Comparative aspects of the calcium-sensitive photoproteins aequorin and obelin.

1. The calcium-dependency of the process of light emission has been investigated for the photoproteins aequorin and obelin. 2. The experimental curves of light production, expressed as a percentage of the maximal rate of utilisation, versus pCa are accurately predicted by the cooperative action of at least 2Ca-2+ for aequorin and at least 3Ca-2+ for obelin. 3. At low total monovalent cation concentrations, a pH change from 6.8 to 7.1 shifts the light production vs pCa curve by approx. 0.2 pCa units to the right for aequorin, while that for obelin is shifted by some 0.37 pCa units. 4. Other monovalent cations, such as Na+ are able to compete with Ca-2+ for the active sites of aequorin and also shift the light production vs pCa curve to the right. There is no apparent change in the calcium stoichiometry for light production under these conditions. 5. The same calcium stoichiometry for light emission was also obtained for aequorin or obelin in the presence of either unbuffered Ca-2+ solutions or of calcium/EGTA buffers.     

Comparative aspects of the calcium-sensitive photoproteins aequorin and obelin

1. The calcium-dependency of the process of light emission has been investigated for the photoproteins aequorin and obelin.2. The experimental curves of light production, expressed as a percentage of the maximal rate of utilisation, versus pCa are accurately predicted by the cooperative action of at least 2Ca²⁺ for aequorin and at least 3Ca²⁺ for obelin.3. At low total monovalent cation concentrations, a pH change from 6.8 to 7.1 shifts the light production vs pCa curve by approx. 0.2 pCa units to the right for aequorin, while that for obelin is shifted by some 0.37 pCa units.4. Other monovalent cations, such as Na⁺ are able to compete with Ca²⁺ for the active sites of aequorin and also shift the light production vs pCa curve to the right. There is no apparent change in the calcium stoichiometry for light production under these conditions.5. The same calcium stoichiometry for light emission was also obtained for aequorin or obelin in the presence of either unbuffered Ca²⁺ solutions or of calcium/EGTA buffers.     

Changes in Intracellular Free Calcium Concentration during Illumination of Invertebrate Photoreceptors : Detection with Aequorin

Aequorin, which luminesces in the presence of calcium, was injected into photoreceptor cells of Limulus ventral eye. A bright light stimulus elicited a large increase in aequorin luminescence, the aequorin response, indicating a rise of intracellular calcium ion concentration, Ca_i. The aequorin response reached a maximum after the peak of the electrical response of the photoreceptor, decayed during a prolonged stimulus, and returned to an undetectable level in the dark. Reduction of Ca_o reduced the amplitude of the aequorin response by a factor no greater than 3. Raising Ca_o increased the amplitude of the aequorin response. The aequorin response became smaller when membrane voltage was clamped to successively more positive values. These results indicate that the stimulus-induced rise of Ca_i may be due in part to a light-induced influx of Ca and in part to release of Ca from an intracellular store. Our findings are consistent with the hypothesis that a rise in Ca_i is a step in the sequence of events underlying light-adaptation in Limulus ventral photoreceptors. Aequorin was also injected into photoreceptors of Balanus. The aequorin responses were similar to those recorded from Limulus cells in all but two ways: (a) A large sustained aequorin luminescence was measured during a prolonged stimulus, and (b) removal of extracellular calcium reduced the aequorin response to an undetectable level.     

Comparison of the changes in cytoplasmic free calcium concentration induced by phenylephrine, vasopressin and angiotensin II in hepatocytes

Effects of phenylephrine, vasopressin and angiotensin II on cytoplasmic free calcium concentration, [Ca2+]c, were examined by monitoring aequorin bioluminescence in isolated hepatocytes preloaded with aequorin. In the presence of 0.5 mM calcium in the medium, the pattern of changes in aequorin bioluminescence induced by phenylephrine was different from that induced by vasopressin or angiotensin II. When extracellular calcium concentration was reduced to 1 microM, however, these three agents induced identical changes in aequorin bioluminescence. These results suggest that the mode of action of phenylephrine on cytoplasmic free calcium concentration differs from that of either vasopressin or angiotensin II and that the difference in ability to increase calcium influx may account for the distinct patterns induced by these agents.     

The effect of physiologically occurring cations upon aequorin light emission. Determination of the binding constants.

