Jarfi said:
What exactly is the deal with turbulence? why does it scare you guys so much, to me all it is is waves, disorted waves and the transfer of kinetic energy trough a medium. So if the medium is not solid the kinetic energy will spread in a very complex manner because there are billions of atoms, but it will all make common sense when you'd see it spreading, maybe hooks in molecules would disort a stream and it would all start spinning, or a wave would meet small dust particles and be disorted and disorting itself in a snowball effec.. but what's the deal, I know this is complicated but there's nothing about the fundementals I see that's weird.
Am I not getting the word turbulence, why do you say it's such a mystery? I mean it's a mystery mathematically because of all the variables(dust, shape of molecules, multiple waves and streams of medium disorting each other) so calculating 100% would need a sick computer... but in itself I don't see the complexity.
It isn't that it is scary, per se. The breakdown to turbulence starts in the free stream of a flow, where there are, in all real flows, various disturbances (vortical, acoustic, etc.). The nature of these disturbances constitutes a relatively large parameter space to explore.
Next, these disturbances interact with the surface roughness on a surface through a process known as receptivity. The result is that, through wave diffraction, fluid dynamic and probably other unknown processes, the free stream disturbances are converted into wavelengths, frequencies and amplitudes to which the boundary layer is receptive. This is a huge parameter space constituting the size and pattern of roughness on a surface, the nature of the free stream disturbances and the conditions of the boundary layer.
The boundary layer itself is similar to a forced mass-spring-damper system in that it is a dynamical system. However, it is, in general, a dynamical system consisting of multiple equations that are highly nonlinear in nature. Three of those equations are the Navier-Stokes equations, plus the energy equation, continuity equation, and (various) equation(s) of state. This complicated system has not even been proven to have a general solution (thus the millenium prize). The receptivity process provides the initial conditions by which the boundary layer is excited, and depending on a variety of parameters, these disturbances may grow, decay, or do a combination of the two. There are also a number of larger-scale phenomenon, such as crossflow or Görtler vortices, that can affect the stability of the system. For a detailed look at this whole process, check out Mack's 1984 AGARD Report titled "Boundary-Layer Linear Stability Theory".
Once those wave grow to a certain amplitude, they become nonlinear. From that point on, there is a potential interplay between any number of an infinite number of instability modes propagating through the given boundary layer, and there is no real one-size-fits-all theory to these interplays. For now, there are only some pretty good descriptions of this regime for a few select situations such as wind tunnels or flows with limited, known CFD inputs. Eventually, the nonlinear waves grow large enough that breakdown occurs to turbulence. The breakdown process is also quite unknown. This is also a nearly infinite parameter space.
Some, including myself, believe that turbulence can ultimately be described as a sort of spatiotemporal chaos. Turbulent flow, however, has never been described in sufficient detail in a way that can confirm this. In general, design using turbulent flow assumptions occurs by using the general properties we know about it, such as increased skin friction and heat transfer. Often, this is done with what are called turbulence models, ant those are really kind of a blacksmith job that get you a good-enough answer. They improve all the time, but they don't really describe the full flow, but rather the properties of interest.
Turbulent flow itself is characterized by an energy cascade through a series of increasingly small length scales, starting with the integral length scales, which are determined by the dominant flow features in the mean flow and are highly anisotropic, going all the way down to the Kolmogorov microscales, which are locally isotropic and depend on the flow properties. These small scales are where energy dissipation finally takes place, so they are equally important to the larger flow scales, yet they are often the ones that must be modeled because computational grids simply can't be dense enough to solve those flows at reasonable conditions within a reasonable length of time. The bottom line is that in order to make the problem tractable to a computer, major assumptions must be made or else the flow conditions must be so unrealistic as to not include the transition phenomenon in detail. We won't crack the problem computationally for probably at least another half-century, according to a well-known practioner of direct numerical simulation with whom I am familiar. The computational meshes are simply too large and too fine to be solvable on today's computers.
So in essence, it isn't that the problem is scary, but rather than it is huge and takes a lot of time and effort to crack. Even when computers can solve it, we will still need to develop some theoretical framework to describe it. Experiments will be useful for validating computational solutions, but they cannot hope to get the kind of detail required to truly solve the problem, so they are limited to the validation role as far as I can see.
That said, the stability (or instability, rather) of boundary layers and the eventual transition to turbulence is an interesting problem, which is why I am personally drawn to it. It is also one of the more theoretical areas of study within fluid mechanics.
Wow that took a long time to type and is still just a very quick rundown, haha!
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MagnetoBLI said:
The thermodynamic relations I currently use within aerospace engineering are dated and based upon particularly well-defined physics. This has made me desire a more undefined science where I can let my imagination play a larger role.
That's fine, then move to a more theoretical course of study. However, basing the level of theory involved in a subject based on undergraduate classes, particularly in engineering, is somewhat foolhardy. Engineering is ultimately the application of physics and mathematics, and as such, the undergraduate classes are often a blend of theory and applications and don't get too close to the bleeding edge. When you move into the graduate level, things usually get considerably more theoretical.
MagnetoBLI said:
By collective behavior, I mean a phenomena rather than matter itself.
The
only fields where you will be dealing with matter itself are things like condensed matter physics and particle physics and any applied mathematics branches dealing with these fields. Otherwise, even most other physics fields are dealing with larger phenomena.
MagnetoBLI said:
Are new variables produced frequently in fluid dynamics, i.e equivalent to the fundamental ones like temperature or pressure? I thinking that temperature and vorticity are actually not too dissimilar now, hmm...
You can't generally just create variables. The physical world only has certain properties, and after those properties have been described, you can't just pull others out of thin air. Even theoretical physics follows this pattern where most if not all the fundamental properties are known and it is a matter of proving our theories about those properties. The only variables that are ever really "produced" are things like similarity variables.
MagnetoBLI said:
The first paragraph of the following link briefly attempts to explain why fluids aren't taught in physics undergrad usually. This is what got me questioning the potential in fluids as solving turbulence seems too intractable of a problem and I'm not a pure mathematician!
http://www.ap.smu.ca/~dclarke/PHYS4380/documents/introduction.pdf
Those points are valid. Basically, other disciplines have taken over as the prime caretakers of fluid mechanics as physicists have move on to other fields like quantum mechanics. That doesn't mean that fluid mechanics is not "true physics", but rather than it just is not en vogue with pure physicists of late. It is still a staple of engineering, mechanics and applied mathematics departments worldwide, and at the graduate level, can get very, very theoretical. Indeed, the entire field of perturbation methods for the solution of nonlinear equations evolved mid-century as a result of fluid mechanics and was
later applied to theoretical physics.
Still, I am not sure what exactly it is that is concerning you here. It seems like either fluids just isn't your thing, or else you have some misguided notion about what constitutes "true" physics.