Abstract
The circadian rhythm is an endogenous rhythm with a period of approximately 24 h. Organisms, including insects, possess the rhythm to live with the daily environmental and ecological cycles. This chapter describes and discusses the general characteristics and properties of circadian rhythms. The rhythm is driven by the circadian clock system that often consists of two or more clocks, synchronizing to the environmental cycles to set behavioral and physiological events to occur at an appropriate time of day. Insects use various zeitgebers for synchronization with light, which is the most important and powerful approach. Light not only resets the clock in a phase-dependent manner but also has long-lasting aftereffects that are observed in the free-running period and waveform of the rhythm. Constituent clocks form bilaterally paired or hierarchical structures that are important to adapt to environmental cycles with seasonal or day-to-day changes.
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1 Introduction: Self-Sustaining Rhythm
After the genesis of our planet, organisms have been exposed to daily cyclic environments. To cope with the cyclic changes in the environment has been the most important challenge for the organisms living on this planet. Today, organisms live in ecosystems that are changing daily in terms of not only geophysical but also biological aspects. Thus, organisms, including insects, possess daily rhythms to adapt to the daily changing environment. The rhythm is called a circadian rhythm because it persists with a period near but not exactly 24 h even after organisms are transferred to constant conditions, i.e., constant darkness (DD) or constant light (LL), and at a constant temperature.
Circadian rhythms are expressed in various behaviors, including locomotor (Tomioka and Chiba 1982b), stridulatory (Loher 1972), flight (Clopton 1984), feeding (Xu et al. 2008), oviposition (Loher 1979), egg hatching (Tomioka et al. 1991a), larval molting (Truman 1972; Fujishita and Ishizaki 1981), eclosion (Pittendrigh et al. 1958; Truman 1971), and mating activities (Sakai and Ishida 2001). Physiological functions also show circadian rhythms, including light sensitivity of compound eyes (Tomioka and Chiba 1982a; Wills et al. 1985), visual interneurons (Saifullah and Tomioka 2002; Uemura and Tomioka 2006), chemoreception in antennae (Saifullah and Page 2009), and cuticle formation (Wiedenmann et al. 1986; Ito et al. 2008). Figure 2.1a shows an example of the circadian rhythm of locomotor activity in the adult male cricket Gryllus bimaculatus. In the free-running state, the period is called the free-running period, and the phases corresponding to the original daytime and nighttime are called the subjective day and subjective night, respectively (Fig. 2.1a). The term circadian time (CT) is often used to determine phases in the free-running state. CT0 corresponds to the beginning of the subjective day, and CT12 corresponds to the beginning of the subjective night. Activity onsets are usually used to determine the phase and correspond to CT0 in diurnal insects and to CT12 in nocturnal insects. In this way, the CT of the rhythm is determined by dividing one circadian cycle from the activity onset to the next into 24 h.
The rhythm is essentially generated by an endogenous mechanism called the circadian clock that oscillates with a period of nearly 24 h, but under environmental cycles, it is modified by some direct responses to environmental factors, and the modification is called masking effects. The clock has flexibility to change its phase, period, waveform, or amplitude in response to daily or seasonal changes in environmental cycles. Insects possess two or more circadian clocks that compose bilaterally symmetrical or hierarchical structures, which allow insects to cope with those day-to-day or seasonal changes in daily environmental cycles. This chapter outlines these general features of insect circadian rhythms.