1. The effect of K+, Na+, Mg2+ and pH upon the rate of aequorin utilization has been investigated in the presence of Ca2+. 2. The aequorin light emission in a medium simulating the in vivo cationic conditions for barnacle muscle fibres indicates that two Ca2+ are apparently involved in this process for free calcium concentrations higher than approx. 10(-5) M. However, for free calcium concentrations lower than 10(-6) M, the intensity of light emitted by aequorin shows a steeper dependency upon [Ca2+] than the square low relationship, indicating that a third Ca2+ should be involved in the process of aequorin light emission, as it has been previously predicted (Moisescu, D.G., Ashley, C.C. and Campbell, A.K. (1975) Biochim. Biophys. Acta. 396, 133-140). 3. The inhibitory effect of physiologically occurring cations upon the aequorin light emission can be explained by the cooperative action of two cations, competing with Ca2+ for the reactive sites on aequorin. 4. At a given concentration, Na2+ was found to have a stronger inhibitory effect upon the aequoring light emission than K+. 5. The experiments indicate a strong interaction between Na+ and K+ in this inhibitory process, since for a given total concentration of monovalent cations, a mixture containing both Na+ and K+ has a larger inhibitory effect on the aequorin light response than solutions containing either Na+ or K+ alone. 6. All other interactions between K+, Na+, H+ and Mg2+ appear to be weak. 7. The reaction schemes used for the explanation of these and other published results on aequorin (Moisescu, D.G., Ashley, C.C. and Campbell, A.K. (1975) Biochim. Biophys, Acta 396, 133-140 and Blinks, J.R. (1973) Eur. J. Cardiol. 1, 135-142) are described, and the 'absolute' binding constants of all physiologically occurring cations for aequorin have been determined. 8. Based on these parameters one can make accurate quantitative predictions for the aequoring light response under a variety of ionic conditions, and this suggests that it is possible to determine absolute free calcium concentrations providing that the ionic composition of the solutions is known, and that the relative rate of aequorin utilization is higher than 0.005.     

Effect of anaesthetics on calcium-induced luminescence of aequorin

The effect of some general and local anaesthetics on the calcium-induced luminescence of aequorin was studied in vitro using a photomultiplier tube and recording technique. Purified aequorin (0.1 microliter) was injected into a 500 micron diameter porous cellulose acetate capillary tube containing 0.5 M KC1, 20 mM phosphate (pH 7.2) and calcium-EGTA buffers. The trapped aequorin was superfused with buffer solutions which sometimes contained anaesthetic (test) solutions. The results showed that some anaesthetics, e.g. urethane, etomidate and lignocaine, increased whereas others, e.g. methohexitone, thiopentone, decreased the light output (luminescence) of aequorin in constant ionized calcium and EGTA buffers. Similar results were produced by some non-anaesthetic drugs, e.g. glycerol, TEA, caffeine, etc. Concentration-response curves for calcium-dependent and -independent luminescence of aequorin showed that anaesthetics variously affected the aequorin response. Some anaesthetics, e.g. lignocaine, increased the maximum response while others, e.g. etomidate, increased the affinity (i.e. decreased EC50s) of aequorin to calcium ions without altering the slope, which remained at about 2. It was concluded that anaesthetics can either excite or depress aequorin luminescence, the effect being dependent on the type and the concentration used.     

Kinetic investigations in single muscle fibres using luminescent and fluorescent Ca2+ probes

The Ca2+-sensitive photoprotein aequorin and the Ca2+-dependent fluorescent indicators quin 2 and TnCDANZ have been used to investigate contractile processes in single crustacean muscle fibres. The investigations with quin 2 indicate that the free Ca2+ rises to a maximum value before peak force as with aequorin light (approximately 200 msec delay at 12 degrees C) and subsequently decays more slowly, unlike the majority of the aequorin signal, although an aequorin 'tail' signal remains. The resting quin 2 fluorescence from the cell suggests an upper limit of 348 nM for the resting calcium concentration. Experiments with TnCDANZ indicate that this fluorescence response rises rapidly but then the rate of rise slows to reach a maximum value at a time when peak force is achieved and then the fluorescence signal decays more slowly than force. The latter result implies that Ca2+ is attached to the Ca2+-specific sites of TnC when externally recorded force is small.     

A direct demonstration that inositol-trisphosphate induces an increase in intracellular calcium in Limulus photoreceptors

Inositol-trisphosphate was pressure-injected into Limulus ventral photoreceptors; these injections induced electrical responses that mimic several aspects of the electrical responses induced by light. Single cells were also injected with aequorin. Injections of inositol-trisphosphate into such cells induced an increase in luminescence from the intracellular aequorin, even in the absence of extracellular calcium ions. These aequorin responses show directly that inositol-trisphosphate induces an increase in ionized calcium concentration within intact and functioning cells that arises from release of calcium ions from intracellular stores.     

