Another point is that the laws of chemistry which underlie biological processes are all thought to be based on electromagnetic interactions between molecules, and the equations of electromagnetism have the mathematical property of "Lorentz-invariance", which means they must work the same way in the different inertial reference frames used in SR, which means the speed of all electromagnetism-based clocks moving at velocity v in a given frame must be observed to slow down by [tex]\sqrt{1 - v^2/c^2}[/tex]. The only way biological processes wouldn't slow down is if they did not obey the known laws of electromagnetism.
To understand what Lorentz-invariance means mathematically, it might be a little easier to first look at the meaning of Galilei-invariance. In Newtonian physics, if you have two coordinate systems moving at velocity v relative to each other along their respective x-axes, and one uses coordinates (x,y,z,t) while the other uses coordinates (x',y',z',t'), then to transfrom between the two coordinate systems you'd use the "Galilei transform" here:
[tex]x' = x - vt[/tex]
[tex]y' = y[/tex]
[tex]z' = z[/tex]
[tex]t' = t[/tex]
and
[tex]x = x' + vt'[/tex]
[tex]y = y'[/tex]
[tex]z = z'[/tex]
[tex]t = t'[/tex]
To say a certain physical equation is "Galilei-invariant" just means the form of the equation is unchanged if you make these substitutions. For example, suppose at time t you have a mass [tex]m_1[/tex] at position [tex](x_1 , y_1 , z_1)[/tex] and another mass [tex]m_2[/tex] at position [tex](x_2 , y_2 , z_2 )[/tex] in your reference frame. Then the Newtonian equation for the gravitational force between them would be:
[tex]F = \frac{G m_1 m_2}{(x_1 - x_2 )^2 + (y_1 - y_2 )^2 + (z_1 - z_2 )^2}[/tex]
Now, suppose we want to transform into a new coordinate system moving at velocity v along the x-axis of the first one. In this coordinate system, at time t' the mass [tex]m_1[/tex] has coordinates [tex](x'_1 , y'_1 , z'_1)[/tex] and the mass [tex]m_2[/tex] has coordinates [tex](x'_2 , y'_2 , z'_2 )[/tex]. Using the Galilei transformation, we can figure how the force would look in this new coordinate system, by substituting in [tex]x_1 = x'_1 + v t'[/tex], [tex]x_2 = x'_2 + v t'[/tex], [tex]y_1 = y'_1[/tex], [tex]y_2 = y'_2[/tex], and so forth. With these substitutions, the above equation becomes:
[tex]F = \frac{G m_1 m_2 }{(x'_1 + vt' - (x'_2 + vt'))^2 + (y'_1 - y'_2 )^2 + (z'_1 - z'_2 )^2}[/tex]
and you can see that this simplifies to:
[tex]F = \frac{G m_1 m_2 }{(x'_1 - x'_2 )^2 + (y'_1 - y'_2 )^2 + (z'_1 - z'_2 )^2}[/tex]
In other words, the equation has exactly the same form in both coordinate systems. This is what it means to be "Galilei invariant". More generally, if you have any physical equation which computes some quantity (say, force) as a function of various space and time coordinates, like [tex]f(x,y,z,t)[/tex] [of course it may have more than one of each coordinate, like the [tex]x_1[/tex] and [tex]x_2[/tex] above, and it may be a function of additional variables as well, like [tex]m_1[/tex] and [tex]m_2[/tex] above] then for this equation to be "Galilei invariant", it must satisfy:
[tex]f(x'+vt',y',z',t') = f(x',y',z',t')[/tex]
In relativity, instead of using the Galilei transformation to transform between coordinate systems moving at velocity v relative to each other, you use the Lorentz transformation:
[tex]x' = \gamma (x - vt)[/tex]
[tex]y' = y[/tex]
[tex]z' = z[/tex]
[tex]t' = \gamma (t - vx/c^2)[/tex]
where [tex]\gamma = 1/\sqrt{1 - v^2/c^2}[/tex]
and
[tex]x = \gamma (x' + vt')[/tex]
[tex]y = y'[/tex]
[tex]z = z'[/tex]
[tex]t = \gamma (t' + vx'/c^2)[/tex]
So just as with Galilei-invariance, Lorentz-invariance means that if you take some equation for a law of physics written in terms of x,y,z,t coordinates and use the Lorentz transform to make substitutions and rewrite this equation in terms of x',y',z',t' coordinates, the equation will end up looking the same as if you had just replaced x with x', y with y', z with z' and t with t'--the equation should have exactly the same form in both coordinate systems. This means that any equation that's Lorentz-invariant should satisfy:
[tex]f( \gamma (x' + vt' ), y' , z', \gamma (t' + vx' /c^2 ) ) = f(x' ,y' ,z' , t')[/tex]
As long as all the fundamental equations of physics are Lorentz-invariant, it must be true that you'll see phenomena like time dilation and Lorentz contraction...perhaps this will help answer the question asked by Sam Woole and Sherlock about what the "physical explanation" for these phenomena is. If you were writing a computer program to simulate an imaginary world with any laws of physics you wanted, and all the equations you picked to govern the simulation happened to have this mathematical property of Lorentz-invariance, then you would automatically see time dilation and Lorentz contraction in the simulated world, whether you had planned it that way or not.