Effects of altitude on circadian rhythm of adult locomotor activity in Himalayan strains of Drosophila helvetica

Latitude and altitude of origin are known to modify fundamental properties of the pacemaker controlling circadian rhythms of eclosion, oviposition and adult locomotor activity of naturally occurring clock phenotypes of Drosophila [1]. For example, latitude of origin dramatically altered the basic parameters of eclosion rhythm of the Japanese strains of D. auraria [2,3], the European strains of D. littoralis [4-6] and D. subobscura [7]. Variability in properties of eclosion and adult locomotor activity rhythms of D. ananassae strains captured from Sri Lanka and India were accounted for by the environmental conditions prevailing at the latitude of origin [8,9]. Molecular polymorphism in the period gene of latitudinal strains of D. melanogaster, D. littoralis and D. simulans captured in Europe, Africa and Australia was ascribed to natural selection [1,10-13]. Variation in patterns of adult locomotor activity of eleven species of Drosophila originating from across the United States were attributed to the latitude of origin and the physical nature of the breeding site [14].

Studies on the altitudinal variation in the circadian physiology of Drosophila are rather few as compared to those on latitudinal variation. For example, altitudinal variation in photoperiodic response to diapause and the number of generations per year were studied in strains of four Drosophila species from Japan [15]. Genetic components for the altitudinal differences in oviposition rhythm were analyzed by carrying out crosses within and between populations of D. buzzatii that originated from different altitudes in Argentina [16]. Altitude of origin also modified the pacemaker properties controlling eclosion and oviposition rhythms of D. ananassae strains [17-21]. The present experiments were designed to determine whether or not the altitude of origin affected the parameters of entrainment and free-running rhythm of adult locomotor activity of D. helvetica strains originating from different altitudes in the Himalayas.

Laboratory populations of the high altitude Himalayan (haH) strain of D. helvetica (Burla, 1948) originating from Hemkund-Sahib (4,121 m above sea level, 30.81°N, 79.81°E) and the low altitude Himalayan (laH) strain originating from Birahi (1,132 m a.s.l., 30.62°N, 79.65°E) were derived from 21 and 15 wild-caught gravid females in the field, respectively, in April 2005. Thus, they were genetic representatives of the populations from their breeding sites in nature. Flies were maintained on standard cornmeal medium at 20°C (± 0.5°C) and ~60% relative humidity under cycles of 12 h of white light at 100 lux and 12 h of complete darkness (LD 12:12). Males of these strains were used for assaying the adult locomotor activity in the field and laboratory. The activity rhythm of individual flies was monitored by the computerized method described elsewhere in detail [8]. The method in brief is as follows: Activity of an individual male was monitored by placing the fly into a glass tube (length × outer diameter: 100 × 7 mm). One end of the tube was inserted into a container having 10 g of culture medium and the other end was plugged with cotton. The tube was placed in the path of an infrared beam. The culture medium was replenished once a week. Interruption of the infrared beam by fly movement triggered an all-or-none electronic signal that was amplified, counted, accumulated and then registered every 6 min on the hard disk of a computer.

Onset of activity was considered as the phase reference point of the rhythm because it was a more precise and predictable phase point than the mid-point or end of activity. The phase of activity onset (Ψ_o) was defined as the time from the sunrise in the field or lights-on of LD 12:12 cycles in the laboratory to the time of activity onset as given by an eye-fitted line to 11 successive activity onsets. The phase of activity termination (Ψ_e) was defined as the time from the sunset in the field or lights-off of LD 12:12 cycles in the laboratory to the time of end of activity as given by an eye-fitted line to 11 successive activity offsets. The interval (Ψ_M-E) between the morning peak and evening peak during entrainment was measured by eye-fitted lines to the offsets of morning peaks and onsets of evening peaks for 11 days. Activity phase (α) was regarded as the average interval between two eye-fitted lines joining 11 activity onsets and 11 activity offsets. The rest phase (ρ) was calculated by subtracting α from 24 h during entrainment or from the period of free-running rhythm (τ) in constant darkness (DD). τ was determined by fitting least square regression line to 11 successive activity onsets during steady-state free-runs. Total activity per cycle (TAPC) in each strain was determined by taking the average number of activity passes from the pooled data of 21 flies for 11 days during entrainment or free-running state. When entrained by natural LD 14.1:9.9 cycles in the field or artificial LD 12:12 cycles in the laboratory, the activity peaks of each strain were restricted to specific times of the photophase. Thus, it was possible to divide the natural photophase of 14.1 h or the artificial photophase of 12 h equally into three sectors: morning, midday and evening. A fly was considered to have the morning, midday and/or evening peak of activity if the activity passes in the given part of the photophase were > 30% of the TAPC.

