A turbine blade (or any propeller blade) is essentially a rotating wing. Because this wing is rotating, the velocity along the span of the wing will not be constant. Specifically, it will increase from 0 at the hub to the angular velocity times the length of the blade at the very tip. Or:
V_{tip} = \omega L
However, this velocity variation is only in the plane of the blade. There is also a velocity component moving perpendicular to the blade or in other words, along the direction of the hub. If you resolve these velocity components you find that the wind direction is actually coming at an angle relative to the blade. This angle is greatest at the tip of the blade.
To generate thrust the blade, being a wing, essentially has to generate lift. The equation for lift is as follows:
L = C_{L} 1/2 \rho V^{2} S
L = lift
CL = lift coefficient
\rho = air density
V = wind velocity
S = Blade project surface area
The lift coefficient is the key here, it is almost always experimentally determined and has been found to be proportional to
C_{L} \propto [ \alpha, M, Re ]
Where:
Re = reynolds number, the ratio of inertial forces to viscus forces most basically
M = the mach number, ratio of wind velocity to speed of sound
α = angle of attack, the angle of the blade relative to the direction of the wind.
For the most basic cases:
CL varies linearly with \alpha
As Re increase the maximum possible CL increases
CL varies minimally with M as M<.3, when M>.3, CL slightly increases as M increases. Crazy things happen when M>1, you can actually get negative lift with the same airfoil shape at lower speeds! I tried to find a more concise explanation of the trend, but I couldnt. I may contribute later on tonight if I can dig up one of my old books.
All else being equal, it is clear that the lift coefficient is the key to changing the blade performance. It is also suffice to say that the angle of attack is the only thing a designer has direct control over given some set of operating conditions. In conclusion, the blades are twisted to change the angle of attack and thus the blade performance.
What are some examples of performance parameters?
If you wish to design a highly efficient blade you would want to minimize the total drag incurred. To do this, you must ensure that the CL/CD (CD being the drag coefficient, analogous to the lift coefficient) is maximized along the span. For every section of a wing, there exists a maximum CL/CD which is proportional too...α!
If you want to produce a blade that gives you the most amount of lift for a given rotation speed, you want to maximize CL along the span. Again, the maximum value of the lift coefficient is strongly proportional to...α!
In addition, you can create special CL distributions along the span of the blade, which may meet some design criteria.
Hope this helped. Also, check out http://www.desktop.aero/appliedaero/preface/welcome.html for more info.