The Shuttle Experiment takes advantage of magnetic heterogeneity of gravity-sensing cells (statocytes), which respond to the displacement of typically starch-filled amyloplasts. Ponderomotive magnetic forces, act on structures of different magnetic properties in High Gradient Magnetic Fields (HGMF). The magnetic system consists of ferromagnetic wedges, magnetized by strong permanent NdFeB magnets. The HGMF result from the high density of magnetic field lines in the wedges with the greatest density at the wedge tip. The field density decreases at the transition from the ferromagneticas wedge to air and thus forms the HGMF. The HGMF affects amyloplasts through a ponderomotive force, comparable with the gravity force. The magnetic force is a function of the magnetic gradient and decreases with the distance from the edge. Flax seedling will be allowed to grow such that the tips of their roots pass through the HGMF. As a result of the internal displacement of the amyloplasts the roots are expected to curve as if they were gravistimulated.

We have the following objectives:


MORE INFORMATION ON PHYSICAL PRINCIPLES UNDERLYING OUR EXPERIMENT.

We are exploiting heterogeneity of magnetic susceptibility (æ) of plant gravity receptor cells (statocytes) to displace statoliths (dense starch-filled organelles, a.k.a. amyloplasts) inside the cells. Intracellular sedimentation of statoliths is presumed to be the primary step of gravity perception in plants. A possibility to displace them without affecting the rest of the plant by centrifugation or re-orienting in the gravity field is a potent research tool for studying plant graviperception and signal transduction. Statoliths are stronger diamagnetics, than the cytoplasm [1-6]. In a non-uniform magnetic field they are repulsed from stronger field zones by the ponderomotive magnetic force: Fm= (æpcp)Vgrad(H2/2), where æp is the magnetic susceptibility of plastids, æcp - that of cytoplasm, grad(H2/2) is the dynamic factor of the magnetic field. If magnetic field is very strong and very non-uniform (so-called high gradient magnetic field [HGMF]), with grad(H2/2)= 109 to 1010  Oe2/cm, this force can be equivalent to the gravity force. In our experiments with several types of magnetic systems [1-10] we were able to displace amyloplasts inside receptor cells in roots [2-6] and shoots [7,8,10] of higher plants, and inside protonemata of the moss Ceratodon purpureus [9]. This displacement (intracellular magnetophoresis) caused positively gravitropic organs (roots of flax and Arabidopsis, wwr-mutant of Ceratodon) to curve in the direction of amyloplast displacement (i.e., away from the stronger field), while negatively gravitropic organs (shoots of tomato and barley, WT of Ceratodon) curved in the direction opposite to the amyloplast displacement. This pattern of the physiological response of the plants is consistent with gravitropism, and the kinetics of the curvature is similar to the gravitropic curvature [1-10]. Starchless mutant of Arabidopsis did not curve in HGMF, indicating, that starch-filled bulk organelles are necessary for the effect, and that other cell components are not significantly affected by the field [4]. This shows, that magnetic ponderomotive forces acting on amyloplasts can simulate gravity for plants.

This approach not only can provide information on physical heterogeneity of the cells and organelles, but also can serve as a research tool for signal transduction in plants. Such manipulation of amyloplasts is likely to answer some of the basic questions of the sequence of events in gravisensing and a possible involvement of the cytoskeleton in graviperception. We can also expect answers as to whether amyloplast displacement or the force that amyloplasts exert on the ER system leads to the cascade of events that results in curvature. Small size of the area of HGMF with a significant dynamic factor allows to stimulate only a small portion of receptor cells of a bigger plant organ, allowing to study relative sensitivity and importance of different regions of the organ for gravity perception and response [7,8,10], which is impossible to do by any other method.


distribution of magnetic field near the tip of a magnetized ferromagnetic wedge Figure 1. High Gradient Magnetic Field (HGMF) in the vicinity of an edge of a ferromagnetic wedge magnetized by a (uniform) external magnetic field. The density of field lines is proportional to the field intensity, red arrows indicate the direction of force acting on diamagnetic substances. Diamagnetic amyloplasts would move away from the wedge edge and positively gravitropic roots are expected to curve as shown.


Our publications on the topic.

  1. Kuznetsov AA, Kuznetsov OA 1989 Simulation of gravity force for plants by high gradient magnetic field. Biofizika, 35: 835-840.
  2. Kuznetsov OA 1989 Some applications of magnetophoretic methods to plant physiology problems, MS thesis, Dolgoprydny, Russia: 85p.
  3. Kuznetsov OA 1993 Non-uniform magnetic field and relaxational oscillations as instruments for plant cell exploration. PhD thesis, Moscow, Russia: 132p.
  4. Kuznetsov OA, Hasenstein KH 1996 Magnetophoretic induction of root curvature. Planta 198: 87-94.
  5. Hasenstein KH, Kuznetsov OA, Blancaflor EB 1996 Induction of root curvature by magnetophoresis and cytoskeletal changes during graviresponse. Proceedings of 6th European Symposium on Life Sciences Research in Space, Trondheim, Norway: 71-74.
  6. Kuznetsov OA, Hasenstein KH 1997 Magnetophoretic characterization of plant gravity receptors. in: Scientific and clinical applications of magnetic carriers. (U.Hafeli, W.Shutt, J.Teller, M.Zborowski, eds.), Plenum Press, New York: 429-444.
  7. Kuznetsov OA, Hasenstein KH 1997 Magnetophoretic induction of curvature in coleoptiles. J. of Exp. Botany 48 (316): 1951-1957.
  8. Hasenstein KH, Kuznetsov OA 1999 Graviresponse of lazy-2 tomato seedlings to curvature-inducing magnetic gradients is modulated by light. Planta 208: 59-65
  9. Kuznetsov OA, Schwuchow J, Sack FD, Hasenstein KH 1999 Curvature induced by amyloplast magnetophoresis in protonemata of the moss Ceratodon purpureus. Plant Physiol. 119 (2): 645-650
  10. Weise SE, Kuznetsov OA, Hasenstein KH and Kiss JZ 2000 Displacement of amyloplasts in Arabidopsis inflorescence stems causes localized curvature. Plant Cell Physiol. 41: 702-709.
  11. Kuznetsov OA, Brown CS, Levine HG, Piastuch WC, Sanwo MM, Hasenstein KH 2000 Composition and physical properties of starch in microgravity-grown plants. Adv. Space Res. 27: 887-892
  12. Kuznetsov OA, Hasenstein KH 2001 Intracellular magnetophoresis of statoliths in Chara rhizoids and analysis of cytoplasm viscoelasticity. Adv. Space Res. 28: 651-658