Reciprocity in the activation of geotropism in oat coleoptiles grown on clinostats

Summary The activation of geotropism in oat coleoptiles, grown on horizonta clinostats, i.e., without the tropic influence of gravity, shows a reciprocal relationship between force and time. Two methods were used to approximate geotropic presentation time. In one, this parameter was estimated by extrapolation to zero response from the linear relationship, response = a+b log stimulation time. In the other, stimulation times of very short as well as longer durations were used; under these conditions, the response curve shows two distinct rates, with the lower rate for stimuli of brief duration. The intersection of the two rate-segments of the response curve was taken as the presentation time. Both methods show reciprocity for the activation of geotropism, but yield significantly different reciprocity constants. The ability of the coleoptile to sense gravity is not affected by gravity compensation. With agar as a growth medium, the magnitude of response to gravity is greater than with sand. However, coleoptiles grown in sand are more sensitive to geotropic activation.Work supported by the U. S. Atomic Energy Commission and the National Aeronautics and Space Administration.     

Wirkung von Vorbestrahlung mit Rot- oder Blaulicht auf die geotropische Empfindlichkeit von Maiskoleoptilen

The early geotropic downward bending of corn (Zea mays L.) coleoptiles was found to be influenced by red and blue light. The coleoptiles were illuminated from above and kept in the dark for defined intervals; afterwards they were positioned horizontally and their curvature was monitored for 40 min. After illumination with red light and a 120 min interval and early upward bending instead of an early downward bending was found. This effect was nullified by a far-red illumination administered immediately after exposure to red light. These results indicate that the phytochrome system influences the geotropic reaction. After illumination with blue light and a 30 min interval little downward bending was found. This result corresponds well with the findings of earlier authors who measured the late geotropic reaction, on the basis of the hypothesis that the strength of the early downward bending is a measure of the geotropic sensitivity. The dose-effect curve of the blue light influence on geotropic sensitivity, measured by early downward bending, is very similar to the dose-effect curve of the phototropic curvature of corn coleoptiles. This fact together with the earlier finding of similar adaptation times of about 30 min suggests the existence of some common transducers in the reaction chain of phototropism and geotropism.

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Abkürzungen HR Hellrot - DR Dunkelrot - D Dunkel - WT Wartezeit - DK Dunkelkontrolle     

Geotropism and the lateral transport of auxin in the corn mutant amylomaize

Summary In coleoptiles of the amylomaize corn mutant (AM), the amyloplasts are much reduced in size in comparison with the wild type corn (WT), permitting a comparison of geotropic responsiveness as related to lateral displacement of amyloplasts and lateral transport of auxin. The amyloplasts of AM showed 30–40% lesser lateral redistribution in response to horizontal exposure in comparison with WT. With geotropic stimulation, the lateral transport of auxin in the direction of growth was 40–80% less, and the geotropic curvature by the coleoptiles was also significantly less in the mutant as compared with WT. These correlations support the hypothesis that the starch plastids serve as gravity sensors in the geotropic responses of coleoptiles.     

The Effects of Red, Far-red, and Blue Light on the Geotropic Response of Coleoptiles of Zea mays

The effects of red, far-red, and blue light on the geotropicresponse of excised coleoptiles of Zea mays have been investigated.Seedlings were grown in darkness for 5 or 6 days, exposed tovarious light treatments, and then returned to darkness fordetermination of the geotropic response. The rate of response of the coleoptiles is decreased after theyhave been exposed to red light (620–700 mµ, 560ergs cm^–2sec^–1 for the 24 hrs, but not for the 4hrs, preceding stimulation by gravity. Furthermore, their rateof response is greatly reduced if they are exposed to red lightfor 10 min and then returned to darkness for 20 hrs before geotropicstimulation. At 25° C an interval of 6 to 8 hrs elapses between a 10-minexposure to red light and the first detectable decrease in thegeotropic response of the coleoptile. This interval can be lengthenedby exposing the seedlings to low temperatures (0° to 2°C) after the light treatment but cannot be greatly shortenedby increasing the duration of exposure to red light. Using a standard procedure of exposing 5-day-old etiolated seedlingsto light for various times, replacing them in darkness for 20hrs and then determining the response of the coleoptiles to4 hrs geotropic stimulation, it has been found that: (a) Exposureto red light for 15 sec significantly decreases the geotropiccurvature of the coleoptiles and that further reduction occurson increasing the length of the light treatment to 2 and 5 min.(b) Far-red light has no effect on the geotropic response ofthe coleoptiles but it can completely reverse the effect ofred light. After repeated alternate exposure to red and far-redlight the geotropic response of the coleoptile is determinedby the nature of the last exposure, (c) Complete reversal ofthe effect of red light by far-red radiation only occurs whenexposure to far-red follows immediately after exposure to red.The reversing effect of far-red radiation is reduced if a periodof darkness intervenes between the red and far-red light treatments,and is lost after a dark interval of approximately 2 hrs. The effect of red light on the rate of geotropic response ofthe coleoptiles is independent of their age and length at thetime of excision. Blue light acts in a similar way to red light, but the seedlingsare less sensitive to blue than to red light. Coleoptiles grown throughout in a mixture of continuous, weak,red, and far-red light have a lower rate of geotropic responsethan etiolated coleoptiles.     

