Phosphofructokinase (isozymes) activation by theophylline or by 3',5' cyclic AMP administration.

Phosphofructokinase activity of rat thyroid, kidney and muscle can be enhanced by in vivo administration of theophylline or cyclic AMP. This enhancement occurs in the different tissues to a different extent depending on the tissue-specific isozymes. Thyroid and muscle phosphofructokinase which is mainly A-type, is strongly stimulated after administering theophylline in the drinking water over a 8 days period. The kidney enzyme which encompasses about 50% of each A and B type is activated to a lesser extent. Liver phosphofructokinase which is pure B-type shows very little response if any. Comparable results have been obtained with either the muscle or liver enzyme after two to four hours treatment with a single injection of 10 mg/rat of either cyclic AMP or theophylline. This short-term activation could be eliminated by treating the animals with Actinomycin D, 30 min prior to theophylline or cyclic AMP. The possible mechanisms leading to the enhancement of phosphofructokinase activity are discussed.     

Content of 3',5' cyclic AMP and cyclic AMP phosphodiesterase in dormant and activated tissues of Jerusalem artichoke tubers

Using an highly sensitive and specific radioimmunoassay for 3′,5′ cyclic AMP, we have detected this cyclic nucleotide in partially purified extracts obtained from tuber tissues of Jerusalem artichoke. The level of cyclic AMP found in dormant tubers was very high compared with those of sprouting tubers and rapidly declines when dormant tissue slices are activated by incubation in aerated water. Cyclic AMP phosphodiesterase seems to play an important role in these changes of cyclic AMP content.     

Resolving UV Bioactinometric Results with Intensity and Time Distributions

A UV reactor with an annular design, a total liquid volume of 460[emsp4 ]ml, and outfitted with a single lamp with 1690[emsp4 ]mW of germicidal power was tested. Coliphage MS2 was used as a bioactinometer to measure the UV dose at a flow rate of 56.7[emsp4 ]ml/sec in water with a very low absorbance. The Beers Law coefficient was A₁₀0.003. The measured dose (MS2 bioactinometry) was 35.2±1.1[emsp4 ]mW-sec/cm².A retention time distribution was generated with a dye tracer study. The reactor was modeled as if flow was confined to ten equal volume paths existing as concentric rings around the lamp. The UV intensity along each path (ith intensity) was calculated to generate a simulated distribution of UV intensity in the reactor. The retention time distribution was subdivided to estimate the retention time associated with each decile jth time) of the total flow.Seven methods of associating the ith intensity with the jth retention time were used to produce simulated dose distributions for the reactor. The average UV dose for each distribution was calculated as the average of the products of I and t (AP protocol) and by the apparent survival (AS protocol), in which the predicted survival along each path was averaged to back-calculate dose from the reference batch inactivation curve. The average dose predicted assuming that time and intensity were independent was 51.5[emsp4 ]mW-sec/cm² based on the arithmetic average (AP protocol). Using the apparent survival method, the predicted dose for the independent distribution (I independent of t) was 36.4[emsp4 ]mW-sec/cm². Three methods of developing dependent structure between time and intensity were tested. In the best possible case for stratified flow (I negatively correlated with t) the calculated (AS) intensity was 46.3[emsp4 ]mW-sec/cm^2. In the worst case for stratified flow (I positively correlated with t) the AS intensity was 32.0[emsp4 ]mW-sec/cm². In a rational case where flows were assumed to be distributed parabolically (low flow at the wall and at the lamp) produced an AS intensity of 37.7[emsp4 ]mW-sec/cm². When either time or intensity was averaged, while the other variable was allowed to keep its distribution, the (AS) dose (time averaged 43.3[emsp4 ]mW-sec/cm², intensity averaged 41.0[emsp4 ]mW-sec/cm²), yielded a poor prediction compared to the measured value.The errors associated with averaging time, intensity, or both, far outweigh the errors associated with choosing a rational distribution or an independent distribution of time and intensity in the prediction. This observation is generally true whenever an organism is exposed to UV light in a flow through reactor such that the range of doses is within the portion of the inactivation curve exhibiting strong exponential decay.