Simultaneous measurement of Ca2+ in muscle with Ca electrodes and aequorin. Diffusible cytoplasmic constituent reduces Ca(2+)-independent luminescence of aequorin

Estimates of cytoplasmic Ca2+ concentration ([Ca2+]i) were made essentially simultaneously in the same intact frog skeletal muscle fibers with aequorin and with Ca-selective microelectrodes. In healthy fibers under truly resting conditions [Ca2+]i was too low to be measured reliably with either technique. The calibration curves for both indicators were essentially flat in this range of [Ca2+], and the aequorin light signal was uniformly below the level to be expected in the total absence of Ca2+. When [Ca2+]i had been raised to a stable level below the threshold for contracture by increasing [K+]o to 12.5 mM, [Ca2+]i was 38 nM according to aequorin and 59 nM according to the Ca-selective microelectrodes. These values are not significantly different. Our estimates of [Ca2+]i are lower than most others obtained with microelectrodes, probably because the presence of aequorin in the cells allowed us to detect damaging microelectrode impalements that otherwise we would have had no reason to reject. The observation that the light emission from aequorin-injected fibers in normal Ringer solution was below the level expected from the Ca(2+)-independent luminescence of aequorin in vitro was investigated further, with the conclusion that the myoplasm contains a diffusible macromolecule (between 10 and 30 kD) that interacts with aequorin to reduce light emission in the absence of Ca2+.     

Oscillations of calcium ion concentrations in Physarum polycephalum

Aequorin is a photoprotein which emits light in response to changes in free calcium concentration. When aequorin was microinjected into plasmodia of Physarum polycephalum, light emission varied in synchrony with the motile oscillations of the organisms. Therefore, movement is correlated which changes in the concentration of free calcium.     

Insulation of the conduction pathway of muscle transverse tubule calcium channels from the surface charge of bilayer phospholipid

Functional calcium channels present in purified skeletal muscle transverse tubules were inserted into planar phospholipid bilayers composed of the neutral lipid phosphatidylethanolamine (PE), the negatively charged lipid phosphatidylserine (PS), and mixtures of both. The lengthening of the mean open time and stabilization of single channel fluctuations under constant holding potentials was accomplished by the use of the agonist Bay K8644. It was found that the barium current carried through the channel saturates as a function of the BaCl2 concentration at a maximum current of 0.6 pA (at a holding potential of 0 mV) and a half-saturation value of 40 mM. Under saturation, the slope conductance of the channel is 20 pS at voltages more negative than -50 mV and 13 pS at a holding potential of 0 mV. At barium concentrations above and below the half-saturation point, the open channel currents were independent of the bilayer mole fraction of PS from XPS = 0 (pure PE) to XPS = 1.0 (pure PS). It is shown that in the absence of barium, the calcium channel transports sodium or potassium ions (P Na/PK = 1.4) at saturating rates higher than those for barium alone. The sodium conductance in pure PE bilayers saturates as a function of NaCl concentration, following a curve that can be described as a rectangular hyperbola with a half-saturation value of 200 mM and a maximum conductance of 68 pS (slope conductance at a holding potential of 0 mV). In pure PS bilayers, the sodium conductance is about twice that measured in PE at concentrations below 100 mM NaCl. The maximum channel conductance at high ionic strength is unaffected by the lipid charge. This effect at low ionic strength was analyzed according to J. Bell and C. Miller (1984. Biophysical Journal. 45:279-287) and interpreted as if the conduction pathway of the calcium channel were separated from the bilayer lipid by approximately 20 A. This distance thereby effectively insulates the ion entry to the channel from the bulk of the bilayer lipid surface charge. Current vs. voltage curves measured in NaCl in pure PE and pure PS show that similarly small surface charge effects are present in both inward and outward currents. This suggests that the same conduction insulation is present at both ends of the calcium channel.     

Ionized calcium concentrations in squid axons

Values for ionized [Ca] in squid axons were obtained by measuring the light emission from a 0.1-mul drop of aequorin confined to a plastic dialysis tube of 140-mum diameter located axially. Ionized Ca had a mean value of 20 x 10(-9) M as judged by the subsequent introduction of CaEGTA/EGTA buffer (ratio ca. 0.1) into the axoplasm, and light measurement on a second aequorin drop. Ionized Ca in axoplasma was also measured by introducing arsenazo dye into an axon by injection and measuring the Ca complex of such a dye by multichannel spectrophotometry. Values so obtained were ca. 50 x 10(-9) M as calibrated against CaEGTA/EGTA buffer mixtures. Wth a freshly isolated axon in 10 mM Ca seawater, the aequorin glow invariably increased with time; a seawater [Ca] of 2-3 mM allowed a steady state with respect to [Ca]. Replacement of Na+ in seawater with choline led to a large increase in light emission from aequorin. Li seawater partially reversed this change and the reintroduction of Na+ brought light levels back to their initial value. Stimulation at 60/s for 2-5 min produced an increase in aequorin glow about 0.1% of that represented by the known Ca influx, suggesting operationally the presence of substantial Ca buffering. Treatment of an axon with CN produced a very large increase in aequorin glow and in Ca arsenazo formation only if the external seawater contained Ca.     

