Embryology Biology 441 Spring 2012 Albert HarrisHow mechanical forces cause geometrical shapesGenes > Forces > Anatomy

Many structures of the body are mechanically equivalent to water balloons. Fluid interiors pushing out, inflating flexible surfaces. Here are sixteen examples. Please try to think of more. Let's try for 20. #1) Hollow blastulas (sea urchins) and blastocysts (mammals) are examples.
#2) The brain, and the rest of the central nervous system, are a hollow, fluid filled tube. A simple experiment is to poke a small hole in any part of the neural tube, and reduce the pressure to near zero. Insertion of a hollow glass tube will prevent the hole from closing. This results in the brain lobes not inflating. #3) The eyeball is inflated with a weak gel, which acts like a liquid. Inserting a hollow glass tube through the eyeball will prevent its inflation. (Dr. Coulumbre proved this, at the NIH) #4) Teleost oocytes form their upwardbulging blastodisk by cytoplasmic pressure pushing against a circle where the contractility of the cell cortex is weaker than elsewhere. #5) Cleavage (cytokinesis) of all animal cells is caused by strengthening of cytoplasmic actomyosin in the circumferential direction in a beltlike contractile ring that pinches the cell in two after mitosis (And separate from the mechanism of chromosome movement in mitosis). #6) Polar body formation is a special unequal form of cytokinesis, that follows each meiotic division of oocytes. #7) Cartilages expand by electroosmotic pressure pushing outward against resistance of collagen and elastin fibers. These fibers wrap around the outside of each cartilage, and also run through the interior of the cartilage. Visualize water balloons with very gooey water inside, and with nylon threads and rubber bands wrapped around the outside, and also running through the interior, The shapes of the bones that will later replace cartilages are created by directional differences in cartilage swelling. "Long bones" get their shapes from resistance to swelling being stronger in the circumferential direction, and weaker in the direction of greatest elongation. NOTE: To the extent that the outward swelling pressure is osmotic, this pressure is not capable of being stronger in one direction in any direction than in any other direction. (Ask yourself: can a concentration of ions be stronger in one direction than another? Hint: No) Chemical concentrations can easily be larger in some place than others, but can't be larger in any direction than another. Be careful not to confuse this with chemical gradients, in which concentrations change from place to place.
Gradients DO have directions; (they are vector quantities) #8) Notochords are tightly packed with weak, vacuolated, jellylike, cells; and are tightly wrapped with sheets of collagen fibers, running in spirals. #9) Blood vessels (arteries, veins, capillaries) are lined with a special kind of thin epithelial cells named "endothelial cells", which are wrapped by collagen fibers, smooth muscle cells, and fibroblasts. It's an unasked mystery what mechanism wraps them with collagen. Another is why smooth muscle cells orient circumferentially; perpendicular to what contact guidance usually produces!
#10) The chambers of the heart; I hope you now agree that embryology needs whatever mathematical concepts, tools, vocabulary or methods help us think cumulatively & make sense of counterbalances between fluid pressures and stretched surfaces. I promise these first steps won't be difficult or require equations. HERE WE GO...
Tensions are not scalars, and they are not vectors either.
Many important variables belong to this new category:
The curvature of surfaces belongs to this other category of variable. Try to imagine a gradient of a vector! Would it be another vector? Or what?
Scalar variables have an amount at each location in space. The first such variable that mathematicians analyzed was tension (and compression, which equals negative tension) So they named the whole category of variables "tensors"
Tension (equals "stress") is a tensor. (a symmetric tensor of the second order)
Notice that they didn't invent new words for third, fourth, fifth order tensors! A ratio of a second order tensors to a third order tensor would be a fifth order tensor. (You add the numbers of the orders) Elastic resistance is the ratio of stress to strain. 4 = 2 + 2 Don't worry too much about the following small fact, which I hope may give you some sense of direction: Tensor variables differ as functions of direction according to certain equations (which I won't even tell you, lest you memorize them), which contain either the cosine of the directional angle, or the cosine squared of that angle, or the cosine cubed, or the cosine to the fourth power, etc. Fourth order tensors vary as the fourth power of the cosine of the directional angle; Second order tensors vary as the cosine squared, etc. An interesting consequence is that except where curvatures and tensions happen to be the same in all directions (spheres, planes, etc.) then for any second order tensor their maximum directions are always exactly perpendicular to their minimum directions. However much it seems as if surely you could carve a block of soap, or twist a block of rubber, such that curvatures and stresses wouldn't have maxima perpendicular to minima, it's logically impossible.
