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Period Mechanism of Semilunar Eclosion Rhythm of the Marine Midge Pontomyia oceanaChang, Yin-hao 07 August 2006 (has links)
We studied the eclosion rhythm of the marine midge Pontomyia oceana in southern Taiwan. The lunar/semilunr rhythm is known to be endogenous since it persists under continous light or dark conditions. In this study, we discovered that the period of the eclosion rhythm is about 15 days, although the midges have to spend an additional 15 days in the beginning of their lives before entering the eclosion rhythm. The period of the semilunrar eclosion rhythm is controlled by counting cycles of endogenous circadian rhythms which in term was entrainable by external light-dark (LD) cycles. We demonstrated this by modifying the period of LD cycles in different parts of their life histories with or without the entraining factor and then observing the ecolsion times in the laboratory. Night light can entrain the semilunar eclosion rhythm; we discovered that the cue and the eclosion are in the same phase of the semilunar rhythm but with a full cycle of shift. Temperature compensation in period control is demonstrated in this species. Q10 values close to 1 is found between 24 to 30¢XC in the laboratory.
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The Effect of Temperature on Synchronized Eclosion and the Study of Eclosion Rhythm of the Marine Midge Pontomyia oceanaLee, Pin-Hsien 15 June 2000 (has links)
Abstract
The effects of temperature on daily eclosion time and monthly eclosion days of the marine midge Pontomyia oceana were investigated. We changed temperature at different times on the eclosion day. The results show that P. oceana has started related metabolic processes at sunrise which lead to eclosion after sunset. Daily temperature cycles do not have concentrating effect on daily eclosion time. Two peaks of eclosion dates occurred from the same batch of fertilized eggs in the laboratory without cyclic environmental factors. High culturing temperature results in short interval (duration) between fertilization and eclosion, whereas more days are required at low temperature. The culturing temperature has a significant influence upon the numbers of P. oceana occurring in different eclosion peaks. High first/second peak ratio occurred at high temperatures whereas relatively more eclosed at the second peak at low temperature. The eclosion dates of offspring are not related to their parents with regard to the 2 peaks. There was an corresponding shift in eclosion days in eggs fertilized 2 days apart. It suggested that circasemilunar eclosion times were not caused by cues in the laboratory.
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Mechanism of Circasemilunar Eclosion rhythm of the Marine Midge Pontomyia oceanaLee, Yi-jen 31 July 2002 (has links)
The mechanism of semilunar emergence rhythm of the marine midge, Pontomyia oceana, was investigated. We used night light (1 lux) to entrain the emergence of the midge. Night light of 4 nights or more can effectively synchronize the semilunar emergence. Moreover, the night light has to be given about 10 days after fertilization to be effective. A batch of fertilized eggs of the marine midge emerge in two semilunar cycles, a second round of night-light treatment is necessary to synchronize the second peak of emergence. We also investigate whether the semilunar rhythm is dependent on the daily rhythm of the midge. Using different day length, from 20 to 28 hours per day, with equal light and dark periods, we want to know if the midges are counting numbers of light-dark cycles, or are independent of light-dark cycles, in determining their semilunar emergence. The results were intermediate between the two hypotheses. We suggest that the midge was not affected by light-dark cycle for the first 14 days of their life, afterward they count 15 light-dark cycles before emergence. This also explains how the second emergence peak occurs about 45 days after fertilization.
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Adaptation Mechanism of Eclosion Date Dimorphism in the Marine Midge Pontomyia oceana (Diptera¡GChironomidae)Leu, Yi-Jye 16 July 2001 (has links)
Two peaks of eclosion dates, about 15 days apart, occur in the same batch of fertilized eggs in the marine midge, Pontomyia oceana. Two hypotheses, the variable adaptive peaks and the bet-hedging hypotheses, were proposed as the ultimate factor of the polymorphic phenomenon. They were tested by experiments controlling feeding amount and photoperiod, as well as selective breeding experiments. The offspring eclosing in the two peaks do not differ in fecundities, egg diameters, thorax and head lengths of males; this is not compatible with the variable adaptive peaks hypothesis. Both peaks exist under various feeding and photoperiods, although peak ratios differed in the former. The results in the first peak lineage did not support there is genetic component in peak ratio determination. The experiments in the second peak lineage had much lower success rates, although the results seemed to suggest a genetic component. The results in a more extreme selection experiment did not support that there is genetic component either. The present results are more compatible with the bet-hedging hypothesis. Wind velocity may be a factor hard to predict by the midges, and it may cause reproductive failure of them. Whereas high emergence synchronization, a prominent feature of the marine midge, may have advantages in many aspects, it also concentrates the risk of total reproductive failure. Spreading offspring to more than one suitable eclosion peak, the midge may have sacrificed short-term reproductive rate for long-term fitness.
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