A chemical method for intracellular loading of the calcium indicator aequorin in mammalian skeletal muscle.

The bioluminescent calcium indicator aequorin was loaded into bundles of skeletal muscle fibers from the rat extensor digitorum longus by macroinjection, a technique previously applied only to cardiac muscle. After loading, the amplitude and time course of the twitch returned to control values, indicating lack of damage to the fibers. Individual light signals (i.e., calcium transients) were recorded during each twitch or tetanus without the need for signal averaging. The calcium transients obtained were qualitatively and quantitatively similar to those reported previously with microinjection of aequorin. Our data suggest that macroinjection may be the method of choice for loading aequorin into mammalian skeletal muscle.     

The effect of alcohols on aequorin luminescence

The effect of alcohols from ethanol to octanol on aequorin luminescence was biphasic; enhancement of both peak light and total photon yield at low concentrations, and inhibition of these parameters at high concentrations. The potency of alcohols to exert these effects was in the same order as the oil/water partition coefficients of the alcohols. It is argued that neither of these effects is related to calcium binding by aequorin, since alcohols enhanced calcium-independent luminescence, and the inhibition of responses is not associated with a reduction in the rate of aequorin 'consumption' on binding of calcium.     

Bioluminescence and secondary structure properties of aequorin mutants produced for site-specific conjugation and immobilization

Aequorin is one of several photoproteins that emits visible light upon binding to calcium ions. It has been widely used as a Ca(2+)-indicator and as an alternative highly sensitive bioluminescent label in binding assays. The apoprotein of aequorin binds an imidazopyrazine compound (coelenterazine) and molecular oxygen to form a stable photoprotein complex. Upon addition of calcium, the photoprotein undergoes a conformational change leading to the oxidation of the chromophore with the release of CO(2) and blue light. To gain more information of structure-function relationships within the photoprotein that will aid in the design of mutants suitable for site-specific conjugation and immobilization, polymerase chain reaction (PCR)-based site-directed mutagenesis was employed to produce five different aequorin mutants. The five mutants included a cysteine-free mutant and four other mutants with single cysteine residues at selected positions within the protein. The aequorin mutants exhibited different bioluminescence emission characteristics with two mutants showing a decrease in relative light production in comparison to the cysteine-free mutant. Additionally, circular dichroism (CD) spectra revealed that the single amino acid substitutions made for two of the aequorin mutants did alter their secondary structures.     

Dissociation of changes in apparent myofibrillar Ca2+ sensitivity and twitch relaxation induced by adrenergic and cholinergic stimulation in isolated ferret cardiac muscle

In isolated, aequorin-injected ferret cardiac muscle we measured the apparent myofilament Ca2+ sensitivity and its relationship to twitch relaxation time in the presence of autonomic perturbations. The Ca2+-tension relation was determined from the peak aequorin luminescence and peak twitch tension measured in muscles across a broad range of bathing [Ca2+] in the presence and absence of acetylcholine (ACh) (1 microM) or isoproterenol (ISN) (1 microM), or both drugs. ACh shifted the relationship of peak tension to (peak) aequorin light leftward, which suggests an increase in myofilament Ca2+ sensitivity, but it did not alter relaxation, which was measured as the time for peak tension to decay by 50% (t 1/2 R). ISN produced its previously documented effects, i.e., a rightward shift of the relationship of peak tension to peak aequorin light and a decrease in t1/2R. ACh abolished the ISN effect on the peak tension-aequorin light relationship but did not reverse the effect of ISN to decrease t1/2R. The effects of ACh and ISN of modulating the apparent myofilament Ca2+ sensitivity in intact muscles, corroborate findings of previous studies in isolated myofibrillar preparations. However, these perturbations of myofilament Ca2+ sensitivity in the intact muscle do not relate to twitch relaxation, measured as t1/2R, since (a) ACh affects the former but not the later and (b) the effect of ISN on the Ca2+-tension relationship is abolished by ACh, while the relaxant effect persists.     