Just because a tensor variable can in principle vary with direction, it doesn't have to.
Soap bubbles are a good example. Another is the surface tension of droplets of liquid.
Tension at their surfaces are caused (and resisted) by tendencies of liquids to leave the surface and move into the liquid. Notice that balloons are different. The tensions at their surfaces are caused by stretching rubber. These tensions can be different in one direction from another, and also different from one place to another. But maxima and minima still can't help being perpendicular. Living cells, with actively contractile cortical layers of "cytoplasmic actin and myosin" are capable of even more variation than soap bubbles. The same is true of sheets of living cells. This free ability to vary includes the ability to contract with equal strengths in all directions and at all locations. That will cause cells and groups of cells to behave as if they had a "surface tension". Many scientists have mistakenly concluded that isotropic contraction must be caused (literally) by surface tension.
"How do you KNOW she is a witch?" 'She is made out of soap!'
D'Arcy Thompson mistakenly persuaded himself and his readers that selfbuilding shapes can only result from tensions that don't vary with direction; others believe that convergence to any consistent geometry, via two or more alternative sequences of intermediate geometries, can only be caused by forces that are reversible, conservative and minimize of free energy. Mathematicians tend to think that they somehow "own" the concept of tensors, think of them more in the sense of "transformation of number matrices", not as physical variables, and prefer biologists not to use them. Better they should be helping us understand extracellular matrices. Incidentally, tensors played a major role in the escape of physics from the "ether" concept, which was analogous to "positional information" in today's embryology. Some engineering and mathematical concepts embryologists need. (& 99% of biologists never learn about)
Stress = mechanical force per crosssectional area: Either tensile stress or compressive stress
Strain= proportional stretching or compression (produced by stresses)
Young's modulus = the slope of the curve of stress per strain
Hooke's law = linear proportionality of stress to strain
Please understand that Hooke's law is NOT a law of nature.
Also, when Hooke's Law is not obeyed, then
Young's modulus is not constant, & so doesn't really exist
SOME EQUATIONS WE WILL TALK ABOUT TODAY ARE EXACTLY TRUE. The curvature of surfaces and layers may be the single most important variable for us to understand, in relation to shape.
Curvature = angular change of the tangent line per distance
the Radius of Curvature = 1 / divided by curvature
A straight line has zero curvature .
A circle has constant curvature . A sphere has constant curvature in all directions . A plane has zero curvature in all directions. What is the curvature of the surface of a cylinder? ...of the surface of a cone? ...of the surface of a lemon? ...of the surface of an eyeball?, or a lens?
A cylinder has zero curvature in the lengthwise direction;
Curvature of surfaces varies with direction, It turns out that stress and strain also can vary with direction.
And elastic moduli vary even more with direction. Differential Geometry is a division of higher mathematics in which shapes are defined in terms of curvatures, instead of the x, y. z coordinates that we learn about in elementary mathematics.
Stress, strain and curvature (of surfaces)
You know something about vectors , right?
Examples of scalar variables: temperature, chemical concentrations Examples of vector variables: wind speed, magnetic force (also gradients of scalar variables are vectors)
Vectors can (correctly!) be regarded as tensors of the first order. Stress, strain and curvature are tensors of the second order. Elastic moduli are tensors of the fourth order.
(I think maybe birefringence is a tensor of the third order)
Do not be frightened by tensors. They are your friends.
A stretched string can exert sideways pressure
"Tension " means the same thing as tensile stress. Pressure across a flexible sheet of material obeys this equation:
Pressure = T * C + t * c
Because tension and curvature can vary with direction,
Really, it could be more accurate to take some kind of integral.
