Material Derivative and Implicitly Given Variables for Velocity Calculation

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Homework Help Overview

The discussion revolves around the material derivative and its application to a function defined implicitly with respect to time and space variables. The original poster presents a problem involving a function \( F \) and its relationship to velocity components, with specific equations provided for \( F \), \( a \), and \( b \). The context includes the use of the material derivative \( \frac{DF}{Dt} \) and its implications for the given equations.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the implications of differentiating the variable \( a \) and question whether it should be treated as constant or variable in the context of the velocity equations. There is discussion about the terms involved in the material derivative and the potential need for implicit differentiation.

Discussion Status

The conversation is ongoing, with participants raising questions about the treatment of variables and the correctness of the original poster's approach. Some guidance has been offered regarding the differentiation of \( a \) and the interpretation of the velocity terms, but no consensus has been reached.

Contextual Notes

There is a noted ambiguity in the treatment of \( a \) as either a constant or a variable, which affects the differentiation process. The original problem statement has been referenced multiple times to clarify the context of the discussion.

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Homework Statement


Show ##DF/Dt=0##. ##F = x-a-e^b\sin(a+t)## and ##a## is given implicitly as ##y=b-e^b\cos(a+t)## where ##a=f(y,t)## and ##b## is a constant. Also, velocity is $$u=e^b\cos(a+t)\\v=e^b\sin(a+t)$$

Homework Equations


##DF/Dt=F_t+v\cdot\nabla F##

The Attempt at a Solution


##F_t = -e^b\cos(a+t)##
##v\cdot \nabla F = e^b\cos(a+t) \cdot 1 + e^b\sin(a+t) \cdot 0 = e^b\cos(a+t)##.
Then ##DF/Dt = -e^b\cos(a+t)+e^b\cos(a+t)=0##. Is this correct? It feels too easy.

Thanks!
 
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What happened to Da/Dt?
 
So you're saying ##F_t=a'(t)-e^b\cos (a+t)\cdot (a'(t)+1)##. But then the convective term would also have the ##y## component, namely ##v\cdot (a'(y)-e^b\cos (a+t)\cdot a'(y)##?

Also, ##x## velocity is given by ##u=e^b\cos(a+t)##. Then ##a## was not differentiated for ##u=x'(t)##.

Sorry if this looks weird, I'm using the app for the first time and I can't see Tex output.
 
Last edited by a moderator:
Orodruin, do you still think I should differentiate ##a## since they did not for the velocity term?
 
You make it sound as if the velocity was not given on the form you have quoted. My understanding of what you posted is that you were given the velocity.
 
Orodruin said:
You make it sound as if the velocity was not given on the form you have quoted. My understanding of what you posted is that you were given the velocity.
I apologize for the ambiguity. So the particle's position is given by: $$x=a+e^b\sin(a+t)\\y=b-e^b\cos(a+t)$$ Then the velocity as in the first post, which is given in the question stem. Does this clarify my question?
Thanks for your patience!
 
Could you quote the problem statement verbatim?
 
Orodruin said:
Could you quote the problem statement verbatim?
Definitely. It follows:
A particle's flow path is described as
$$x=a+e^b\sin(a+t)\\y=b-e^b\cos(a+t)$$
Thus the spatial velocity is
$$u=e^b\cos(a+t)\\v=e^b\sin(a+t)$$ Show that the kinematic boundary condition is satisfied along the curve derived from above by setting ##b=const## and ##a## is a parameter.
Hint: One could consider this curve to be $$x-a(y,t)-e^b\sin(a(y,t)+t)=0$$.

The kinematic boundary condition is ##DF/Dt=0## where ##F## is a curve of the boundary, presumably the hint's curve.
 
But ##u=\partial_tx##, and they did not implicitly differentiate ##a##, but treated it as a constant. If this is true for the time derivative, since ##a## is a functino of ##t## and ##y##, then ##D a/D t = 0##. Do you agree?
 

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