Parameters of entrainment and free-running rhythm were assayed in 21 males (age: 3 days post-eclosion) of each strain in two sets of experiments. The first set of experiments was performed simultaneously at the breeding site of each strain in the field to study the natural entrainment patterns of these strains in LD cycles under two temperature regimes, the naturally fluctuating temperature (NFT) and at constant temperature (CT) of 20 ± 0.5°C. Initially five culture bottles (10 adults of each gender per bottle) and 21 activity monitoring units were housed in each of two identical glass-enclosures (2 × 2 × 2 m) which were uniformly exposed to direct sunlight at the breeding site of each strain. Cross ventilation in each glass-enclosure was achieved by two screened openings (15 × 15 cm). Maintenance (i.e., transferring flies to the bottles containing fresh culture medium, changing the culture medium in the containers of activity recording units, etc.) was carried out by manipulation through two sleeves attached to round openings (21 cm diameter) in each glass enclosure. Flies were bred for one generation and then entrainment was studied in adults of the next generation at the same temperature regime in which they were reared. Flies in the first glass enclosure were exposed to the NFT regime. Flies in the second glass enclosure were exposed to the CT at 20 ± 0.5°C by connecting both of the enclosure openings to a split air-conditioning machine whose thermostat was kept at 20°C. Relative humidity in all four glass enclosures was 60 ± 10%, as both breeding sites were surrounded by moist vegetation. Data on adult locomotor activity of both strains were obtained in July 2005 when the natural photoperiod was ~14 h. Temperature, relative humidity and light intensity were recorded continuously.

A second set of experiments examined the entrainment and free-running rhythm parameters at 20 ± 0.5°C and ~60 % relative humidity in the laboratory. Entrainment was studied in LD 12:12 cycles (100 lux during L and complete darkness during D) for 11 days, and then the flies were transferred to DD to determine τ. Effects of altitude and temperature on Ψ_o, Ψ_e, Ψ_M-E, α/ρ ratio, TAPC and τ of both strains were compared by t-tests.

Figure 1 illustrates the activity records of representative males of each strain in actogram format and the mean entrainment pattern of 21 males of each strain for 11 days in histogram format. Mean values of five entrainment parameters of these strains are given in Table 1. Although both strains were entrained by natural LD cycles in the NFT and CT regimes, the altitude of origin altered the uni/bimodality of the activity pattern (Figure 1) and the other four parameters of entrainment of the haH strain (Table 1). The haH strain had unimodal activity pattern with a single delayed peak that commenced in the forenoon and continued till evening, while the laH strain had bimodal activity pattern with early morning peak that was separated from the evening peak by a period of inactivity of ~4 h (Figure 1A–H). Figure 2 gives profiles for the natural light intensity and environmental temperature obtained at the breeding site of each strain in the NFT regime. Although light intensity profiles at the two breeding sites were almost similar, the temperature profiles were strikingly different, as the temperature varied from ~7 to 21°C at the high altitude (Figure 2A) but from ~20 to 33°C at the low altitude (Figure 2B). Figure 3 gives almost similar profiles for the natural light intensity obtained at the breeding sites of these strains under the CT regime at 20 ± 0.5°C. Ambient temperature did not affect the Ψ_o of either strain and Ψ_e of the laH strain but it affected the Ψ_e of the haH strain as it was postponed by ~2 h in the CT regime (Figures 2 and 3, Table 1). Ambient temperature also affected the Ψ_M-E of the laH strain as it was reduced by ~3 h in the CT regime as compare to that in the NFT regime (Figure 1E–H, Table 1). The reduction in Ψ_M-E was caused by the addition of activity at the end of the morning peak and at the beginning of the evening peak (Figure 1G, H).