For a soap film, the mechanism that generates the tension has the same strength in all directions: therefore: P = T * (C + c) If we stretch a soap film across a curved ring, then P=0 so C = c Which is another way of saying that, at each location on the film, curvatures in perpendicular directions are exactly equal & opposite
The pressure inside a big bubble
Inside any given bubble, Pressure is a constant at each part of the surface. Although stretching a bubble may cause this interior pressure to change, nevertheless P = T * (C + c) In a complex froth of bubbles, there will be different pressures in different bubbles, and curvatures will vary widely, but they will always obey these equations [EXACTLY] The surface tension of bubble surfaces (and liquid interfaces) does not vary as a function of direction. That is NOT true of a rubber sheet, or a balloon, or an eyeball, etc. much less of the surfaces of cells, or of epithelial sheets! (liquid and bubble interfaces are special cases, not a law of nature)
When tension can vary with direction, then P = T*C + t*c
This equation controls the shape of the eyeball: If T in the cornea is made 1/3 as strong as in the sclera, then the curvature of the cornea will be 3 times larger than the sclera.
You let me control the Ts and Ps: I can make the Cs do what I want!
Developmental biology is about how genes create & control anatomy The equations above cause the shape of the brain, the shape of cartilages (and thereby, the whole skeleton), the shape of limb buds, the diameters and branching patterns of blood vessels, etc. etc. etc. This is very important for plastic surgery, & many other specialties To understand these issues (even a little) puts you way ahead of other future MDs. Unfortunately, it is difficult to measure or map forces inside developing embryos, or to cause experimental changes in forces, or to predict exactly what differences are predicted by theories. Much published research in this area has been based on fundamental mistakes, misunderstandings, and oversimplifications. For example, the directional elongation of cartilage is claimed to be caused by directional secretion of matrix and growth of cells. Can you see why this is impossible and can't be the true explanation?
But the electroosmotic pressure of cartilage is a scalar, which means it cannot possibly vary with direction. Pressure can vary from one location to another; and that can contribute to shape; but directional expansion has to be mostly caused by weakening of tension in one axis relative to tensions in the perpendicular axes.
Reducing tensions inside embryos causes spatial irregularities and major birth defects, as extreme as doubling of organs.
These photographs show the development of the embryonic rudiments of feathers in pieces of bird skin. When the skin develops normally, on the embryos surface (or if it is kept under mechanical tension) then the feather rudiments form with highlyregular spatial periodicity. But when skin is cultured without the normal amount of mechanical tension, then the feather rudiments form at irregular positions. On the surface of a soap film , or a balloon , in which the internal pressure is the same at all points on the surface, then pressure is equal to stress multiplied by curvature. In other words, the local amounts of stress automatically adjust according to the local amounts of curvature , so that one multiplied times the other is a constant everywhere. To the extend that the material is flexible, & pressure is constant. If tension (=stress) becomes larger, then curvature becomes smaller. Curves can be defined by the amount of curvature at each point. (Negative curvature means the line has curved back on itself) Polarized light is one of the only methods by which one can "see" the complicated geometric patterns of mechanical stresses inside developing embryos.
Although the following is beyond the scope of this course, you may be interesting in knowing that one of the advantages of using mechanical forces for the direct control of anatomical patterns is that such mechanisms can directly optimize the geometrical arrangements of organs, for example in the branching patterns of blood vessels.
