The heat capacities of two samples of vanadium and two of tantalum have been measured in the normal and superconducting phases in the temperature interval between 1.7^∘{} and 5^∘{}K. Below the transition temperature T₀, the superconducting heat capacity of both metals could be represented accurately by the relation Cₛ=AT+BT². In the normal phase the data obeyed the usual relation Cₙ=γT+(464θ³)T³. From these data H vs T curves were calculated and values of H₀, the threshold field at absolute zero, were obtained. For the better vanadium sample the values of the various constants were found to be T₀=4.89^∘K, A=-1.97×10^-3 cal/mole deg², B=1.69×10^-3 cal/mole deg³, γ=21.1×10^-4 cal/mole deg², Θ=273^∘K, and H₀=1340 oersteds; for the better tantalum sample T₀=4.38^∘K, A=-1.45×10^-3 cal/mole deg², B=1.33×10^-3 cal/mole deg³, γ=13.0×10^-4 cal/mole deg², Θ=231^∘K, and H₀=860 gauss. The measured heat capacities were compared with the predictions of the Koppe theory and the α model.
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Worley et al. (1955) studied this question.
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