The lateral transport of IAA in intact coleoptiles of Avena sativa L. and Zea mays L. during geotropic stimulation

Summary Movement of IAA was studied in excised coleoptile apices and whole seedlings of Zea mays L. and Avena sativa L. during geotropic stimulation. A micropipette technique permitted the application of [5-³H]IAA at predetermined points on the coleoptiles with minimal tissue damage.When [5-³H]IAA was applied to the upper side of a horizontal excised Zea coleoptile, about 60% of the recoverable radioactivity had moved into the lower half after 2 h. In contrast, when application was made to the lower side of a horizontal excised coleoptile, only 4% of the radioactivity migrated to the upper half. There was, thus, a net downward movement of 56%. Similar patterns of distribution were found for radioactivity in both the tissue and the basal receiver blocks. In horizontal shoot tissues of intact Zea seedlings a net downward movement of about 30% of the recoverable radioactivity occurred after 1 h of geotropic stimulation. Comparable experiments with Avena indicated a net downward movement of 6–12% in excised apices of coleoptiles and in the intact shoot. In both Zea and Avena chromatographic analyses of tissue and receiver blocks indicated that the movement of radioactivity reflected that of IAA.In Zea coleoptiles, the lateral migration of radioactivity after 2 h was 3 to 4 times greater in the apical tissues than in the basal tissues. A significant net downward movement of radioactivity was detected after 10 min of geotropic stimulation in the extreme apex of Zea coleoptiles but not in the more basal regions.These experiments show that downward lateral transport of IAA occurs in intact shoots of Zea and Avena seedlings upon geotropic stimulation. Lateral transport of IAA had previously been demonstrated only in sub-apical segments of Zea coleoptiles.     

The dose-response curve of the gravitropic reaction: a re-analysis

The dose-response curve of the gravitropic reaction is often used to evaluate the gravisensing of plant organs. It has been proposed (Larsen 1957) that the response (curvature) varies linearly as a function of the logarithm of the dose of gravistimulus. As this model fitted correctly most of the data obtained in the literature, the presentation time (tp, minimal duration of stimulation in the gravitational field to induce a response) or the presentation dose (dp, minimal quantity in g.s of stimulation to induce a response) were estimated by extrapolating down to zero curvature the straight line representing the response as a function of the logarithm of the stimulus. This method was preferred to a direct measurement of dp or tp with minute stimulations, since very slight gravitropic response cannot be distinguished from the background oscillations of the extremity of the organs. In the present review, it is shown that generally the logarithmic model (L) does not fit the experimental data published in the literature as well as the hyperbolic model (H). The H model in its simplest form is related to a response in which a ligand-receptor system is the limiting phase in the cascade of events leading to the response (Weyers et al. 1987). However, it is demonstrated that the differential growth, responsible for the curvature (and the angle of curvature), would vary as a hyperbolic function of the dose of stimulation, even if several steps involving ligand-receptor systems are responsible for the gravitropic curvature. In the H model, there is theoretically no presentation time (or presentation dose) since the curve passes through the origin. The value of the derivative of the H function equals a/b and represents the slope of the cune at the origin. It could be therefore used to estimate gravisensitivity. This provides a measurement of graviresponsiveness for threshold doses of stimulation. These results imply that the presentation time (or presentation dose) derived from the L model cannot be used anymore as an estimate of gravisensitivity. On the contrary, the perception time (minimal duration of a repeated stimulation which induces a response), which is less than 1 s, should be related to the perception of gravity. The consequences of these results on the mode of action and the nature of graviperception are discussed.     