2 Free-Running Period: Dependency on Environmental Conditions
Although the free-running period of the circadian rhythm is generally quite accurate and stable, it changes in response to environmental lighting and temperature conditions. Light usually has significant effects on the free-running period. In vertebrates, J. Aschoff established an empirical rule called Aschoff’s rule for the light dependency of the free-running period: the free-running period is shorter in LL than in DD and becomes shorter with an increase in light intensity in diurnal animals, while the opposite is seen in nocturnal animals (Aschoff 1960; Pittendrigh 1960; Aschoff 1979). This is successfully applicable to most nocturnal insects: the free-running period is shorter in DD than in LL. For example, in the cricket G. bimaculatus, the free-running period under LL is longer than 24 h, which is significantly longer than that under DD (Fig. 2.1) (Tomioka and Chiba 1982b). Similar light-dependent changes in the free-running period have been known for several other nocturnal insect species, including the cockroaches Rhyparobia (Leucophaea) maderae and Periplaneta americana (Roberts 1960) and the beetle Carabus problematicus (Weber 1967), with some exceptions where the free-running period is shorter in LL, e.g., nocturnal pit-building activity in larvae of the ant-lion Myrmeleon obscurus (Youthed and Moran 1969). However, for diurnal insects, several Nasonia wasps are the only species that are thus far known to follow Aschoff’s rule, showing a shorter free-running period in LL than in DD (Bertossa et al. 2013). Most other diurnal insects violate Aschoff’s rule, with the free-running period being shorter under DD than LL. These include the dung beetle Geotrupes sylvaticus (Geisler 1961), the mosquito Aedes aegypti (Taylor and Jones 1969), the bean bug Riptortus pedestris (Numata and Matsui 1988), the blow fly Calliphora vicina (Hong and Saunders 1994), and the fruit fly Drosophila melanogaster (Konopka et al. 1989).
However, spontaneous changes in the free-running period sometimes occur under DD or LL. For example, some of the New Zealand weta Hemideina thoracica show locomotor rhythm free running with a period shorter than 24 h for the first several days in DD, but the period abruptly becomes longer, and in some cases, the period repeatedly becomes longer and shorter (Lewis 1994). Similar repetitive period changes were reported for the brow fly Calliphora vicina kept under DD (Kenny and Saunders 1991) and the onion fly Delia antiqua (Watari and Arai 1997). In the cricket G. bimaculatus, the period initially longer than 24 h after transfer to LL gradually becomes shorter and, in some cases, even shorter than 24 h, as shown under DD (Fig. 2.1b). The gradual period shortening caused by long-term exposure to LL is attributable to a single optic lobe clock, since the period change occurs after unilateral ablation of the optic lobe. This seems not caused by reduced photoreceptor sensitivity because the expression level of the circadian photoreceptor gene (opsin-long wavelength (opLW)) is higher in crickets kept under LL for long term than in those kept under LD (Moriyama et al. 2022).
Under LL, the rhythm often disappears, resulting in behavioral arrhythmicity. It is debatable whether this LL-induced arrhythmicity is attributable to arrest of the clock at a specific phase called singularity, whether the clock maintains its oscillation but its control to overt rhythms is somehow disturbed or whether it is caused by desynchronization of multiple oscillators that control the overt rhythm. With careful experiments in Drosophila pseudoobscura eclosion rhythms, Winfree (1970) found that treatment of Drosophila pupae with 50-sec dim blue light (10 μW/cm2) at 6.8 h after LL/DD transition led the eclosion to be arrhythmic and suggested that the clock can be stopped by falling the oscillation to singularity.
3 Temperature Compensation
The free-running period of the circadian rhythm is well known to be rather stable against changes in temperature. Figure 2.2a shows an example of the temperature independence of the period in the cricket G. bimaculatus. This particular cricket was kept at 25 °C for the first 10 days and then transferred to 20 °C under constant darkness. The average free-running periods were 23.8 h and 22.9 h at 25 °C and 20 °C, respectively (Ikeda and Tomioka 1993). The temperature coefficient Q10 in this species was 0.91, slightly smaller than 1.0. Similar values of Q10 have been reported for the fruit fly D. melanogaster (Fig. 2.2b) (Konopka et al. 1989; Matsumoto et al. 1999), the brow fly C. vicina (Saunders and Hong 2000), and the cockroach R. maderae (Pittendrigh and Caldarola 1973). Biochemical reactions occurring in biological systems, including insects, are temperature-dependent, and Q10 is usually 2.0–3.0. Therefore, there is a mechanism that maintains the free-running period to be constant irrespective of temperature, and the mechanism is called temperature compensation. The exact mechanism of temperature compensation remains to be elucidated. Although there are some possible hypotheses for the mechanism, it is apparently regulated by biochemical reactions because some mutations of clock-related genes, e.g., timelessritu and timelessblind, deeply affect temperature compensation (Fig. 2.2b) (Matsumoto et al. 1999; Singh et al. 2019).
