D.R. Fredrickson
Argonne National Laboratory
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Featured researches published by D.R. Fredrickson.
The Journal of Chemical Thermodynamics | 1970
D.R. Fredrickson; M.G. Chasanov
Abstract A high-precision drop calorimetric system has been used to measure the enthalpy of UO2 and National Bureau of Standards sapphire in the temperature range 500 to 1500 K, relative to 298.15 K. All temperatures are based on IPTS-48. The UO2 results can be represented by the equation: H°(T) − H°(298.15 K) = {19.7614( T K ) + 5.49053 × 10 −4 ( T K ) 2 + 6.96890 × 10 6 ( T K ) −1 − 7951.68} cal mol −1 Values of Cpo, Ho(T) − Ho(298.15 K), So, and {G o − H o (298.15 K )} T are tabulated. The sapphire results can be represented by the equation: H°(T) − H°(298.15 K) = {27.6002( T K ) + 1.61393 × 10 −3 ( T K ) 2 + 9.65836 × 10 5 ( T K ) −1 − 11554.31} cal mol −1
The Journal of Chemical Thermodynamics | 1973
D.R. Fredrickson; M.G. Chasanov
A high-precision drop-calorimetric system has been used to measure the enthalpy (relative to 298.15 K) of Na 2 O in the temperature range 500 to 1300 K. A rapid rise in the derived C p ( T ) is observed about 900 K, which may be attributed to the onset of a diffuse transition in Na 2 O and a disordering of the Na + ions. The results are therefore represented by two equations, one for temperatures below 900 K and another for temperatures above 900 K. In the range 298 to 900 K: { H o ( T ) − H o ( 298.15 K ) } / c a l t h m o l − 1 = 13.8814 ( T / K ) + 4.4249 × 10 − 3 ( T / K ) 2 − 4532.09. In the range 900 to 1300 K: { H o ( T ) − H o ( 298.15 K ) } / c a l t h m o l − 1 = 35.4157 ( T / K ) − 2.80046 × 10 − 2 ( T / K ) 2 + + 1.42549 × 10 − 5 ( T / K ) 3 − 8036.87. All temperatures are based on IPTS-68. Values of { H o ( T )− H o (298.15 K)}, C o p ( T ), { S o ( T ) − S o (298.15 K)}, Δ H o f ( T ), Δ G o f ( T ), and log K o p ( T ) are tabulated.
The Journal of Chemical Thermodynamics | 1972
D.R. Fredrickson; M.G. Chasanov
Abstract The enthalpy (relative to 298.15 K) of Na3UO4 was measured from 500 to 1200 K using a high-precision drop-calorimetric system. The following equation represents the enthalpy of Na3UO4 in the temperature range 298 to 1200 K. All temperatures are based on IPTS-68. Values of Cpo(T), {Ho(T)−Ho(298.15 K)}, So(T), and {G o (T)−H o (298.15 K)} T are tabulated.
The Journal of Chemical Thermodynamics | 1980
D.R. Fredrickson; Gerald K. Johnson; P.A.G. O'Hare
Abstract High-temperature enthalpy increments and derived heat capacities are reported for Cs 2 CrO 4 . There is a solid-to-solid transition at (1031 ± 3) K and the melting temperature is (1236 ± 5) K. The enthalpies of transition and fusion are (2.9 ± 0.6) and (35.3 ± 0.7) kJ mol −1 , respectively, and the entropies of transition and fusion are (2.8 ± 0.6) and (28.6 ± 0.5) J K −1 mol −1 , respectively. Results obtained in this study are combined with other recent data to produce a table of the thermodynamic functions of Cs 2 CrO 4 to 1500 K.
The Journal of Chemical Thermodynamics | 1971
D.R. Fredrickson; M.G. Chasanov
A high-precision drop-calorimetric system has been used to measure the enthalpy (relative to 298.15 K) of MoS2 in the temperature range 500 to 1200 K. All temperatures are based on IPTS-48. The results can be represented by the following equation, which should be used only over the experimental range: H o ( T ) − H o ( 298.15 K ) = { 16.8278 ( T / K ) + 9.4045 × 10 − 4 ( T / K ) 2 + 5.1881 × 10 4 ( T / K ) − 1 − 5495.38 } cal mol − 1 . Values of Cop(T), Ho(T) − Ho(298.15 K), So(T), and {Go(T) − Ho(298.15 K)}/T are tabulated.