Entrainment of Geotropic Oscillations in Hypocotyls of Heliunthus annuus– An Experimental and Theoretical Investigation

A theory for the geotropic movements of the Heliunthus unnuus hypocotyl has been given earlier by Johnsson et ul. In the present paper this theory is tested by extensive experiments. The magnitude as well as the rate of geotropic curvature are found to be in agreement with the theoretical predictions. Further, the geotropic reaction time, defined as the time between the start of geotropic stimulation and the start of the geotropic reaction is determined as a function of the stimulation angle with respect to the plumb line. A slight variation found in the reaction time is included in the theory.     

Geotropic curvature of decapitated Avena coleoptiles after application of tips of maize roots,tips of Avena coleoptiles,indoleacetic acid,or abscisic acid

Isolated Avena coleoptiles were decapitated at different distances from the tip and then placed horizontally, after which the geotropic curvature was measured. No geotropic curvature could be detected during the first 3 h. Later, upward curvature occurred which was found to depend inversely on the length of the decapitated tips. When the tips of maize roots or Avena coleoptiles were placed on the cut surface of decapitated Avena coleoptiles, the coleoptiles showed a significantly stronger upward curvature as compared to controls which had been provided with agar blocks on the cut surface. The same upward curvature was found with decapitated coleoptiles provided with agar blocks containing 10^-6 or 10^-7 M indoleacetic acid (IAA). After application of abscisic acid (ABA) at concentrations of 10^-6 and 10^-8 M to the decapitated coleoptiles, the curvature observed was not different from that of the controls; at higher concentrations of ABA the curvature was found to be lower than that of the controls. It is concluded that root tips secrete a substance which may replace the effect of IAA in coleoptiles. The results are discussed in view of the validity of the Cholodny-Went hypothesis for the geotropic reaction of roots.Abbreviations ABA abscisic acid - IAA 3-indoleacetic acid     

Movement of Cell Organelles and the Geotropic Curvature in Roots of Norway Spruce (Picea abies)

The geotropic development in roots of Norway spruce [(Picea abies (L.)] H. Karst, has been followed by light and electron microscopy and compared with the movement of cell organelles (statoliths) in the root cap cells. The geotropic curvature develops in two phases: (a) an initial curvature in the root cap region, which results in an asymmetry in the extreme root tip and which appears after about 3 h stimulation in the horizontal position; and (b) the geotropic curvature in the basal parts of the root tip, which after 8 h is distributed over the entire elongation zone. A graphic extrapolation, based on measurements of the root curvatures after various stimulation periods, indicates a presentation time in the range of 8 to 10 min. The root anatomy and ultrastructure have been examined in detail in order to obtain information as to which organelles may act as gravity receptors. The root cap consists of a central core (columella) distinct from the peripheral part. The core contains three to four rows of parenchymatic cells each consisting of 15 to 18 storeys of statocyte cells with possibly mobile cell organelles. Amyloplasts and nuclei have been found to be mobile in the root cap cells, and the movement of both types of organelles has been followed after inversion of the seedlings and stimulation in the horizontal position for various periods of time at 4°C and 21°C. Three-dimensional reconstructions of spruce root cap cells based on serial sectioning and electron microscopy have been performed. These demonstrate that the endoplasmic reticulum (ER)-system and the vacuoles occupy a considerable part of the statocyte cell. For this reason the space available for free movement of single statolith particles is highly restricted.     

GEOTROPIC EXCITATION IN HELIX

Rotation of an inclined surface on which Helix is creeping straight upward, such that the axis of the animal is turned at a right angle to its previous position, but in the same plane, leads to negatively geotropic orientation after a measurable latent period or reaction time. The duration of the latent period is a function of the slope of the surface. The magnitude of the standard deviation of the mean latent period is directly proportional to the mean latent period itself, so that the relative variability of response is constant. The dependence of reaction time upon extent of displacement from symmetrical orientation in the gravitational field is found also by tilting the supporting surface, without rotation in the animal''s own plane. On slopes up to 55°, the relation between latent period and the sine of the slope is hyperbolic; above this inclination, the latent period sharply declines. This change in the curve is not affected by the attachment of moderate loads to the snail''s shell (up to 1/3 of its own mass), and is probably a consequence of loss of passive stable equilibrium when rotated. When added loads do not too greatly extend the snail''s anterior musculature, the latent period for the geotropic reaction is decreased, and, proportionately, its σ. These facts are discussed from the standpoint that geotropic excitation in these gasteropods is due to impressed muscle-tensions.     

