KINETICS OF PHYTOCHROME PELLETABILITY*

Abstract— The pelletability of P_r from maize coleoptiles was studied as a function of the delay time between a red and a far-red light pulse given in vivo. The obtained curve can be resolved into three parts. The two slowest reactions have half lives of 40 s and 3.6 min at 0°C. Furthermore, a break in the Arrhenius plot from the slowest reaction of the curve indicates that either the phytochrome “receptor” or the phytochrome molecule itself undergoes a jump in the Arrhenius activation energy at 20°C. These data are in good agreement with kinetic studies of phytochrome pelletability also discussed in this paper.     

IRRADIATION-ENHANCED PHYTOCHROME PELLETABILITY IN AVENA: PIGMENT RELEASE BY Mg2+-GRADIENT ELUTION

Abstract— Gradient elution is used to facilitate controlled withdrawal of Mg²⁺ from phytochrome-rich particulate fractions from irradiated Avena sativa L. shoots. The bound pigment from red-irradiated tissue is released in a discrete band when the Mg²⁺ falls to just below 1 mM. This phytochrome has an apparent molecular weight of ?300 kilodaltons upon gel filtration, indistinguishable from that of the unbound pigment in the same extract and from that in the 50,000 × g supernatant from non-irradiated Avena. This indicates that the bound phytochrome is released as a soluble molecule at a Mg²⁺ concentration above that which permits release of the particulate binding partner from other particulate components. These findings appear to preclude the possibility that the phytochrome-binding partner association can be selectively preserved at a Mg²⁺ level that would permit separation and analysis of phytochrome-bearing particles without the complication of Mg²⁺-induced membrane and RNP aggregation. “Cycled” P_fr (that from tissue irradiated with a red-far red sequence prior to homogenization) is released at 0.1 to 0.2 mM Mg²⁺. This indicates that “cycled P_r is more tenaciously bound by the particulate fraction than is P_fr. This effect is photoreversible both by further in vivo and subsequent in vitro irradiations, suggesting that the state of the pigment, rather than of the binding partner, directly controls the tenacity of the interaction. Increasing concentrations of KCl release the pigment from the particulate fraction in the presence of 10 mM Mg²⁺; increasing Triton X100 concentrations do not. This confirms the ionic nature of the pigment-particulate fraction interaction and indicates strongly that the phytochrome is located external to any membrane vesicles present (although not necessarily that it is bound directly to such vesicles). The data further suggest that phospholipid polar head groups are not primarily responsible for the binding.     

ANALYSIS OF Pfr DESTRUCTION IN AMARANTHUS CAUDATUS L EVIDENCE FOR TWO POOLS OF PHYTOCHROME*

Abstract— Kinetics of the destruction of the far red absorbing form of phytochrome (P_fr), measured by in vivo spectroscopy, show two phases: after a saturating red light pulse, rapid first order decay results in the loss of most, but not all, of the detectable P_rr; decay of the rest is much slower. The concentration of the more stable P_fr is positively correlated to the concentration of the total P_fr established at time zero. The linear relationship between total and ‘stable’ P_fr exludes the existence of a threshold level of P_fr for fast destruction. Photoconversion of the P_r (red absorbing form of phytochrome) present during the slow decay, by exposure to a second light pulse, is followed by fast destruction of most of the newly formed P,_r, whereas some P_fr formed by the first pulse still remains. The experiment suggests that not all P_fr molecules are accessible to the same destruction mechanism, i.e. there are two populations of P_fI.     

PHYTOCHROME CONTROL OF ITS OWN SYNTHESIS IN Sorghum vulgare AND Avena sativa

The accumulation of phytochrome in the dark was measured for Avena sativa seedlings after a white light pretreatment and for Sorghum vulgare seedlings after continuous red or far-red light treatments, using the herbicide Norflurazon to prevent greening under continuous irradiation. In both cases the accumulation of phytochrome depends on the state of the phytochrome at the light-dark transition: high P_fr levels (red light pulse) led to a slower rate of phytochrome accumulation than lower P_fr levels (long wavelength far-red (RG 9) light pulse). Poly-(A⁺)-RNA was isolated fromA. sativa seedlings grown for 48 h in darkness + 24 h WL + light pulse (5 min) (red, RG 9 light, red followed by RG 9 light or RG 9 followed by red light pulse) + 19 h darkness. The poly-(A⁺)-RNA was translated in a rabbit reticulocyte lysate system and the translation products were immunoprecipitated by specific anti-phytochrome antibodies. It was demonstrated that the activity of mRNA coding for phytochrome was under phytochrome control.     