Both strains of D. helvetica were also entrained by LD 12:12 cycles at 20 ± 0.5°C in the laboratory. Figure 4 shows the double plotted activity records of the representative male of each strain and Figure 5 illustrates the mean entrainment pattern of 21 males of each strain for 11 days. Values of Ψ_o, Ψ_e, α/ρ ratio and the TAPC of both strains are summarized in Table 2. Entrainment parameters of both strains followed the same trend as that exhibited during entrainment to natural LD cycles in the field. Altitude of origin significantly affected Ψ_o, Ψ_e, α/ρ and TAPC (p < 0.01) of these strains in LD 12:12 cycles. Transfers from LD 12:12 cycles to DD were always followed by 2–3 transient cycles before steady state free-running rhythms were established in each strain (Figure 4). Although both strains exhibited free-running rhythmicity with a unimodal activity pattern, the values of τ and TAPC differed significantly (p < 0.01) (Table 2). The unimodal activity pattern of the haH strain was retained during the transient cycles and subsequent steady-state free-runs in DD. However, the bimodal activity pattern was abolished in all males of the laH strain immediately after the LD 12:12 to DD transfer, as the evening peak disappeared. The morning peak was retained during transient cycles and in subsequent steady-state free-runs.

Altitude of origin delayed the phase of activity onset of the haH strain of D. helvetica by ~6 h when compared to that of the laH strain in all entraining LD cycles in the field and laboratory. Failure of the haH flies to begin activity before sunrise in the field like the laH flies (Figure 1) might be due to the masking effect [22] of 'non-permissible' low temperature (~9°C) in the field at sunrise (Figure 2A). This possibility should be ruled out because the 'permissible' temperature at 20°C at sunrise, as imposed in the CT regime, failed to advance the Ψ_o of this strain (Figure 3A). It appears that the lights-on transition of LD cycles was the phase determining photic signal for the haH flies to initiate activity as they also commenced activity ~4.5 h after lights-on of LD 12:12 cycles (100 lux during L) (Figure 4A). Even the increment in light intensity of the photophase from 100 to 500 lux or the increment in duration of the photophase from 12 to 14 h failed to advance the Ψ_o of this strain (in preparation). The laH flies, however, initiated activity ~1 h before lights-on of all entraining light-dark cycles. Thus, these results demonstrate that the altitude of origin altered the Ψ_o of the haH strain. Moreover, the lights-on transition appears to be the photic signal of LD cycles for timing the phase of activity onset in both these strains. Three reference points of photophase – namely, the lights-on, lights-off and midpoint – are useful in determining the activity onset in various insects [23].

The activity pattern and the phase of activity onset during entrainment seem to have adaptive relevance in Drosophila [8]. The unimodal activity pattern with a delayed phase of activity onset in the haH strain of D. helvetica may be the result of natural selection to avoid low temperature in the morning at the high altitude of its origin. High altitude Himalayan strains (1,321 to 2,346 m a. s. l.) of D. ananassae were also characterized by a unimodal activity pattern with a delayed activity peak occurring late in the morning [8]. Low temperature and decreased barometric pressure at high altitude are reported to reduce walking speed and flight performance in D. melanogaster [24]. The laH strain of D. helvetica, however, showed a bimodal activity pattern in which the early morning peak was separated from the evening peak by a period of ~4 h of inactivity in the noon which should be considered as the result of natural selection so that these flies would take advantage of the relatively cooler part of the day in the morning hours for foraging, mating, etc. but would avoid desiccation on exposure to relatively high temperature at noon at its breeding site in the field. Forty-two low altitudinal strains of D. ananassae originating from the western coast of India (0 m, a. s. l.) had bimodal activity patterns with early morning peaks [8]. Females of a Drosophila parasitic wasp, Leptopilina heterostoma, from southern regions had bimodality with morning and evening activity peaks, while the northern strains were active mostly during the afternoon [25].