Relationships between Photo-induced and Gravity-induced Electrical Potentials in Zea Mays

A comparison is made between gravity-induced and light-induced transversal electrical potentials in excised coleoptiles of Zea Mays. The potentials are measured with a vibrating condensor method, thus the plants are not touched at the measuring point. It is found that all experimental evidence supports the assumption that the reaction chains leading to the potentials are identical in the two cases, apart of course from the perception stages. This theory is based on the following points which have been experimentally verified:

• 1 The stimulus-response functions are quite similar. In both cases the voltage is a logarithmic function of the stimulation time (at least for shorter stimulation times). When continuous stimulation is used, the stimulation time must exceed a threshold value to cause a transversal potential.
• 2 Some inhibitors (DNP and NaN₃) diminish both types of potential.
• 3 A latency time is found in photo-induced potentials as well as in gravity-induced ones. The Q₁₀ for the latency period of the photo-induced potentials is found to be 2.8, which is the same as for the chemical part of the latency period of the gravity-induced potentials.
• 4 In both cases the potential-generating process is controlled by a Q₁₀ of 1.6–1.8, thus indicating this process as separate from the one mentioned above.
• 5 The temperature dependence of the maximum voltage follows in both cases the same pattern with a maximum at about 25–30°C.

Some measurements on potential oscillations are described and discussed. The origin of the potentials is discussed.     

A Theory for Circumnutations in Helianthus annuus

A theory is given for circumnutations in plants, especially hypocotyls of Helianthus annuus, which were used as experimental material The theory is based on the lateral auxin transport, which arises when a gravitational force component acts on the plant. With a suitable time delay between stimulus and response, oscillations or circumnutations should arise. It is possible to describe these oscillation phenomena by the solutions of a differential equation, derived in this paper. The time delay has a central role in this equation. The time delay is assumed to be identical with the geotropic reaction time for the hypocotyls. The ratio between the periodic time for the circumnutations and the reaction time for geotropic curvatures was found to be approximately constant in the temperature region investigated (namely 15–40°C), which supports the theory. Different methods of recording the circumnutations were used, 8 mm film camera technique being the most frequently employed. The introduction of a weighting function for describing the plants “memory” of the stimulation makes it possible to relate the periodic time of the circumnutations to the reaction time for geotropic curvatures. The necessity of this weighting function as well as of the time delay in the equations is emphasized. An explanation of the “Fünfphasen-bewegungen”, reported in the literature, is presented.     

The Threshold Stimulus for Geotropism

The minimum effective geotropic stimulation time is very short for coleoptiles, hypocotyls and roots. New data from the literature are used to emphasize that the minimum time is of the order of 10–20 s. The existence of such a short minimum time should be carefully considered in the design of geotropic experiments in Spacelab, which are now at the planning stage. Even brief acceleration periods at 1 g or less during a flight might cause unintentional geotropic effects. The short minimum stimulation time also has relevance for the statolith theory: since the distance which an amyloplast can sediment during this time is very small, no long sedimentation distance is likely to be required for georeception. Moreover, the magnitude of thermal noise must be considered in evaluating proposals for the georeceptive mechanism.     

Die Dosis-Wirkungsrelationen bei geotroper und phototroper Reizung: Vergleich von Mono- mit Dicotyledonen

Zusammenfassung der Ergebnisse Die geotropen Krümmungen von Avena-Coleoptilen und Lens-Epicotylen nehmen linear proportional der Reizdauer zu. Bei geringen Reizzeiten sind beide Objekte gleich hoch empfindlich; bei längerer Reizdauer krümmen sich die Avena-Coleoptilen etwas stärker. Lens-Epicotyle reagieren auf zunehmende phototrope Reizung mit einer ersten und einer zweiten positiven Krümmung. Zwischen beiden Krümmungsbereichen (etwa von 10 000–1 000 000 lx · sec) sind sie phototropisch unempfindlich. Negative Krümmungen treten, nie auf. Ebenso verhalten sich 12 weitere dicotyle (Brassica napus, Brassica oleracea subsp. capitata, Brassica oleracea subsp. bullata, Lepidium sativum, Vicia villosa, Sinapis alba, Cucumis sativus, Linum usitatissimum, Helianthus annuus, Agrostemma githago, Raphanus sativus, Convolvulus tricolor) und 3 weitere monocotyle (Hordeum distichon, Secale cereale, Triticum aestivum) Pflanzenarten.Die phototrope Empfindlichkeit ist für Avena-Coleoptilen und Lens-Epicotyle im Bereich der ersten positiven Reaktion gleich groß, im Bereich der zweiten positiven Krümmung sind Avena-Coleoptilen empfindlicher. Das Reizmengengesetz ist für Lens-Epicotyle (wie für Avena-Coleoptilen) in der ersten positiven Krümmung gültig, in der zweiten positiven nicht.