There is a classic problem in higher Mathematics called "Plateau's Problem" which is to calculate equations for the surface that has the minimum total area for a given perimeter. These diagrams show computer solutions for Plateau's Problem for an arbitrarily shaped edge. A soap film stretched across a wire will automatically "find" the shape that has the minumum total area. Any sheet of material that contracts with the same amount of tension in all directions will also "find" the shape with the minimum total area. But if a sheet of material contracts with a stronger force in some directions than in other directions, then the shapes that it will form will be different than those formed by soap films. The shapes that are formed do not depend on whether the contracting layer is made out of soap, or rubber, or living cells. What matters is whether the tension varies with direction, or varies from place to place. If a layer of cells happens to contract with the same strength at each place, and in all directions, then the shapes it will form will be the same as would be formed by a soap film. Unfortunately, when cell contraction happens to obey such simple rules, then many people say the force must be "surface tension". Textbooks often say this. But active contraction by actin and myosin can obey simple rules, or it can obey more complicated rules, in the sense of exerting stronger stress at some locations than others, or stronger stress in some directions than others. Such increased asymmetry of the forces exerted is a very effective way to create anatomical shapes. Most biologists have never learned the simplest concepts of tensor properties, or different kinds of symmetry. So when a contractile layer begins to contract more in one place that another, or more strongly in one direction than another, 99% of embryologists don't know how to think about what is happening. The subfield of mathematics that finds shapes and equations that minimize or maximize some property is known as "The Calculus of Variations". So, Plateau's Problem is one of many problems that belongs to the calculus of variations. The category of computer simulations that predicts (simulates) shapes and tension patterns that will be produced by materials as a result of obeying a given set of rules are called "Finite Element Methods". Although the actual materials you are interested in consist of infinite numbers of points, the computer simulation is based on a deliberately simplified, and finite, set of points with forces acting between then. Millions of dollars are spent on finite element simulations of anatomical organs, and more research of this kind is needed. For example, some finite element simulations of sea urchin gastrulation and of neurulation in birds and amphibians have been published in embryological journals. (Google "George Oster".
Much further research is needed on this general topic. This research is being held back by mistaken theories that genes can only work by controlling the x, y, z coordinates where cells will differentiate. Sometimes, that's actually what happens (probably). But it's wrong to think chemical patterns always have to come first, and control mechanical and geometric patterns. But people who have never heard of differential geometry or tensors, but only studied about x, y, z coordinates, tend to assume that coordinates are the only possible way genes could create geometrical patterns.
Threedimensional shapes of cells, whole organisms and of tissues and organs are created, controlled, changed, and healed in large part by means of adjusting contractile forces at cell surfaces (surfaces, layers of cytoplasmic actin and myosin just inside membranes), organ surfaces, and interfaces between cells and tissues. A few examples,
2) lobes of the developing brain 3) chambers of the heart 4) cytokinesis (cleavage) of cells 5) osmotic swelling of cartilage and shaping of bone 6) intervertebral discs (and their herniations “slipping”) 7) aneurisms of arteries 8) varicose veins 9) alveoli of lungs, branching of bronchi 10) branching angles of arteries 11) blastula formation, and many more examples.
For example by localized contraction of cytoplasmic actin cortexes adjacent to concave surfaces of invaginating cell sheets. If you had a magic wand that could control surface curvatures, then you could change and create the shapes of everything. More often, curvatures are indirectly controlled by adjusting stresses (tensions) and pressures P = C*T + c*t If you let me control the amounts of T and t, then can I control C and c? Do I also need to control P? There has been lots of unnecessary confusion on these issues. One fact to get used to is that curvature can also be measured as "radius of curvature". C = 1/R If you measure angles in radians, rather than degrees (a 180 degree angle is Pi radians) A circle whose tangents change by 1 radian per centimeter has a radius of 1 centimeter. I would have spared you this, except that biologists have mostly expressed surface curvatures in terms of radius of curvature; so you see equations like this P = T/R +t/r or worse than that!: P = T (1/R + 1/r) Do you see what's being slipped past us by this second equation above? Tension is being treated as if it were a scalar variable, or a scalar CONSTANT! For some special cases, like soap bubbles, T cannot vary with direction or location. (It is isotropic and homogeneous). That also makes the math easier, but many people (including D'Arcy Thompson) mistook this special case for a general rule. (He didn't understand physics well enough to realize what he was assuming.) Thompson could only explain a few special biological shapes. But left almost everybody with the impression that he had exhaustively explored all the possibilities for creating biological shapes be means of surface tensions. (It's as if Columbus had expected to discover new continents, but come back after finding Bermuda, & said that was all there was. Consider specific questions: A) Two soap bubbles, sharing a side; one bubble bigger than the other.
2) Or does the big bubble bulge into the smaller bubble? 3) Or does the smaller bubble bulge into the big one? 4) Does the answer differ from one try to another?
5B) Big bulges into little 5C) Little bulges into big 5D) Result varies; depends on other factors? Is random? Unknowable?
7) What if two blastulas shared a side; one bigger & the other smaller. 8) What if two spherical masses of reaggregated sponge cells adhered along one side.