INTERACTION BETWEEN PHYTOCHROME AND THE BLUE LIGHT PHOTORECEPTOR SYSTEM IN Mougeotia*

Abstract— Face-to-profile chloroplast movement in Mougeotia was induced by sequences of strong blue and red short irradiations. This type of response occured only when blue light was applied prior to or simultaneously with red light, and far-red irradiation was necessary after the sequence to cancel the remaining gradient of the far-red absorbing form of phytochrome P_fr. The dependence of the response magnitude on blue and red light sequences was studied for a wide range of light durations and dark intervals. The relationship between the response and the dark interval points to the lack of direct coupling between phytochrome and blue-absorbing “cryptochrome”. It was postulated that a photoproduct having a life-time of2–3 min is formed by the blue-light-mediated reaction. This photoproduct interacts with phytochrome during its transformation or with its final P_fr form.     

AN ATTEMPT TO LOCALIZE THE THRESHOLD REACTION IN PHYTOCHROME-MEDIATED CONTROL OF LIPOXYGENASE SYNTHESIS IN THE MUSTARD SEEDLING

Abstract —Synthesis* of the enzyme lipoxygenase (LOG)? in the cotyledons of the mustard seedling (Sinapis alba L.) is controlled by phytochrome (P_fr) through a threshold (all-or-none) mechanism. The data of the present paper confirm the previous assumption (Oelze-Karow and Mohr, 1973) that the primary reaction of P_fr (P_fr+ X → P_frX ? P_frX‘) is the site of the highly cooperative threshold reaction. Suppression of LOG synthesis depends on the presence of P_frX’. However, P_frX‘ is only stable above the threshold level of P_fr. If the level of P_fr is below the threshold, P_frX is stable, and no suppression of LOG synthesis occurs. As long as the level of P_fr remains below the threshold, no destruction of P_fr takes place. Destruction of P_fr occurs only as long as [P_fr]?is above the threshold level. Thus the simplest formulation of the actual threshold reaction in the LOG response is P_frX?_frX’ state at [P_fr] below threshold no P_fr destruction LOG synthesis suppressed state at [P_fr] above threshold P_fr destruction(¹k_d LOG synthesis unimpaired The reversible threshold reaction is thus an integral part of the “primary reaction” of P_fr occurring at the “matrix” specific for the LOG response. The data and conclusions on the LOG response are consistent with an “open phytochrome-receptor model” recently advanced by E. Schäfer (1975). The data are not consistent with the concept that a rapid dark reversion (P_fr→P_r) exists in dicotyledonous seedlings and that the degree of P_fr dark reversion strongly depends on the initial photostationary state, φ?, established by a saturating light pulse.     

KINETICS OF Pfr APPEARANCE IN Amaranthus caudatus‡

Abstract— The kinetics of the far-red absorbing form of phytochrome (P_fr) appearance from intermediates in the pathway from the red absorbing form of phytochrome (P_r) to P_fr that accumulate under high fluence rate white light have been investigated in 3-day old dark grown Amaranthus caudatus seedlings. The appearance of P_(r after a 5 s white light pulse was measured over the temperature range -8 to 25^°C in samples flushed with O₂ or N₂. Over the whole temperature range under anaerobic conditions the kinetics of the slowest component of P_fr appearance are faster than in the presence of O₂. Arrhenius plots are linear over this temperature range and indicate the activation energy for the slowest component of P_fr appearance is 44.05 ± 1.97 kJ mol^?1 for O₂ and 53.69 ± 4.86 kJ mol^?1 for N₂.     

