Using semiconductor detectors, the fragment angular distributions have been measured in the cases of fission of Bi 209 and U 238 induced by alpha particles of various energies ranging from 23 to 115 MeV obtained from the Berkeley 88-in. variable-energy cyclotron. The center-of-mass angular distributions were analyzed by a least-squares fitting code to obtain the value of K 0 2 corresponding to the saddle-point excitation energy E x s for each bombarding energy. The transmission coefficients T l and the mean square of the orbital angular momentum 2 > of the fissioning nucleus required for deducing K 0 2 were determined from optical-model calculations. For both the cases of compound nuclei of At 213 and Pu 242 , it is found that the values of K 0 2 increase more rapidly with E x s than expected on the basis of the Fermi-gas model, irrespective of the assumptions made about the multiple-chance fissions. The fission cross sections of U 238 for alpha-particle energies up to 110 MeV, also measured in this work, enabled us to check the accuracy of the optical-model calculations. The presence of direct interactions and their effects on the deduced values of K 0 2 were also investigated in detail in the case of the target nucleus U 238 . Using the standard expression for Γ n /Γ f , the first-chance values of K 0 2 have been obtained and further corrected for the estimated direct-interaction effects, in the case of the target nucleus U 238 . Even after allowance is made for the direct-interaction effects, the energy dependence of K 0 2 appears to be significantly different from that expected on the basis of the simple Fermi-gas model. These results can be explained within the framework of the Fermi-gas model if it is assumed that J eff /a ½ f increases significantly with the bombarding energy. It appears likely that these results suggest a rapid increase in the effective moment of inertia J eff with the angular momentum, as can be expected on the basis of the observed steep variation in the saddle shapes with Z 2 /A.
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