A physical design is developed for a gas-cooled heavy-water nuclear reactor intended for a project of a nuclear power plant. As a fuel, the reactor would employ thorium with a small admixture of enriched uranium that contains not more than 20% of 235 U. It operates in the open-cycle mode involving 233 U production from thorium and its subsequent burnup. The reactor meets the conditions of a nonproliferation of nuclear weapons: the content of fissionable isotopes in uranium at all stages of the process, including the final one, is below the threshold for constructing an atomic bomb, the amount of product plutonium being extremely small. ] proposed an idea of nuclear-power-plant reactors that would meet the requirements of a nonproliferation of nuclear weapons. The idea ensured nonproliferation on the basis of existing physics laws. Specifically, fuel elements of such a reactor contain 238 U, 232 Th, and 235 U. As the reactor operates, 233 U formed from thorium takes the place 235 U. The ratios of 238 U, 235 U, and 232 Th concentrations are chosen in such a way that, at any stage of reactor operation, including the discharge period, the nuclear fuel is inappropriate for creating an atomic bomb. (At the initial stage, within which there is no 233 U in the fuel, we have 235 U < 20% and 235 U/( 238 U + 235 U) < 20%; after a complete replacement of 235 U by 233 U-as a matter of fact, this stage is not achieved in practicethe condition 233 U < 12% is expected to hold for the respective concentration.) For a more detailed exposition of this idea, the interested reader is referred to [3]. It should be noted that, in such a reactor, the spent fuel is protected from stealing and from the use in terrorist attacks by a high radioactivity of 232 U daughter products that arise because of n → 2n fast-neutron-induced reactions. Reactors of this type have yet another advantage: 233 U fission leads to the appearance of substantially smaller amounts of transuranium isotopes and, hence, long-lived radioactivity in relation to the fission of 235 U or 239 Pu † Deceased. and 241 Pu, and this facilitates the transmutation of radioactive waste.As applied to PWR light-water reactors, reactors of this type were calculated by Radkowsky and Galperin [4], while, as applied to VVER reactors, this was done by Ponomarev-Stepnoi and his coauthors [5].Below we presented the results of preliminary calculations for a gas-cooled heavy-water reactor of this type and perform a comparison with a similar VVERbased reactor [5]. The calculations were carried out by B.P. Kochurov.In the Soviet Union, the theory of nuclear reactors was developed by I.Ya. Pomeranchuk, I.