ACTION SPECTRA OF PHYTOCHROME IN VIVO*

Abstract— A method is described to determine spectral properties of phytochrome in vivo. For photochrome in 7-day-old dark-grown Cucurbita pepo L. seedlings the mole fraction of the far-red-absorbing form (P_fr) present at photoequilibrium at 664 nm was found to be 0.76 ± 0.02 in vivo. Based on reflectance measurements, the photon fluence rate just below the surface of the cotyledons was calculated. Local rates of photoconversion for known local fluence rates were measured across cotyledons after non-saturating irradiations with wavelengths between 544 and 781 nm and in situ molar photoconversion coefficients were obtained. In contrast to purified oat phytochrome, the in situ molar photoconversion coefficients for P_fr show a strong shoulder between 660 and 700 nm. The maximum of P_fr absorption is at 726 nm. An isosbestic point of phytochrome is found at 686 nm. The mole fraction of P_fr present at photoequilibrium with 686 nm light is 0.58. The ratio of photoconversion quantum yields (that for P_r→ P_fr divided by that for P_fr→ P_r) is 1.38 ± 0.06.     

PHOTOCONTROL OF PHYTOCHROME DESTRUCTION IN GRASS SEEDLINGS. THE INFLUENCE OF WAVELENGTH AND IRRADIANCE

Abstract— –The kinetics of phytochrome destruction in vivo of coleoptiles and mesocotyls of etiolated grass seedlings (Avena sativa L., Zea mays L.) in continuous light were investigated using wavelength and irradiance as experimental variables. In contrast to dicotyledonous seedlings, the destruction reaction of these monocotyledons is saturated at very low levels of the far-red absorbing form of phytochrome, P_fr (e.g. at 1% of total phytochrome, corresponding to the photostationary state established by 727 nm light, in 2.5-day-old dark-grown Avena). On the other hand, the first-order rate constant of monocotyledon destruction may be at least one order of magnitude larger than in dicots, as indicated by the zero-order rate measured in the presence of saturating amounts of P_fr (τ_l/2 1.5 min in Avena). At sub-saturation P_fr levels, the destruction rate was found to be determined by the rate constants of the photoreactions over a wide range of wavelengths and irradiances. These results can be interpreted in terms of a destruction enzyme with high catalytic efficiency but limited availability. Analysis of in vivo binding of phytochrome to a pelletable cell structure during destruction revealed that both the pelletable and the non-pelletable fraction lose photoreversiblility with similar rates and thus provide no useful information with respect to a causal relationship between the two processes. However, due to the short half-life of P_fr at sub-saturation levels (which make the photoreactions and intermediary processes rate-limiting for destruction even at relatively high irradiances) the existence of a similarly rapid dark-reaction between the photoreactions producing P_fr and the destruction reaction could be demonstrated. This dark reaction displays the properties of P_fr binding to a receptor site.     

SPECTRAL PROPERTIES,PHOTOTRANSFORMATION KINETICS AND PELLETABILITY OF PHYTOCHROME IN Pharbitis nil Chois*

Abstract— An examination has been made of the involvement of phytochrome in the circadian rhythm of flowering in Pharbitis nil Chois. The peak position of P_fr absorption changes with time after a red light pulse. The shortest absorption wavelength of P_fr occurs at the same time as flowering is inhibited by red light in dark grown, red light pretreated plants. Pelletable and supernatant phytochrome show a similar trend with lowest values found at the time of flower inhibition. Neither phototransformation kinetics nor intermediates of phytochrome which accumulate in white light show such a relationship to the circadian rhythm found in flowering of dark grown P. nil.     

PHYTOCHROME ACTION: A REAPPRAISAL

Stems of fully green plants show at least two types of response to light. In one, P_fr inhibits elongation. The second is a promotion of elongation which operates only in light; the effectiveness of red and far-red wavelengths indicates that this response is also mediated through phytochrome. Studies of the de-etiolation process also provide evidence for two modes of action of phytochrome; one is a P_fr-dependent reaction, and the second requires continuous light (or frequent short irradiations). It is proposed that, in addition to reactions which require P_fr and proceed in darkness, an important reaction of phytochrome in green plants occurs only in light. We have termed these two modes of action of phytochrome “static” and “dynamic”. The static mode operates after a brief exposure to light which establishes P_fr; the potential responses are largely reversible by far-red and exhibit reciprocity. The dynamic mode operates only in light and the responses do not show reciprocity. We consider that this mode operates through the transition from one bound form of phytochrome to another. The possible involvement of these two modes of action of phytochrome in photoperiodic mechanisms is discussed.     

