Transcript Math Poster

EXPERIMENTAL MODELS OF MORPHOGENESIS
David Moore & Audrius Meškauskas
School of Biological Sciences, The University of Manchester, Manchester M13 9PT, U.K.
1. There is no reason why the “rules” which govern morphogenesis should not be established. From the rules and a few dimensions, times and rate values a mathematical expression to describe the morphogenetic process could
emerge. Computer models could be derived from that to simulate the whole process. Nice idea! But where do you start? Start simple. Making a stem bend in response to a tropic stimulus is a suitably simple experimental approach.
YOU can choose when to apply the stimulus, it is easily replicated and reaction and response times can be measured readily. Also, the response itself can be measured so the quantitative demands of mathematical modelling can be
satisfied.
The gravitational imperative ...
Norm a l, upright
growth of the
fruit body
2. We have used the gravitropic reactions of mushroom fruit
bodies to study control of morphogenesis because being the
right way up is crucial to a mushroom. Changing orientation is
a non-invasive stimulus. We’ve coupled video observation
and image analysis to get detailed descriptions of the kinetics.
We’ve made and used clinostats to vary exposure to gravity,
and we’ve combined a variety of microscopic observation
techniques to make quantitative observations.
Disorient
P hototropic
response
NO
Meiosis
complete
YES
Gravisensors
Perception
threshold
exceeded
The video sequence
in the background
shows (top) a
culture placed on
its side at 16:37h.
The weight of the
cap makes the
Coprinus cinereus
fruit body swing
downwards, but by
19:19h it has bent
upwards at 45o.
Sadly, one second
later the connection
with the mycelium
breaks and the fruit
body swings round
so the cap points
downwards. But it
doesn’t give up! By
20:37 it’s back to
the horizontal; by
22:10 it’s almost
upright, and by
22:58 the cap is
fully expanded and
releasing spores.
YES
Bend a pex
upwa rds
Bend ing
signa l
6. The model we have now describes the shapes assumed by real stems of Coprinus cinereus. Bending
rate is determined by the balance between signals from detectors of the direction of gravity (a function of
the angle of the stem) and for curvature compensation (a function of the local amount of bending). In a
straight stem displaced to the horizontal the gravitropic signal is maximal and curvature compensation
signal is zero. As the stem bends the gravitropic signal weakens (as the angle of displacement of the
perception system lessens) but the bending enhances the curvature compensation signal.
NO
3. The first step is to summarize these observations and
experiments into a flow chart (as shown at left). This
concentrates attention on critical features and, in a nonmathematical way, produces a formalized description
which is a good starting point for mathematical analysis.
7. In our local curvature distribution model, therefore, straightening is determined by local curvature,
independently of the spatial orientation of that part of the stem.
Signa l from
apex migrates
basipetally
Ea ch successive
segm ent is ca used
to bend
NO
Tip angle
> 35o from the
horizontal
YES
Activate
curva ture
com pensation
4. Next, a “scheme” needs to be constructed which lends itself to mathematical expression whilst still keeping a firm footing in
cell physiology. The basic assumptions of ours are that change in the angle of the apex occurs as a result of four consecutive
stages:
(i) the physical change which occurs when the subject is disoriented (this is called susception)
(ii) conversion of the physical change into a physiological change (this is called perception)
(iii) transmission of the physiological signal to the competent tissue (called transduction)
(iv) the differential regulation of growth which causes the bend and change in apex angle (called response).
We used this scheme to estimate and calculate numerical values for the various parameters of a combined equation that could
generate apex angle kinetics which imitated the reaction of mushroom stems quite well.
8. This model is predictive and
successfully describes the gravitropic
reaction of stems treated with
metabolic inhibitors, confirming its
credibility and indicating plausible
links between the equations and real
physiology.
Com pensa tion
signa l
Gravit ropic res ponse syste m
Signa l from
apex migrates
basipetally
p
s
  d
Perception
Susception
fs ()
tr
r
Transduction
ys
Response
ytr
fp (ys)
Ea ch successive
segm ent is ca used
to straighten
Memory
ftr (yp)
d
fr (ytr)
5. This imitational model dealt with change in apex angle only.
Observations of real stems show a complex distribution of bending and
straightening. Almost 90% of the initial curvature is reversed by
subsequent straightening (we call it “curvature compensation”). A
realistic model of gravitropic bending would describe the process in space
as well as in time. This is where “imitation” ends and “simulation”
begins.
9. Where do we go from here? It’s a
predictive model, so we need to make
predictions and test them. We need to
develop the maths into three spatial
dimensions and to cope with hyphal
communities. Most importantly, we
need to convince somebody to fund the
project!
•Stoĉkus, A. & Moore, D. (1996). Comparison of plant and fungal gravitropic responses using imitational
modelling. Plant, Cell & Environment 19, 787-800.
•Moore, D. & Stoĉkus, A. (1998). Comparing plant and fungal gravitropism using imitational models based on
reiterative computation. Advances in Space Research 21 (8/9), 1179-1182.
•Meškauskas, A., Moore, D. & Novak Frazer, L. (1998). Mathematical modelling of morphogenesis in fungi:
spatial organization of the gravitropic response in the mushroom stem of Coprinus cinereus. New Phytologist
140, 111-123.
•Meškauskas, A., Novak Frazer, L. & Moore, D. (1999). Mathematical modelling of morphogenesis in fungi: a
key role for curvature compensation (‘autotropism’) in the local curvature distribution model. New Phytologist
143, 387-399.
•Meškauskas, A., Jurkoniene, S. & Moore, D. (1999). Spatial organisation of the gravitropic response in plants:
applicability of the revised local curvature distribution model to Triticum aestivum coleoptiles. New Phytologist
143, 401-407.
We thank the British Mycological Society and Federation of European Microbiological Societies for award of
FEMS short term Fellowships to the late Alvidas Stokus and to Audrius Meškauskas which enabled this
research to be initiated. A Royal Society NATO Research Fellowship to AM supported the consolidation and
further development of the work to the stage described here.