Altitude of origin also altered the phase of activity termination of the haH strain of D. helvetica as it was labile and temperature dependent unlike that of the laH strain. The haH flies ceased activity about one hour prior to sunset in the NFT regime when the environmental temperature was ~14°C (Figure 2A). Early cessation of activity of the haH strain in the field might be the result of negative masking by temperature which rapidly falls in the rarefied air at the high altitude of its breeding site. When this strain was subjected to the permissible temperature at 20°C as in the CT regime in the field, its activity was extended by ~2 h as compared to that in the NFT regime. Similarly, its activity ceased ~1 h after lights-off when entrained by LD 12:12 cycles (100 lux during L) (Figure 4A) or by LD cycles in which the photophase (500 lux during L) varied from 10 to 14 h per 24 h at 20°C (in preparation). These results suggest that the termination of activity of the haH strain was labile and temperature dependent. By contrast, the laH strain terminated activity ~0.4 h after sunset during entrainment to all natural and artificial LD cycles, as mentioned above, suggesting that its Ψ_e was rigid.

In order to confirm that the delayed Ψ_o of the haH strain or the advanced Ψ_o of the laH strain of D. helvetica were not simply a consequence of an exogenous response to lights-on or lights-off transitions of light-dark cycles, the flies entrained by LD 12:12 cycles were transferred to DD to determine the period of free-running rhythm, which is the most reliable property of the underlying circadian pacemaker. The altitude of origin indeed affected τ of the haH strain as it was about 4.5 h longer than that of the laH strain (Table 2). In general, an advanced Ψ_o is correlated with short τ and delayed Ψ_o with long τ, as predicted from the model formulated for explaining the relationship among eclosion rhythm parameters of D. pseudoobscura [26]. The present results on D. helvetica strains agree with this model, and the difference in Ψ_o of these strains could be made clear by considering the different τ s of these strains. The haH strain with long τ and laH strain with short τ are expected to phase lag and phase advance, respectively, when entrained by LD 12:12 cycles. That is exactly what we observed. Altitude of origin also affected the τ of eclosion and oviposition rhythms of D. ananassae strains [17,19]. Latitude of origin as well influenced τ of eclosion rhythm of D. littoralis [5], D. subobscura [7] and D. ananassae [9,20,21].

This appears to be the first report analyzing the effects of high altitude of origin on the circadian locomotor activity of D. helvetica. Parameters of entrainment and free-running rhythm of the haH strain of D. helvetica are unique among known Drosophila species. Its delayed but rigid phase of activity onset that refers to the lights-on transition of entraining photophase and the early but labile phase of activity termination that could be postponed by high temperature should be regarded as behavioral adaptations in response to the low temperature and other environmental conditions prevailing at the high altitude of its breeding site which have profoundly influenced the evolution of the pacemaker controlling its locomotor activity rhythm.

α, activity phase; α/ρ, ratio of activity phase to rest phase; CT, constant temperature; τ, period of free running rhythm under constant conditions; NFT, naturally fluctuating temperature; Ψ_o, phase of activity onset; Ψ_e, phase of activity end; Ψ_M-E, interval between morning and evening peaks; ρ, rest phase; TAPC, total activity passes per cycle

The author(s) declare that they have no competing interests.

KVL performed the experiments with the help of CV and MKS, and all three prepared the initial draft of the manuscript. SBI fabricated and maintained the Drosophila activity units, related hardware and software. MSK and AJS statistically analyzed the data. RJB and DSJ conceived and supervised the experiments. All authors approved the final version of the manuscript.

Keny Vanlalhriatpuia, Email: dsjoshi_anr@sancharnet.in.

Vanlalnghaka Chhakchhuak, Email: dsjoshi_anr@sancharnet.in.

Satralkar K Moses, Email: dsjoshi_anr@sancharnet.in.

SB Iyyer, Email: dsjoshi_anr@sancharnet.in.

MS Kasture, Email: dsjoshi_anr@sancharnet.in.

AJ Shivagaje, Email: dsjoshi_anr@sancharnet.in.

Barnabas J Rajneesh, Email: dsjoshi_anr@sancharnet.in.

Dilip S Joshi, Email: dsjoshi_anr@sancharnet.in.