INTERMEDIATES IN THE PHOTOCONVERSION OF FUNCTIONAL PHYTOCHROME IN FERN SPORES OF Dryopteris–II. In vivo KINETICS OF THE DECAY OF Ii700 AND OF THE FORMATION OF Pfr STUDIED WITH A DOUBLE-LASER APPARATUS*

Abstract— Photoconversion of the red-light-absorbing form of phytochrome, P_r, to the far-red-light-absorbing form, P_fr, was investigated in vivo at 22°C with 600 or 800 ns laser pulses of high spectral purity and induction of spore germination in Dryopteris paleacea was used as indicator for the progress of photoconversion. This reaction is initiated by a saturating R-laser pulse of 648.5 nm, establishing an equilibrium of the photochromic system between P_r and the very early intermediates, Iⁱ₇₀₀ (P_rφ Iⁱ₇₀₀)- The decay of Iⁱ₇₀₀ as well as the formation of P_fr was recorded by the application of a second pulse varied between 698 and 717.5 nm, which inhibits the formation of P_lr being absorbed predominantly by Iⁱ₇₀₀or P_fr, respectively. The most effective inhibition for the second pulse is found up to 10 u.s after the first pulse and this is interpreted by photoreversion of Iⁱ₇₀₀ to P_r; thus reducing the formation of P_fr from Iⁱ₇₀₀. This early inhibition decreases between 10 μs to 100 ms after the R-laser pulse, as a result of the decay of Iⁱ_bl to a bleached species I,;. This decay can be described by three first order kinetics with the rate constants k₁₂= 16830 ± 2970 s^-1, k₁₂= 666 ± 218 s^-1,k₁₃= 9.8 ± 0.9 s^-1. A second inhibition, due to the formation of P_fr, is found for dark intervals <100 ms and can be described by two first order kinetics with the rate constants k₂₁= 2.9 ± 0.6 s^-1 and k₂₂= 0.17 s^-l.     

FLUORESCENCE OF PHYTOCHROME IN THE CELLS OF DARK-GROWN PLANTS AND ITS CONNECTION WITH THE PHOTOTRANSFORMATIONS OF THE PIGMENT

Abstract Fluorescence of phytochrome is found in the cells of etiolated monocotyledonous and dicotyledonous plants. The red light-absorbing form of phytochrome (P_r) fluoresces at 77 K with a yield 0.3±0.1 and maxima at 672–673 nm and 684–686 nm in the excitation and emission spectra, respectively. The emission is characterized by the sharp temperature dependence of its intensity, its high (～ 40%) polarization, and the violation of the mirror symmetry rule. Connection of the fluorescence with P_r photoreactions is followed in the interval 77–293 K. A P, photoproduct, lumi-R, is fluorescent with maxima at 696 nm and 705 nm in the excitation and emission spectra; the far-red light absorbing form of phytochrome (P_fr) is practically nonfluorescent. Three isochromic emitting P_r species are present differing in their photochemical properties: P_r1 and P_r2 which phototransform irreversibly and reversibly at T 170 K into lumi-R, and lumi-R₂, respectively, and P_r3 which undergoes photoconversion only at T > 240 K. The activation energies of P_r2 and P_r3 photoreactions are evaluated to be 2.9–3.3 kJ/mol and 26 kJ/mol. Complex dynamics of changes of P_r fluorescence and of the extent of its decrease in the photoconversion P_r? P_fr in germinating pea and bean seeds suggests the existence of two P_r pools one of which is incapable of P_r? P_fr phototransformation. Thus, the developed fluorescent method of phytochrome assay and investigation in the cell revealing multiplicity of phytochrome states in vivo proves to be very sensitive (about 1 ng) and informative.     

PHYTOCHROME IN ETIOPLASTS IN RELATION TO CHLOROPHYLL ACCUMULATION*

Abstract— De-etiolation of maize seedlings reduces their sensitivity for red light potentiation of rapid chlorophyll accumulation in white light. An earlier proposal (Raven and Spruit, 1973) attributes this to migration of the far-red absorbing form of phytochrome (P_fr) to receptors essential for chlorophyll synthesis, thereby increasing the local P_fr/total phytochrome (P_tot)ratio. We have studied etioplasts as possible loci for such P_(r receptors. The level of spectrophotometric phytochrome in purified etioplasts isolated from red preirradiated maize seedlings was higher than that of dark grown plants. The difference was marginally significant, however. We argue that migration of a fraction of cytoplasmic P_fr to the etioplasts, too small to be spectrophotometically demonstrable, could still meet the requirements of the model. Dark destruction of bulk spectrophotometric P_fr following saturating red irradiation of seedlings is not paralleled by a decrease of etioplast phytochrome. the latter remaining essentially constant over long periods. On the other hand, the potentiating effect of red light in intact seedlings is still partially reversible by far red light even after 24 h of darkness when destruction of bulk P_fr is complete. Since this demonstrates persistent presence of P_fr active in potentiation, we propose that at least part of this P_fr is associated with the etioplasts.     