4 Entrainment to Environmental Cycles
One of the most important functions of the circadian clock is to set daily events at an appropriate time of day. To pursue this entrainment, the clock must synchronize to daily environmental cycles. The clock uses some environmental cues, called zeitgebers, to achieve this. Insects use various zeitgebers, including light (Helfrich-Förster 2020), temperature (Tomioka and Yoshii 2006), food (Frisch and Aschoff 1987), and interindividual interactions (Levine et al. 2002). Among these, the most powerful zeitgeber is the light to dark cycle (LD).
When LD is shifted, the rhythm resynchronizes to the newly phased LD by gradual phase advances or delays. Figure 2.3a exemplifies the resynchronization or re-entrainment in the cricket G. bimaculatus. The process of re-enrainment requires several cycles, called transients, to restore the original phase relationship (Pittendrigh 1981a). The existence of transients is a sign of the endogenous nature of rhythm.
The resetting of the clock by light occurs in a circadian time-dependent manner. This trait is explored by experiments with a single light pulse exposure to free-running rhythms under DD. As shown in Fig. 2.3b, c, a light pulse given at early subjective night causes a delay shift of the rhythm, whereas it causes an advance shift when given at late subjective night. On subjective days, the pulse causes little phase shifts. The relationship between the CT at which the light pulse is given and the magnitude of the shifts thus caused is illustrated in the phase response curve (PRC) (Fig. 2.3d). The PRC for circadian rhythms has been obtained in a wide variety of insects, including the fruit flies D. pseudoobscura (Pittendrigh 1960) and D. melanogaster (Orr 1982), the brow flies Lucilia cuprina (Smith 1983) and C. vicina (Cymborowski et al. 1993), the cockroach R. maderae (Wiedenmann 1977), and the cricket G. bimaculatus (Okada et al. 1991). Although the shape of the PRC is basically shared among the tested species, the PRC is classified into two types, type 1 and type 0, based on the amplitude (Fig. 2.3e) (Winfree 1970). Type 1 PRC has low amplitude, and if the time of activity onset is plotted with the phase before the pulse (old phase) on the horizontal axis and the phase after the pulse (new phase) on the vertical axis, the slope of the plot, called the phase transition curve (PTC), is approximately 1. In contrast, type 0 PRC has high amplitude, and the slope of the PTC is approximately 0. The amplitude of PRC depends on the light intensity and duration of light pulses. Thus, the type of PRC could be changed. For example, in the cockroach Nauphoeta cinerea, white light of 3-h duration causes type 1 PRC with low amplitude while that of 12-h duration type 0 PRC with high amplitude (Saunders and Thomson 1977).
5 Range of Entrainment
The rhythm can be entrained to light cycles with periods (Ts) longer or shorter than 24 h but close to 24 h. The PRC predicts not only the phase relationship between the rhythm and the light cycle in a steady-state entrainment but also the range of Ts that can entrain the rhythm. For example, when the cricket G. bimaculatus kept in DD is repetitively given a 3-h light pulse with a period of 26 h, then the cricket’s rhythm could be predicted to synchronize to the cycle as the 3-h light pulse falls at CT 11. This is because a 3-h light pulse falling at CT11 is expected to cause a 2-h delay from the PRC (Fig. 2.3d) so that the period of the cricket’s rhythm, which is close to 24 h, becomes 26 h. The limit of entrainment could also be predicted by the greatest delay and advance shift induced by a light pulse. In the cricket, with a 3-h light pulse, the maximal advance and delay are 2 h and 2.5 h, respectively (Fig. 2.3d) (Okada et al. 1991), so that the predicted range of entrainment is 22 h–26.5 h. The predicted range of entrainment matches well with the experimental results using LDs with L and D of the same duration in the cricket G. bimaculatus; the shorter limit is near T = 21 h, while the longer limit is close to 27 h (Tomioka 1993).
