The theoretical required cooking times for inactivation of type E Clostridium botulinum toxin (5,000 LD5o mouse units per 0.5 ml) in haddock fillets of various sizes were calculated by graphical integration of the toxin inactivation rate and heat penetration data. The results indicated that normal cooking procedures should suffice to inactivate this amount of toxin. This conclusion was substantiated by the following additional experimental observations which revealed that the original experiments had been conducted under conservative conditions. First, maximal heat stability of the toxin was found to occur at about pH 5.5, with decreasing resistance upon increasing pH. The theoretical cooking times were based on destruction of the toxin at pH 6.7. The pH of radio-pasteurized inoculated haddock, when toxin production had occurred, was on the alkaline side, at which condition the toxin is heat-labile. Second, when spoilage was discernible in radiopasteurized inoculated haddock, the toxin titer was low, about 50 LDto mouse units per 0.5 ml. Third, the toxin was adequately inactivated in toxic fillets after deep-fat frying for 3 min at 375 F (190.6 C) or after pan frying for 5 min per side at 400 F (204.4 C). Fourth, in this study, residual toxin activity was assayed by intraperitoneal iniection of mice. It was shown that the oral toxic dose was 50 to 100 times greater than the intraperitoneal toxic dose.

The theoretical required cooking times for inactivation of type E Clostridium botulinum toxin (5,000 ld 50 mouse units per 0.5 ml) in haddock fillets of various sizes were calculated by graphical integration of the toxin inactivation rate and heat penetration data. The results indicated that normal cooking procedures should suffice to inactivate this amount of toxin. This conclusion was substantiated by the following additional experimental observations which revealed that the original experiments had been conducted under conservative conditions. First, maximal heat stability of the toxin was found to occur at about p H 5.5, with decreasing resistance upon increasing p H. The theoretical cooking times were based on destruction of the toxin at p H 6.7. The p H of radio-pasteurized inoculated haddock, when toxin production had occurred, was on the alkaline side, at which condition the toxin is heat-labile. Second, when spoilage was discernible in radio-pasteurized inoculated haddock, the toxin titer was low, about 50 ld 50 mouse units per 0.5 ml. Third, the toxin was adequately inactivated in toxic fillets after deep-fat frying for 3 min at 375 F (190.6 C) or after pan frying for 5 min per side at 400 F (204.4 C). Fourth, in this study, residual toxin activity was assayed by intraperitoneal injection of mice. It was shown that the oral toxic dose was 50 to 100 times greater than the intraperitoneal toxic dose.

At an irradiation temperature of 32'F the inactivation curve for Cloatridium botulinum type E toxin was characterized by an initial lag for the first 2 Mrad followed by an apparent linear portion represented by a D,, of 2.1 Mrad. The effect of irradiating at temperatures up to 117*5°F was only to shorten or eliminate the initial lag, A synergistic effect of irradiation temperature was indicated a t 91.4 and 105.8'F, but at 117.5'F the toxin appeared more radioresistant.

Rate of inactivation curves for the “free” toxin, prototoxin, or activated toxin in crude filtrates of Clostridium botulinum type E were nonlinear, consisting of a fast inactivating rate followed by a slow inactivating rate. Thermodynamic parameters were calculated over a temperature range of 125 to 145 F (51.7 to 62.8 C) for the two different inactivation rates. Energy of activation was low at the lower temperature and high at the higher temperature. The thermal requirement for inactivating similar concentrations of the “free” toxin, prototoxin, or activated toxin was considered to be the same.

Rate of inactivation curves for the "free" toxin, prototoxin, or activated toxin in crude filtrates of Clostridium botulinum type E were nonlinear, consisting of a fast inactivating rate followed by a slow inactivating rate. Thermodynamic parameters were calculated over a temperature range of 125 to 145 F (51.7 to 62.8 C) for the two different inactivation rates. Energy of activation was low at the lower temperature and high at the higher temperature. The thermal requirement for inactivating similar concentrations of the "free" toxin, prototoxin, or activated toxin was considered to be the same.