The Journal of Chemical Thermodynamics | 1976
D.R. Fredrickson; P.A.G. O'Hare
A high-precision drop-calorimetric system has been used to measure the enthalpies (relative to 298.15 K) of α- and β-Na2UO4 to 1300 K, and of Cs2UO4 to 1100 K. In the range 298 to 1193 K the enthalpy increments for α-Na2UO4 can be represented by the equation: H°(T)−H°(298.15 K={38.8476(T/K)+3.09342×10−3(T/K)2+5.01109×105(T/K)−1−13538.12}calthmol−1. In the range 1193 to 1300 K the enthalpy increments of β-Na2UO4 can be represented by: H°(T)−H°(298.15K={53.69844(T/K)−23824.88} calthmol−1. Enthalpy increments for Cs2UO4 are represented over the temperature range 298 to 1100 K by: H°(T)−H°(298.15K)={39.4076(T/K+2.03432×10−3(T/K)2+3.65323×105(T/K)−1−13155.51} calth mole−1. Values of Cpo(T), {Ho(T) − Ho(298.15 K), So(T), and {Go(T) − Ho(298.15 K)}T are tabulated. For the α to β transition in Na2UO4, a value of ΔHtr = 5.9 kcalth mol−1 at 1193 K has been deduced.
The Journal of Chemical Thermodynamics | 1977
P.A.G. O'Hare; Juliana Boerio; D.R. Fredrickson; Henry R. Hoekstra
Solution and drop-calorimetric studies of magnesium uranate are described. From the solution experiments, the standard enthalpy of formation, ΔHfo(MgUO4, c, 298.15 K) was found to be −(1857.0 ± 1.3) kJ mol−1. The drop-calorimetric experiments gave values for the enthalpy increment {Ho(T) − Ho(298.15 K)} and heat capacity Cpo(T), which, over the temperature range 298.15 to 1400 K, are best represented by the equations: {H°(T) − H°(298.15K}J mol−1 = 110.268(TK + 3.3398 × 10−2(TK)2 −7.8127×10−6(TK3 − 35638; C°p(T)J K−1mol−1 = 110.268 + 6.6796 x 10−2(TK) −2.3438 × 10−6(TK)2 The complete thermodynamic functions of MgUO4 are tabulated from 298.15 to 1400 K. The spontaneity of the decomposition of BeUO4 to its component oxides is advanced as an explanation for the non-existence of this compound.
The Journal of Chemical Thermodynamics | 1977
Howard E. Flotow; Darrell W. Osborne; William G. Lyon; Fernande Grandjean; D.R. Fredrickson; Ian J. Hastings
Abstract The heat capacity of triuranium silicide, U 3 Si, has been measured from 1 to 350 K and its enthalpy determined from 298 to 1160 K. The coefficient γ for the heat capacity contribution of the conduction electrons ( γT ) is (39.3 ± 0.4) mJ K −2 mol −1 . Thermodynamic functions are tabulated at selected temperatures between 1 and 1203 K. At 298.15 K, the values determined for the heat capacity C p o , the entropy S o , the enthalpy { H o (298.15 K) − H o (0)}, and the function {G o (298.15 K ) − H o (0)} 298.15 K are (107.90 ± 0.43) J K −1 mol −1 , (174.02 ± 0.70) J K −1 mol −1 , (23297 ± 93) J mol −1 , and −(95.88 ± 0.38) J K −1 mol −1 , respectively. The standard Gibbs energy of formation ΔG f o (U 3 Si, c, 298.15 K) = −(105.6 ± 19.2) kJ mol −1 was derived.
The Journal of Chemical Thermodynamics | 1974
D.R. Fredrickson; M.G. Chasanov
Abstract The enthalpy (relative to 298.15 K) of liquid sodium was measured to 1505 K, using a high-precision drop-calorimetric system. The following equation represents the enthalpy of liquid sodium in the temperature range from 554 to 1505 K: H o (T)−H o (298.15 K ={4.62436( T K )+8.4442 × 10 −4 ( T K ) 2 −5.92445×10 5 ( T K )×10 5 ( T K ) −1 +731.931} cal th mol − All temperatures are based on IPTS-68. Values of {Ho(T) − Ho(298.15 K)}, Cpo(T), and {So(T) − So(298.15 K} are tabulated.
The Journal of Physical Chemistry | 1963
D.R. Fredrickson; Ralph L. Nuttall; Howard E. Flotow; Ward N. Hubbard