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The dose response relations in geotropic and phototropic stimulation: Comparison of mono-with dicotyledonous plants

Summary The increase in the geotropic curvatures of Avena coleoptiles and Lens epicotyls is linear and proportional to the time of stimulation. With low stimulation the sensitivities of both objects are equal; with longer stimulation the curvature of Avena coleoptiles is somewhat greater.To increased phototropic irradiance Lens epicotyls react with a first and a second positive curvature. Between the two ranges of curvature (from about 10,000 up to 1,000,000 lx · sec) they are phototropically insensitive; negative curvatures never occur. The same reaction is shown by 12 other dicotyledonous plants (Brassica napus, Brassica oleracea subsp. capitata, Brassica oleracea subsp. bullata, Lepidium sativum, Vicia villosa, Sinapis alba, Cucumis sativus, Linum usitatissimum, Helianthus annuus, Agrostemma githago, Raphanus sativus, Convolvulus tricolor) and by 3 other monocotyledonous plants (Hordeum distichon, Secale cereale, Triticum aestivum). In the first positive reaction the phototropic sensitivities of Avena coleoptiles and Lens epicotyls are equal, in the second positive reaction Avena coleoptiles are more sensitive. For Lens epicotyls (for Avena coleoptiles, too) the reciprocity law is valid in the first positive reaction, but not in the second positive reaction.

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Aus einer Dissertation der Mathematisch-Naturwissenschaftlichen Fakultät der Universität Rostock (Steyer, 1964).     

Cell elongation in the grass pulvinus in response to geotropic stimulation and auxin application

Summary Horizontally-placed segments of Avena sativa L. shoots show a negative geotropic response after a period of 30 min. This response is based on cell elongation on the lower side of the leaf-sheath base (pulvinus). Triticum aestivum L., Hordeum vulgare L. and Secale cereale L. also show geotropic responses that are similar to those in Avena shoots. The pulvinus is a highly specialized organ with radial symmetry and is made up of epidermal, vascular, parenchymatous and collenchymatous tissues. Statoliths, which are confined to parenchyma cells around the vascular bundles, sediment towards the gravitational field within 10–15 min of geotropic stimulation. Collenchymatous cells occur as prominent bundle caps, and in Avena, they occupy about 30% of the volume of the pulvinus. Geotropic stimulation causes a 3- to 5-fold increase in the length of the cells on the side nearest to the center of the gravitational field. Growth can also be initiated in vertically-held pulvini by the application of indole-3-acetic acid, 1-naphthaleneacetic acid or 2.4-dichlorophenoxyacetic acid. 2.3.5.-triiodobenzoic acid interferes with growth response produced by geotropic stimulation as well as with the response caused by auxin application. Gibberellic acid and kinetin have no visible effect on the growth of the pulvinus. Polarization microscopy shows a unique, non-uniform stretching of the elongating collenchymatous cells. Nonelongated collenchymatous cells appear uniformally anisotropic. After geotropic stimulation or auxin application, they appear alternately anisotropic and almost isotropic. Such a pattern of cell elongation is also observed in collenchyma cells of geotropically-stimulated shoots of Rumex acetosa L., a dicotyledon.Abbreviations 2.4-D 2.4-dichlorophenoxyacetic acid - GA₃ gibberellic acid - IAA indole-3-acetic acid - NAA l-naphthaleneacetic acid - TIBA 2.3.5-triiodobenzoic acid     

Gravitropic responses of the Avena coleoptile in space and on clinostats. I. Gravitropic response thresholds

