Why use mathematical modlling to study cells?
cells move in a complex environment
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| Term | Definition |
|---|---|
Why use mathematical modlling to study cells? | cells move in a complex environment |
Mathematical modeling can be used to visualize cell | Migration
Adhesion
Traction
Plasticity |
Math modeling can be used to understand how cells react to their mechanical environment like: | With cellular rigidity, stress, and compression |
Math modeling can also be used to understand how cells transmit forces on other cells like in: | Tissue (development, etc.)
Embryogenesis
Cancer |
What three tools are necessary to describe cellular phenomena quantitatively? | vectors
fields
derivatives |
Vectors are used to study | direction |
Biological application of vectors | detect the direction in which the concentration increases |
Forces are used to understand | mechanical forces and how they are generated |
Gradients are used to understand | how something is polarized in the direction of a vector |
Scalars quantify | simple values |
Vectors quantify | oriented values |
Fields quantify | values distributed in space |
Scalars (s) do not depend on | direction in space |
Examples of scalar | temperature
mass
molecular concentration
pressure |
Biological examples of scalar | Concentration of glucose around a cell
Intracellular pressure
Light intensity received by a photoreceptor |
Vectors have | direction, sense, and a magnitude |
Vectors are represented by | an arrow in space |
Vectors are defined by its components | V1, V2, V3 in an orthonormal basis (E1, E2, E3) |
The direction of a vector is that of | the line passing through both endpoints |
The sense of a vector is from | the origin to the endpoint or vice versa |
biological examples of a vector | force exerted by a cell on the matrix
migration speed of a cell
growth direction of an axon |
A field is | a function that assigns a quantity (scalar or vector) to every point in space |
Scalar field | c(⃗x) gives a scalar at each position ⃗x (e.g., temperature, concentration). |
Vector field | ⃗v(⃗x) gives a vector at each position ⃗x (e.g., fluid velocity, force). |
Dot product of two vectors | ⃗u · ⃗v = ∥⃗u∥ ∥⃗v∥ cos(θ) |
θ in a dot product of two vectors | is the angle between them |
The dot product | measures how "aligned" two vectors are |
If two vectors point in the same direction, the dot product is | maximal |
If two vectors are orthogonal, the dot product is | zero |
Biological example of a dot product | The mechanical work done by a cell is proportional to the dot product between the force vector it exerts on the substrate and the resulting displacement vector. |
dot product formula in 2D coordinates | ⃗u · ⃗v = uxvx + uyvy |
the cross product of two vectors is | a vector perpendicular to the plane containing ⃗u and⃗ v
|
the cross product is useful for interpreting | torques or moments |
biological application of cross products | a cell exerts a force (microneedle) that causes an object to rotate |
torque of a cell exerting a force can be modeled | by a cross product between the lever arm and the force |
the tensor/outer product of two vectors is denoted by | ⃗u ⊗ ⃗v |
tensor products generate | matrices |
tensor products describe | how one vector acts on another to transform directions into new ones |
it is fundamental for defining quantities in mechanics such as | stress tensor
deformation tensor |
tensor products are NOT commutative | ⃗u ⊗ ⃗v = ⃗v ⊗ ⃗u. |
in cell mechanics, the stress tensor can be expressed as: | the sum of tensor products between force and direction vectors |
biological application of tensor products | actin filaments under tension generate anisotropic stresses that can be represented by σ ∝ f ⊗⃗n,
where ⃗ f is the force per filament
and ⃗n the filament orientation. |
dot product vs. cross product | dot product measures alignment between two vectors
cross product quantifies rotational effects (torque) |
how are matrices used to represent vectors | to represent linear transformations between vectors |
matrix | an array of numbers arranged in rows and columns |
matrices can represent | a linear transformation (rotation, stretching, shearing)
a table of coefficients linking two quantities (stress, strain)
a field of values (in the case of tensors) |
matrices can be: | added
multiplied by a scalar
multiplied by a vector |
condition to be able to compute the multiplication between matrices | matrix A has p columns
matrix B must have p rows |
transpose/symmetry | the diagonals can be transposed
if A = At, then the matrix is symmetrical |
biological example of matrix transposition / symmetry | the stress tensor in an elastic medium (such as the cytoskeleton) is a symmetric matrix
-> forces are the same on both sides of a plane |
biological example of identity and inverse matrices | when a cell undergoes a deformation, one can look for the inverse transformation that would return it to its original shape (passive elasticity) |
matrices encode | stretching, shearing, or rotation effects |
differential operators such as the gradient or divergence quantify | fields such as temperature, concentration, deformation |
gradient of a scalar field | if f(x,y,z) is a scalar of molecular concentration...
the gradient of f is a vector indicating in each direction how f varies locally |
biological application of gradient of a scalar field | If f(x, y) represents a chemokine concentration, then ∇f indicates
the direction in which the cell must move to “climb” the gradient |
biological application of gradient of a scalar field pt. II | gradient of a growth factor concentration guides endothelial cells during angiogenesis |
jacobian matrix | gradient of a vector field |
biological interpretation of gradient of a vector field | this gradient encodes the local variation of the velocity field
useful for understanding cytoplasmic deformation or stress within the actin network. |
divergence of a vector field measures | outgoing flux of the field at a given point |
is divergence of a vector a scalar, true or false? | true |
biological interpretation of divergence of a vector | If ⃗v is a velocity field within the cytoplasm, then the divergence
indicates whether there is dilation (> 0) or compression (< 0). |
biological example of divergence of a matrix | The divergence of the stress tensor in the cytoskeleton gives the internal force field (traction force microscopy) |
gradient with respect to divergence | gradient applies a derivative that increases the rank of objects (scalar → vector, vector → matrix). |
divergence with respect to gradient | divergence applies an operation that decreases the rank (vector → scalar, matrix → vector). |
what is a gradient? | measures how a quantity changes locally. |
what is divergence? | measures how much of that quantity “flows out” from a point. |
tensors | a mathematical object that represents physical quantities in different coordinate systems. |
tensors are used to | generalize the notions of scalars and vectors
model physical phenomena within the cell (mechanical stresses, deformations, fluxes) |
what does a tensors' particularity allow for? | it transforms in a well-defined way when the reference frame
changes. |
tensor order 0 | scalar, represented: T
example: temperature, pressure |
tensor order 1 | vector
example: cell velocity |
tensor order 2 | tensor
example: stress tensor |
biological example of tensors | necessary to understand how cells deform, exert forces, or mechanically respond to their environment (especially those of order 2) |
what does a vector lack? | ability to describe complex directional effects such as:
the distribution of forces on a cell surface
local deformation state of the cytoplasm
elasticity or viscosity of the nucleus |
quantities the depend on the action and the application require what order of tensor? | second-order |
tensors generalize: | scalars (rank 0) and vectors (rank 1) |
second order tensors are represented by | matrices |