The rhythm is sometimes entrained to or free runs under LD cycles beyond the range of entrainment, e.g., shorter than 24 h, such as 12, 8, and 6 h. However, in such a shorter period, the rhythm rigidly maintains the entrained state or free-running state with a period of or close to 24 h (Fig. 2.4a, b). When entrained to the given LD, the clock reads the given LD cycles into a 24-h cycle. It is also known that the rhythm synchronizes to LD cycles with longer periods, e.g., 48 h. To such LDs, the rhythm entrains by repeating the 24-h rhythm twice or more in a given LD cycle.
6 Relative Coordination
When the power of the zeitgeber is weak, circadian rhythms are not entrained to the zeitgeber but only show a phase-dependent modulation of the free-running period. This state is called relative coordination (Aschoff 1981). Figure 2.4c shows an example of the relative coordination. In this particular case, the locomotor rhythm of the cricket Gryllodes sigillatus was recorded under constant darkness with a temperature cycle of 12 h 20 °C and 12 h 25 °C. The cricket cannot synchronize to the temperature cycle but shows a clear change in the free-running period, which is lengthened at 20 °C but shortened at 25 °C.
Relative coordination can also be observed when the rhythm is exposed to LD cycles outside the range of entrainment, as exemplified in Fig. 2.4d (Tomioka 1993). In this case, the cricket G. bimaculatus is exposed to LD 10.5:10.5 (T = 21 h). The cricket cannot be entrained to the given LD, free running with a relative coordination in which τ fluctuates as a function of the phase angle relationship with the light cycle. The period lengthens when the light onset falls during the subjective day, while it shortens if the light onset occurs during the subjective night.
7 Masking Effect of Light
Light has direct effects on behavior bypassing the clock. For example, lights on and off often modulate the activity rhythm in a time-dependent manner. There are two types of masking effects: positive and negative. Positive masking is an enhancement of activity by light, as shown for the cricket G. bimaculatus in Figs. 2.3a and 2.4a. In the cricket shown in Fig. 2.3a, intense locomotor activity occurred at lights on when the LD cycle was 6 h advanced, but this activity soon disappeared as the rhythm restored the original phase relationship with the shifted LD. Thus, positive masking often occurs in a phase-dependent manner, e.g., during late subjective night to early subjective day for nocturnal animals (Tomioka and Chiba 1987). Negative masking is induced when light is given during the subjective night. When a short LD cycle is given, the locomotor rhythm often free runs, but the light phase strongly suppresses activity during subjective night so that the active phase is divided into pieces (Fig. 2.4b). To determine whether the activity observed under LD is caused by an endogenous clock or exogenous masking of light, the rhythm should be observed after transfer to DD, where endogenous components persist but exogenous masking disappears.
8 Multioscillator System and Internal Desynchronization of Rhythms
The daily temporal rhythms are often controlled by two or more circadian clocks. Splitting of the rhythm into two separately running components is strong evidence for the multioscillator nature of the circadian system. Splitting often occurs spontaneously under constant conditions or is artificially induced by blocking the light input to the clock on one side (Wiedenmann 1983; Tomioka et al. 1991b). Figure 2.5a exemplifies the spontaneous rhythm splitting in the cricket G. bimaculatus kept under LL. The splitting occurred through internal desynchronization of the two clocks. In crickets and cockroaches, the two clocks are located one in each optic lobe (Page 1982, 1983; Tomioka and Chiba 1984, 1992). The bilaterally paired nature of the clocks is revealed by surgical removal of the optic lobe in insects with split rhythms: unilateral lobe removal eliminates either of the two rhythms, often with significant changes in the free-running period of the remaining rhythm (Page 1978; Tomioka et al. 1991b; Lewis 1994). This period change suggests that the period of the system is determined by mutual interaction of the two clocks.
