Nondimensionalizing and what to do

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The discussion revolves around the concept of nondimensionalizing variables in fluid dynamics, specifically in the context of a rectangular channel. The paper in question uses the half-width of the channel as a characteristic dimension, leading to the question of whether the fluid depth parameter, ##h##, is dimensionless. It is clarified that while ##h## is a parameter, it can still be treated as dimensionless when normalized by natural units. The conversation emphasizes the importance of maintaining dimensional consistency when converting variables like ##y## into dimensional form by multiplying with the appropriate natural unit. Overall, the thread highlights the nuances of dimensional analysis in fluid mechanics and the importance of understanding how to handle units in calculations.
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Hi PF!

There is a paper I'm reading about fluid that is sloshed in a rectangular channel, where the width is ##x##, the length of of the channel is ##z##, and the channel height ##y##. The paper reads: "All further discussion will be carried out in dimensionless variables, choosing the half-width ##l## of the channel as the characteristic dimension. Then in Cartesian coordinates the region ##\Omega## occupied by the fluid in the equilibrium state is determined by the inequalities $$-1<x<1,\,\,\,\,h\leq y \leq \Gamma(x)$$ where ##h## is the depth of the fluid and ##y =\Gamma(x)## is the equation for the surface."

My question is, is ##h## dimensionless? Later in the paper ##h## is a parameter, but when comparing to an experiment, is ##h## dimensional?
 
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If they state that they will use dimensionless variables you should probably trust them. That means that all variables have been normalised by the corresponding natural unit.

Having h as a parameter does not prevent it from being dimensionless.
 
Orodruin said:
If they state that they will use dimensionless variables you should probably trust them. That means that all variables have been normalised by the corresponding natural unit.

Having h as a parameter does not prevent it from being dimensionless.
So how do I get ##y## into dimensional form? This is confusing because they don't state what ##h## is beyond the lower bound. It makes sense to me that dimensionally ##-l\leq x\leq l## and after non-dimensionalizing becomes ##-1\leq x \leq 1##, but how to get ##y## into dimensional form?
 
Multiply by the corresponding natural unit, just like for ##x##.
 
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Orodruin said:
Multiply by the corresponding natural unit, just like for ##x##.
Great, that's what I thought. And area ##l^2##. Thanks!
 
Note that, in a sense, we are always doing this whenever we are using actual values for physical variables. The only difference here is that the length unit is chosen based on a dimension present in the problem, not on a preexisting definition (such as cm or inches).

If you are entering numbers into a calculator, those are dimensionless. It is up to you to keep track of the units. The same goes for computer code. (Unless you are like me and program your own C++ class to take care of units for you.)

For example, in uniform motion of 12 m taking 3 s. What you would put into the calculator is 12/3=4. This is dimensionless. It is up to you to take care of the units, which are 1 m and 1 s. Dividing the units gives you a speed unit (1 m)/(1 s) = 1 m/s.
 
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Yea, that's a good call! I like seeing things from this view.

Ummmm I don't use C actually but perhaps if computations get spendy I may switch over...

And thanks for the help!
 

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