We conducted a series of gravitropic experiments on Avena coleoptiles in the weightlessness environment of Spacelab. The purpose was to test the threshold stimulus, reciprocity rule and autotropic reactions to a range of g-force stimulations of different intensities and durations The tests avoided the potentially complicating effects of earth's gravity and the interference from clinostat ambiguities. Using slow-speed centrifuges, coleoptiles received transversal accelerations in the hypogravity range between 0.1 and 1.0 g over periods that ranged from 2 to 130 min. All responses that occurred in weightlessness were compared to clinostal experiments on earth using the same apparatus.
Characteristic gravitropistic response patterns of Avena were not substantially different from those observed in ground-based experiments. Gravitropic presentation times were extrapolated. The threshold at 1.0 g was less than 1 min (shortest stimulation time 2 min), in agreement with values obtained on the ground. The least stimulus tested, 0.1 g for 130 min, produced a significant response. Therefore the absolute threshold for a gravitropic response is less than 0.1 g.     

Phototropism of rice (Oryza sativa L.) coleoptiles: fluence-response relationships, kinetics and photogravitropic equilibrium

Phototropism of rice (Oryza sativa L.) coleoptiles induced by unilateral blue light was characterized using red-light-grown seedlings. Phototropic fluence-response relationships, investigated mainly with submerged coleoptiles, revealed three response types previously identified in oat and maize coleoptiles: two pulse-induced positive phototropisms and a phototropism that depended on stimulation time. The effective ranges of fluences and fluence rates were comparable to those reported for maize. Compared with oats and maize, however, curvature responses in rice were much smaller and coleoptiles straightened faster after establishing the maximal curvature. When stimulated continuously, submerged coleoptiles developed curvature slowly over a period of 6 h, whereas air-grown coleoptiles, which showed smaller phototropic responsiveness, established a photogravitropic equilibrium from about 4 h of stimulation. The plot of the equilibrium angle against log fluence rates yielded a bell-shaped optimum curve that spanned over a relatively wide fluence-rate range; a maximal curvature of 25° occurred at a fluence rate of 1 μmol · m⁻² · s⁻¹. This optimum curve apparently reflects the light sensitivity of the steady-state phototropic response. Received: 28 June 1996 / Accepted: 30 July 1996     

Redistribution of Endogenous Indoleacetic Acid, Abscisic Acid and Gibberellins in Geotropically Stimulated Ribes nigrum Shoots

The presence of IAA, ABA and gibberellins in extracts of shoots of Ribes nigrum was demonstrated by gas-liquid chroma-tography (GLC) for both IAA and ABA and by the lettuce hypocotyl assay for gibberellins. Quantitative estimation of the three substances in extracts from upper and lower halves of shoots which had been kept horizontal, and which showed negative geotropic response after 4 h, indicated a redistribution of hormones during the geotropic stimulation. The ratio of the hormones in lower and upper halves was 3.8:1 and 2.8:1 for IAA and giberellins respectively, whereas the ratio of ABA in upper and lower halves was 2.1:1. There is, however, no evidence for the participation of gibberellins and ABA in the early development of negative geotropic curvatures, since shoots of intact Vicia faba seedlings treated with 100 mg/1 solution of GA₃, ABA and 10 mg/1 IAA for 30 min prior to geotropic stimulation, developed negative geotropic curvatures, although shoots pretreated with 50 and 100 mg/1 IAA did not develop curvature.     

Gravitropism of maize and rice coleoptiles: dependence on the stimulation angle

Gravitropism of maize and rice coleoptiles was investigated with respect to its dependence on the angle of displacement or the initial stimulation angle (ISA). Close examination of curvature kinetics and the response to a drop in stimulation angle (SA) indicated that the gravtropic response during an early but substantial part of the curvature development is directly related to the ISA, there being no effect of the reduction of SA resulting from the curvature response itself. On the basis of this finding, the relationship between the steady SA and the curvature rate was determined. In maize, the curvature rate increased linearly with the sines of SAs up to an SA of 90 degrees. Rice coleoptiles, however, showed a saturation curve in the same range of SAs. The saturation profile was nearly identical between coleoptiles grown in air and those submerged in water, although the latter elongated much faster. Rice coleoptiles appeared to be far more sensitive to gravity than maize coleoptiles. It is concluded that the sensitivity to gravity, assessed through dependence on ISA, is a property inherent to a given gravitropic organ. Long-term measurements of curvature indicated that the coleoptiles bend back past the vertical. This overshooting was marked in submerged rice coleoptiles.