INTERMEDIATES IN THE PHOTOCONVERSION OF FUNCTIONAL PHYTOCHROME IN FERN SPORES OF Dryopteris-I DEMONSTRATION AND QUANTITATIVE CHARACTERIZATION OF THE PHOTOCHROMIC SYSTEM Pr⇔ Ii700USING NANOSECOND-LASER PULSES*,†

Abstract— Spores of Dryopteris paleacea and D. filix-mas are positively photoblastic with an optimum in the action spectrum around 665 nm. Light is perceived by phytochrome and the relationship between germination and mole fraction of the far-red-absorbing form of this pigment, P_fr, was investigated with saturating irradiations between 662 and 747 nm under low-fluence-rate conditions. These control irradiations establish a proportion of the total phytochrome, P,_tot, as P_fr with P_fr/P_tot–φ at equilibrium. These φ -values were calculated according to data for native oat phytochrome (Kelly and Lagarias, 1985, Biochemistry 24, 6003) and the spectral characteristics of the interference filters. With this method a linear relationship could be found between φ and germination from 2 to 70% for D. paleacea and from 2 to 90% for D. filix-mas, if probit germination was plotted vs probit φ This correlation formed the basis of investigating the phytochrome photoconversion by dye-laser pulses of 380 ± 30 ns under high-fluence-rate conditions, and thus to test quantitatively the impact of the photoreversibility of intermediate reactions of the photoconversion and the red-absorbing form of phytochrome, P_fr on the final P_fr-level. Spore germination was initiated by a single-laser pulse in the range from 592 to 700 nm. The most effective wavelengths were 649 and 660 nm in both species, and at saturation maximal germination (ca. 50%) was obtained from 592 to 665 nm for D. paleacea or ca. 60% germination from 592 to 670 nm for D. filix-mas. Both saturation levels correspond to a ø-value between 0.40 and 0.45. This significantly diminished photoconversion is a consequence of the high-fluence-rate conditions during the laser pulse which establishes the photochromic system between P_r and a set of very early intermediates, Iⁱ_700, (= P_r? Iⁱ₇₀₀). This system can be described by the extinction coefficients of P_r and the intermediates Iⁱ₇₀₀, and by the quantum yields, 4,φ for the forward and reverse reactions as φ If φ is calculated, assuming a quantum yield of 1:1 for both reactions and with the extinction coefficients of P_r and Iⁱ_7(l() (= lumi-R) given by Eilfeld and Riidiger (1985, Z. Naturforsch. 40c , 109), significantly higher values are calculated for / as compared to φ found in the control experiments. These results can be explained either: (i) with a quantum yield ratio φ_pr-φ1700: φ_1700φpr=1:1 and an assumed additional dark reaction leading from Iⁱ₇₀₀ or later intermediates back to P_r: or (ii) with a quantum yield ratio φ_{pr φ 1700}: φ_{1700 φpr}=1:2. In this case all Iⁱ₇₀₀ have to relax to P_fr. In this case all Iⁱ₇₀₀ have to relax to P_fr.     

PHYTOCHROME-CONTROLLED FERN-SPORE GERMINATION: PHASE-SPECIFIC MODULATION BY ELEVATED TEMPERATURES*

The phytochrome-mediated spore germination in Dryopteris is inhibited by raising the temperature from 22 to 27 or 32°C. As reported earlier (W. Haupt (1990) Photochem. Photobiol. 52,57–59), the elevated temperature is effective during the “coupling phase”, i.e. when P_fr, the active form of phytochrome, starts the processes leading to germination. In addition, a strong effect has now been found in the “preinduction phase”, i.e. when the spore develops its competence to react to P_fr. This latter effect is overcome, if in the subsequent coupling phase a high level of P_fr is allowed to act for a long time. Moreover, the inhibiting effect in a2–3 day preinduction phase is most obvious in or even restricted to its terminal 24 h. It is proposed that the temperature acts by reversibly abolishing the cell's competence to react to P_fr, and that this effect can extend into the coupling phase. Not yet understood is an “inversion” effect in D. paleacea: if the temperature is raised in the earlier parts of the preinduction phase, the effect of P_fr in the subsequent coupling phase is enhanced rather than inhibited.     

