hydrostation would like to pass water backwards in time even though marginal revenue is negative in the first period. Of course, this requires that marginal revenue is even more negative in the second period.</p><p>We now consider the case in which a hydro-constraint binds in period 2, but no hydro-constraint binds in period 1. If the overflow constraint binds, then <img src="20-1500119\38740141-52fe-4ecf-afc5-a0490cd558e2.jpg" /> and<img src="20-1500119\51856d77-f4db-4998-b1d8-dd75b2775e34.jpg" />. If the resource constraint binds then <img src="20-1500119\bf768cc1-5c36-4fc7-a886-684c63a18623.jpg" /> and<img src="20-1500119\d6fcd88e-ad85-46e5-b972-2e3e12ebd3e0.jpg" />. In both cases, the two equations are redundant, and only determine the value of<img src="20-1500119\13ac3822-9ecd-493a-8477-2bca24ff7e0f.jpg" />. However, if either of the hydro-constraints binds strictly, then <img src="20-1500119\76d7da7c-18a5-4c9e-8f8a-7bf0f4af652a.jpg" /> and Equation (4)</p><p>nails down the exact values of <img src="20-1500119\c89fe357-bc73-4e4d-9f5e-27e5aeae930d.jpg" /> and<img src="20-1500119\01e97b9c-663d-4cfa-a48c-2125d56ff9be.jpg" />.</p><p>We already established that if neither binds then</p><p><img src="20-1500119\0e914e9a-ea31-493e-bce4-336024feb631.jpg" />. The possibility remains of a weakly binding second period hydro-constraint remains, in which case <img src="20-1500119\1e561de0-a9a6-4286-ba81-839e27b2cfd4.jpg" /> is undefined.</p><p>In equilibrium, the overflow constraint can’t bind weakly in the second period. Assume otherwise. If<img src="20-1500119\54a361ea-25c3-4c21-995b-c7590d93d117.jpg" />, then one can increase <img src="20-1500119\64033ce4-ff7d-4f5b-91b0-f24e9d8e9a0b.jpg" /> without decreasing <img src="20-1500119\9c667c21-4ba1-48ea-a174-526e19271afe.jpg" /> and increase profits. If<img src="20-1500119\bbad764f-3f4a-49e3-9ea7-f754d4c317f6.jpg" />, then one can decrease<img src="20-1500119\745e6b61-9adc-4142-8dcd-fef7fd1f71be.jpg" />, which increases profits by making the overflow constraint bind in the second period. On the other hand, the second period resource constraint can bind weakly. In this case, Equation (4) is not useful. However, when the resource constraint binds weakly, the equilibrium is easy to calculate;<img src="20-1500119\20329f84-f55a-459e-917c-00422bca6cea.jpg" />, and<img src="20-1500119\ce3844a7-cb86-43cb-8137-e6a454b32fb5.jpg" />.</p><p>Multiple equilibria are possible because whether the overflow constraint binds, or not, is determined endogenously by first period output. Since the two firms set output in each period simultaneously, there are circumstances where the hydrostation wants to force the overflow constraint to bind for some choices or<img src="20-1500119\2679b695-e951-41dc-826d-37c85d842755.jpg" />, but not for others. That is, for some values of <img src="20-1500119\995e1387-fe0f-4058-b0f5-0723279fcee1.jpg" /> and<img src="20-1500119\c99e7d71-033c-442b-9c2b-34767dd6e599.jpg" />, there are multiple equilibria.</p><p>&#160; We conclude with an example which illustrates how the water resource determines the equilibrium. Set<img src="20-1500119\07b9cb1c-1215-404f-8e83-d492099f0cb1.jpg" />, a<sub>1</sub> = 5, a<sub>2</sub> = 8 and<img src="20-1500119\557d65b1-5ed5-45a5-b35f-cf6f80151601.jpg" />. <xref ref-type="fig" rid="fig1">Figure 1</xref> illustrates the equilibrium outputs for the hydrostation as a function of the water supply. There are three general situations: water is scarce, water is abundant, and water</p><p>is over abundant. The left hand box of <xref ref-type="fig" rid="fig1">Figure 1</xref> graphs the transition from scarce to abundant; we set <img src="20-1500119\e26e15c6-0309-48cc-87d8-505647b1f254.jpg" /> and increase <img src="20-1500119\753f1d52-23fa-47d6-91ef-b0a4a32d103f.jpg" /> up from zero. From zero to the first dotted line, the second period resource constraint bindsand Equation (4) holds with<img src="20-1500119\831e9458-ac0f-4db1-bfd1-f7d60bbed2aa.jpg" />. From the first to the second dotted line, the second period resource constraint binds weakly and<img src="20-1500119\23fe6fd0-815d-4f78-af62-349c1c88bfc3.jpg" />. To the right of the second dotted line: no constraints bind, <img src="20-1500119\2591cfac-2f22-4706-b69d-1a75ca99af94.jpg" />and<img src="20-1500119\7af596b9-3bbe-499b-92f8-f36c7ec7d904.jpg" />.</p><p>The right hand box in <xref ref-type="fig" rid="fig1">Figure 1</xref> graphs the transition from abundant to over abundant. We set<img src="20-1500119\1ba8b96c-c86a-46b6-8f2c-fb05347b940f.jpg" />, and increase <img src="20-1500119\a8eb5389-e009-45aa-acf9-3e71a5ed9df3.jpg" /> from 0. To the first dotted line, the only equilibrium has <img src="20-1500119\27ee7abc-5992-4813-a345-b45fb5160e8d.jpg" /> and<img src="20-1500119\31436be7-98b6-4045-abac-bcee30702528.jpg" />. At the first dotted line, there is sufficient water to support an equilibrium in which overflow constraint binds in the second period. Between the first two dotted lines, both these equilibria exist. At the second dotted line, the reward from forcing the overflow constraint to bind in the second period becomes too great, and the first equilibrium disappears. At the third dotted line, <img src="20-1500119\271c7bbe-827d-48d4-b1a3-982cee1f180d.jpg" />, which removes the strategic benefit from increasing<img src="20-1500119\f06bd26d-a024-435f-b511-f9990b9645ef.jpg" />. At the fourth dotted line, the marginal revenues are equal across the two periods, and so additional water is spread between them evenly.</p></sec><sec id="s4"><title>REFERENCES</title></sec><sec id="s5"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.21508-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">C. Crampes and M. Moreaux, “Water Resource and Power Generation,” International Journal of Industrial Organization, Vol. 19, No. 6, 2001, pp. 975-997. 
doi:10.1016/S0167-7187(99)00052-1</mixed-citation></ref><ref id="scirp.21508-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">J. Robles, “Infinite Horizon Hydro Power Games,” Unpublished Manuscript, Victoria University, Wellington, 2009.</mixed-citation></ref></ref-list></back></article>