In addition to the bilaterally paired organization, there is a system with clocks that have a hierarchical relationship. The best-known clock system is that of the fruit fly D. pseudoobscura, which regulates eclosion rhythms. Adult emergence from pupal cases occurs in the early morning in D. pseudoobscura. With light pulse and temperature pulse experiments, the underlying regulatory mechanism was revealed to include a light-sensitive circadian oscillator (A oscillator) and a temperature-sensitive oscillator (B oscillator) (Pittendrigh 1981b). In this A-B two-oscillator model, the A oscillator is the master, entraining the B oscillator, which is the slave and determines the timing of eclosion (Fig. 2.5b). Light resets the A oscillator immediately but not the B oscillator, which gradually restores the original phase relationship with the A oscillator through the entraining effect from the A oscillator (Tackenberg et al. 2017). The resynchronizing process of the B oscillator appears as transients.
9 Aftereffects
The circadian rhythm is genetically programmed, and insects show the rhythm without experiencing any periodic environment. However, the rhythm is known to change its waveform to tune to a given photoperiod (Pittendrigh and Daan 1976). Figure 2.6 exemplifies the waveform modulation by entrainment to LDs of variable L-to-D ratios in the cricket G. bimaculatus (Koga et al. 2005). When experiencing longer light phases, the ratio of the active phase to the rest phase (α/ρ-ratio) was smaller, and the free-running period was shorter. The magnitude of changes in the α/ρ ratio was dependent on the number of cycles experienced. These phenomena are comparable to the aftereffects found in vertebrates: the white-footed mouse, Peromyscus leucopus, for example, the subjective night length and the free-running period were clearly dependent on the light cycle in which the animal had been exposed (Pittendrigh and Daan 1976). In vertebrates, these changes in the free-running period and circadian waveform are explained by photoperiod-dependent changes in the coupling state of two circadian oscillators, which regulate the lights-on (morning) peak and lights-off (evening) peak, respectively (Pittendrigh and Daan 1976). Additionally, in insects, there are some lines of evidence suggesting a similar role of oscillator coupling in controlling the circadian waveform (Wiedenmann and Loher 1984; Helfrich-Förster 2001; Koga et al. 2005). However, the waveform modulation could be attributable at least in part to a single optic lobe clock because the modulated waveform persisted in isolated and cultured optic lobes (Koga et al. 2005). More clear evidence for this was obtained in the cockroach R. maderae: experience of T cycles with a period longer or shorter than 24 h causes long-lasting changes in the period of optic lobe clocks, and the change was maintained even after the optic lobe was transplanted to another individual (Page 1982, 1983). A remaining important issue is how these history-dependent changes occur and are maintained. This question deserves to be solved at the cellular and molecular levels.
10 Future Perspectives
As we have seen in this chapter, circadian rhythms have properties unique to biological rhythms. These properties were previously explored behaviorally and physiologically but are now being studied at cellular and molecular levels. In particular, the oscillatory and photic entrainment mechanisms of the circadian clock are already largely understood, albeit for some insects, including D. melanogaster. These will be discussed in other chapters. However, there are still some unresolved issues, such as temperature compensation and aftereffects. Comprehensive analysis of genes by next-generation sequencers and regulation of gene expression by RNAi and gene editing techniques are now widely used in studies on insect circadian rhythms. These innovations in circadian rhythm research are expected to help us to deepen our understanding of the various properties of clocks and their adaptive significance.
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Tomioka, K. (2023). General Feature of Circadian Rhythms. In: Numata, H., Tomioka, K. (eds) Insect Chronobiology. Entomology Monographs. Springer, Singapore. https://doi.org/10.1007/978-981-99-0726-7_2
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