THE EFFECT OF DEUTERIUM OXIDE ON THE FLUORESCENCE AND PHOTOTRANSFORMATION OF 124 kDALTON PHYTOCHROME*

Abstract— To probe the nature of primary photoprocess and the mechanism of the phototransformation of undegraded 124 kDa oat phytochrome, solvent deuterium isotope effects on the fluorescence and phototransformation of phytochrome have been investigated. The fluorescence intensity and lifetime of phytochrome (P_r form) are greater in D₂0-buffer than in H₂O-buffer, suggesting a possible involvement of proton transfer in the primary photoprocess of phytochrome. Although the photostationary equilibrium (P_r to P_fr ratio) was not altered by deuterium oxide, in contrast to degraded phytochrome, the rate constants of both transformations, P_r→ P_fr and P_fr→ P_r were enhanced by up to 24%. The P_r to P_fr phototransformation of degraded phytochrome, however, was retarded by about the same percentage in D₂O. These opposite effects of D₂O with degraded and undegraded phytochromes underscore the fact that the P_r form from the former reverts to the P_r form in the dark, apparently catalyzed by deuterated general and/or conjugate acidic group(s). With the degraded phytochrome the deuterium oxide enhancement of the rate of dark reversion was approximately 2-fold (Sarkar and Song, 1981). Both the fluorescence intensity and the rates of phototransformation of phytochrome were enhanced in D₂O with successive photocyclings (P_r→ P_fr→ P_r→ P_fr→ P_r etc.) with alternating red and far-red irradiation. It has been proposed that successive photocycling of phytochrome in D₂O results in proton-deuteron exchange in the partially exposed P_tr chromophore and/or its surrounding amino acid residues.     

Comparison of the protein conformations between different forms (Pr and Pfr) of native (124 kDa) and degraded (118/114 kDa) phytochromes from Avena sativa

Abstract— Circular dichroic properties of native, 124 kDa phytochrome from etiolated Avena sativa seedlings have been examined and compared with those of degraded phytochrome (118/114 kDa). The CD spectrum of the P_r form of 124 kDa phytochrome does not differ significantly in the visible region from that of 118/114 kDa P_r. In contrast, the CD spectrum of the P_fr form of 124 kDa phytochrome differs from that of the 118/114 kDa species in the far-red, red and blue regions of the spectrum. This result confirms that the NH₂-terminal polypeptide segment has a critical role in chromophore-protein interaction in the P_fr but not in the P_r form. In the UV region, 124 kDa phytochrome exhibits a photoreversible difference between the CD spectra of P_r and P_fr, whereas no such difference is observed for 118/114 kDa preparations. These data suggest a possible photoreversible change in secondary structure of the 124 kDa phytochrome polypeptide that requires the presence of the 6/10 kDa NH₂-terminal domain to occur.     

THE MODE OF INTERACTION BETWEEN BLUE (UV) LIGHT PHOTORECEPTOR AND PHYTOCHROME IN ANTHOCYANIN FORMATION OF THE SORGHUM SEEDLING

Two non-photosynthetic photoreceptors (phytochrome and a blue light photoreceptor) are involved in light-mediated anthocyanin synthesis in the mesocotyl of Sorghum seedlings. The present study was undertaken to investigate the kind of interaction between phytochrome and the blue light photoreceptor. The data show that phytochrome (P_fr) can only act once a blue light effect has occurred. On the other hand, the blue light effect cannot express itself without P_fr. It is concluded that there is an obligatory dependency (or sequential interaction) between the blue light effect and the light effect occurring through phytochrome, although the blue light photoreaction per se is not affected by the presence or absence of phytochrome. The latter statement is based on the results of dichromatic experiments, i.e. simultaneous, high fluence rate irradiation with two kinds of light. Blue light can be replaced by UV light. It is not clarified yet whether the effect of blue and UV light is due to the same photoreceptor.