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              Liquid Alkali Metals                                                                        667

              TABLE V Solubility of Carbon in Liquid Lithium and Sodium  molecules being present in the liquid state. The sodium–
                                                                rubidium and sodium–cesium phase diagrams are sim-
              Temperature  Liquid lithium     Liquid sodium
                                                                ilar to that for sodium–potassium, and the binary mix-
                 ◦
                  C      (at. ppm)  (wt. ppm)  (at. ppm)  (wt. ppm)
                                                                                                           ◦
                                                                tures are liquid at temperatures down to −5 and −29 C,
                 200         2       3    0.38 × 10 −6  0.2 × 10 −6  respectively.
                 400        66      114   10.7 × 10 −2  5.6 × 10 −2  With mixtures of three of the alkali metals, the remark-
                 600       460      800      10.5     5.5       able feature is again the very low melting points that can
                 800      1550     2700      184      96        be achieved. Because of its immiscibility with the heavier
                                                                alkali metals, lithium is not suitable as a major compo-
                                                                nent of a lowmelting alloy. Of the other four metals, four
                                                                ternary systems are possible, and the lowest melting points
              V. ALKALI METAL MIXTURES
                                                                that can be achieved are as follows:
              The alkali metals resemble one another in atomic struc-
                                                                         System         Melting point ( C)
                                                                                                  ◦
              ture and in the physical and chemical properties of the
              bulk metals, and it might be expected that the properties  Na–K–Rb             −25
              of mixtures would lie close to the mean of the separate   Na–Rb–Cs             −37
              liquids. Some properties do, in fact, vary linearly with  K–Rb–Cs              −38
              composition; they include density, viscosity, compress-   Na–K–Cs              −78
              ibility, and specific heat. On the other hand, some proper-
              ties of mixtures deviate widely from values that would be  These are claimed to be the lowest melting points of
              calculated additively from the properties of the separate  any known metallic systems, and the alkali metals can
              components.                                       therefore be obtained as liquids at temperatures as low as
                                                                are normally available with organic solvents.
              A. Miscibility
              The heavier elements sodium to cesium are miscible with  C. Other Properties
              oneanotherinallproportionsintheliquidstate,andonlyin
                                                                Electrical resistivity measurement is the major technique
              the case of mixtures with lithium does immiscibility arise.
                                                                used to study reactions in solution, so it is relevant to
              Lithium–sodium mixtures are miscible in all proportions
                                                                note that the resistivity of any liquid alkali metal mixture
              above 305 C, but below this temperature the mixture sep-
                      ◦
                                                                is greater than that of either of the separate metals. The
                                            ◦
              arates into two separate phases. At 171 C, the immiscibil-
                                                                extent of this excess resistivity varies remarkably with
              ity gap extends from 10.1 to 97.0 at.% of lithium. Liquid
                                                                difference in atomic size of the components; the excess
              lithium is even less miscible with the heavier alkali metals.
                                                                forsodium–lithiummixturesisverysmallindeed,whereas
              When liquid lithium and liquid potassium are mixed, two
                                                                that for sodium–cesium mixtures is 10 times the resistivity
              immiscible liquid phases are formed; at 300 C the lithium
                                                ◦
                                                                of sodium alone.
              phase contains 0.43 at.% of potassium, and the potassium
                                                                  The surface tension of a liquid alkali metal mixture
              phase contains only 0.024 at.% of lithium. The miscibility
                                                                also shows pronounced deviation from the mean value.
              of lithium with rubidium and cesium is negligible.                                    −1    −3
                                                                The surface tension of liquid cesium (74 N m  × 10 ),
                                                                                                       −3
                                                                lies much below that for sodium (197 N m −1  × 10 ), and
              B. Melting Points
                                                                since surface tension reflects the attraction between atoms
              The sodium–potassium system has been the most fully  in the liquid, the concentration of cesium in the surface
              explored because at one time it seemed possible that  of the liquid metal mixture should be much greater than
              the eutectic mixture (NaK) might become the accepted  in the bulk of the liquid. Consistent with this, the sur-
              coolant for fast nuclear reactors. At the eutectic composi-  face tension of pure sodium falls rapidly upon addition
              tion, 67.8 at.% potassium, the mixture is liquid at temper-  of cesium, and in the range 40–100% cesium the surface
              atures down to −12.5 C. This low temperature relative  tension is near to that for pure cesium. A similar behavior
                                ◦
              to the melting points of the two pure metals (97.8 and  has been observed for sodium–potassium mixtures. Many
              63.2 C, respectively) is remarkable and must be related  chemical reactions of the liquid alkali metals and their
                 ◦
              to their different atomic sizes. An inflection in the phase  mixtures involve reaction with gases, and care must then
              diagram suggests the presence of a compound Na 2 K;  be exercised in relating reaction rates with bulk composi-
              presumably the atoms can pack into a solid structure  tion when it is the surface composition that is the relevant
              of this composition, and there is no evidence of Na 2 K  factor.
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