Imaging calcium dynamics in living plants using semi-synthetic recombinant aequorins

The genetic transformation of the higher plant Nicotiana plumbaginifolia to express the protein apoaequorin has recently been used as a method to measure cytosolic free calcium ([Ca2+]i) changes within intact living plants (Knight, M. R., A. K. Campbell, S. M. Smith, and A. J. Trewavas. 1991. Nature (Lond.). 352:524-526; Knight, M. R., S. M. Smith, and A. J. Trewavas. 1992. Proc. Natl. Acad. Sci. USA. 89:4967-4971). After treatment with the luminophore coelenterazine the calcium-activated photoprotein aequorin is formed within the cytosol of the cells of the transformed plants. Aequorin emits blue light in a dose-dependent manner upon binding free calcium (Ca2+). Thus the quantification of light emission from coelenterazine-treated transgenic plant cells provides a direct measurement of [Ca2+]i. In this paper, by using a highly sensitive photon-counting camera connected to a light microscope, we have for the first time imaged changes in [Ca2+]i in response to cold-shock, touch and wounding in different tissues of transgenic Nicotiana plants. Using this approach we have been able to observe tissue-specific [Ca2+]i responses. We also demonstrate how this method can be tailored by the use of different coelenterazine analogues which endow the resultant aequorin (termed semi-synthetic recombinant aeqorin) with different properties. By using h-coelenterazine, which renders the recombinant aequorin reporter more sensitive to Ca2+, we have been able to image relatively small changes in [Ca2+]i in response to touch and wounding: changes not detectable when standard coelenterazine is used. Reconstitution of recombinant aequorin with another coelenterazine analogue (e-coelenterazine) produces a semi-synthetic recombinant aequorin with a bimodal spectrum of luminescence emission. The ratio of luminescence at two wavelengths (421 and 477 nm) provides a simpler method for quantification of [Ca2+]i in vivo than was previously available. This approach has the benefit that no information is needed on the amount of expression, reconstitution or consumption of aequorin which is normally required for calibration with aequorin.     

A simple model illustrating the role of turbulence on phytoplankton blooms

 The problem of the vertical distribution of phytoplankton is considered in the presence of gravitational settling, turbulent mixing, population growth due to cell division and a constant rate of loss due to predation and natural death. Nutrients are assumed to be plentiful so that the production rate depends only on the light available for photosynthesis. The non-linear saturation of plankton growth is modeled by allowing the attenuation rate of light to be a linear function of the plankton density. The turbulent diffusivity is assumed constant which corresponds to a mixed layer depth very much greater than the depth of light penetration (euphotic depth). It is shown that an exact analytical solution of this non-linear problem is possible for an idealized model in which the functional dependence of production on light intensity is assumed to be a step function. Non-zero solutions are shown to exist only if the parameters characterizing the system are above a certain critical curve in a two dimensional parameter space. Numerical simulations using functional forms of the production curve that resemble the measured photosynthetic response of plankton, show, that the qualitative behavior of the system is similar to that of the idealized model presented. Comparisons are made with other analytical approaches to the problem. Received: 14 March 2002 / Revised version: 27 September 2002 / Published online: 28 February 2003 Key words or phrases: Self-shading – Plankton – Nonlinear – Turbulence     

Sea ice predicts long‐term trends in Adélie penguin population growth,but not annual fluctuations: Results from a range‐wide multiscale analysis

Understanding the scales at which environmental variability affects populations is critical for projecting population dynamics and species distributions in rapidly changing environments. Here we used a multilevel Bayesian analysis of range‐wide survey data for Adélie penguins to characterize multidecadal and annual effects of sea ice on population growth. We found that mean sea ice concentration at breeding colonies (i.e., “prevailing” environmental conditions) had robust nonlinear effects on multidecadal population trends and explained over 85% of the variance in mean population growth rates among sites. In contrast, despite considerable year‐to‐year fluctuations in abundance at most breeding colonies, annual sea ice fluctuations often explained less than 10% of the temporal variance in population growth rates. Our study provides an understanding of the spatially and temporally dynamic environmental factors that define the range limits of Adélie penguins, further establishing this iconic marine predator as a true sea ice obligate and providing a firm basis for projection under scenarios of future climate change. Yet, given the weak effects of annual sea ice relative to the large unexplained variance in year‐to‐year growth rates, the ability to generate useful short‐term forecasts of Adélie penguin breeding abundance will be extremely limited. Our approach provides a powerful framework for linking short‐ and longer term population processes to environmental conditions that can be applied to any species, facilitating a richer understanding of ecological predictability and sensitivity to global change.