Acceleration of fluid particle

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The discussion focuses on finding the acceleration of a fluid particle in a given velocity field, specifically u = (y, t-x). The correct application of the material derivative Du/Dt involves calculating both the time derivative ∂u/∂t and the convective term (u⋅∇)u. Participants clarify that the operator (u⋅∇) must be applied correctly to both components of the velocity vector. Confusion arises regarding the application of partial derivatives and the non-commutative nature of the operators involved. Ultimately, the correct acceleration is derived as (t-x, 1-y), affirming the importance of understanding vector calculus in fluid dynamics.
sa1988
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Homework Statement



Find acceleration for a general point (x, y) at time t, in the velocity field u = (y, t-x)

Homework Equations



Du/Dt = ∂u/∂t + (u⋅∇)u

The Attempt at a Solution



u/∂t = (0, 1)

(u⋅∇)u = [(y, t-x)⋅(∂/∂x, ∂/∂y)](y, t-x)

= (0 + 0)(y, t-x) = (0, 0)

Thus Du/Dt = ∂u/∂t + (u⋅∇)u = (0, 1) + (0, 0)

= (0, 1)

It seems correct but my lecturer has given a different example, for a different problem, in which he draws out the entire process (presumably for the sake of letting students follow every tiny step) but I think there are typos in his work and it's really confusing things for me. So I've stuck with what I believe to be correct, but would like to run it by you guys to see if things are all ok.

Thanks!

For reference, my lecturer's example is here - http://www1.maths.leeds.ac.uk/~kersale/2620/Examples/sol1.pdf - The part on the final page.

It looks like he's written ∂/∂x in far too many places...?
 
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No, what your lecturer did is correct. Perhaps what you are missing is that \vec{u}\cdot\nabla, with \vec{u}= u\vec{i}+ v\vec{j} is equal to u\frac{\partial }{\partial x}+ v\frac{\partial}{\partial y} and that, being a scalar operator "multiplied" by \vec{u}= u\vec{I}+ v\vec{j} is "multiplied" by both u and v: (\vec{u}\cdot\nabla)\vec{u}= \left(\vec{u}\cdot\nabla(u\vec{i}+ v\vec{j})\right)+ \left(\vec{v}\cdot\nabla(u\vec{i}+ v\vec{j})\right)
= \left(u\frac{\partial u}{\partial x}+ u\frac{\partial u}{\partial y}\right)+ \left(v\frac{\partial u}{\partial x}+ v\frac{\partial u}{\partial y}\right)+ \left(u\frac{\partial v}{\partial x}+ u\frac{\partial v}{\partial y}\right)+ \left(v\frac{\partial v}{\partial x}+ v\frac{\partial v}{\partial y}\right).
 
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HallsofIvy said:
No, what your lecturer did is correct. Perhaps what you are missing is that \vec{u}\cdot\nabla, with \vec{u}= u\vec{i}+ v\vec{j} is equal to u\frac{\partial }{\partial x}+ v\frac{\partial}{\partial y} and that, being a scalar operator "multiplied" by \vec{u}= u\vec{I}+ v\vec{j} is "multiplied" by both u and v: (\vec{u}\cdot\nabla)\vec{u}= \left(\vec{u}\cdot\nabla(u\vec{i}+ v\vec{j})\right)+ \left(\vec{v}\cdot\nabla(u\vec{i}+ v\vec{j})\right)
= \left(u\frac{\partial u}{\partial x}+ u\frac{\partial u}{\partial y}\right)+ \left(v\frac{\partial u}{\partial x}+ v\frac{\partial u}{\partial y}\right)+ \left(u\frac{\partial v}{\partial x}+ u\frac{\partial v}{\partial y}\right)+ \left(v\frac{\partial v}{\partial x}+ v\frac{\partial v}{\partial y}\right).

Thanks for the reply.

I'm a little confused though. I can't see how you get this bit:

(\vec{u}\cdot\nabla)\vec{u}= \left(\vec{u}\cdot\nabla(u\vec{i}+ v\vec{j})\right)+ \left(\vec{v}\cdot\nabla(u\vec{i}+ v\vec{j})\right)And, regarding the the final result:

= \left(u\frac{\partial u}{\partial x}+ u\frac{\partial u}{\partial y}\right)+ \left(v\frac{\partial u}{\partial x}+ v\frac{\partial u}{\partial y}\right)+ \left(u\frac{\partial v}{\partial x}+ u\frac{\partial v}{\partial y}\right)+ \left(v\frac{\partial v}{\partial x}+ v\frac{\partial v}{\partial y}\right)

Is there a way of writing that in vector form?

One thing I did notice is that I messed up by forgetting that in (u⋅∇) , ∂/∂x is not commutative, so I was doing (∇⋅u)u, which is different.

So now I'm getting

(u⋅∇)u = (ux, uu)⋅(∂/∂x, ∂/∂y) (ux + uy)
= (ux∂/∂x + uy∂/∂y) (ux + uy)
= (ux∂(ux)/∂x + ux∂(uy)/∂x + uy∂(ux)/∂y + uy∂(uy)/∂y)

Which I then apply to the given velocity field u = (y, t-x), to get:

Du/Dt = ∂u/∂t + (u⋅∇)u

= (0, 1) + (y ∂/∂x + (t-x) ∂/∂y) * (y, t-x)
= (0, 1) + (y ∂(y)/∂x + (t-x)∂(y)/∂y, y ∂(t-x)/∂x + (t-x)∂(t-x)/∂y)
= (0, 1) + ( 0 + t-x , -y + 0)

= (t-x, 1-y)

Have I gone wrong here?

I've found this on wikipedia, which seems to reflect the same process I've just used:

538885b73da17a0e7211a97108354461.png


Thanks.
 
HallsofIvy said:
No, what your lecturer did is correct. Perhaps what you are missing is that \vec{u}\cdot\nabla, with \vec{u}= u\vec{i}+ v\vec{j} is equal to u\frac{\partial }{\partial x}+ v\frac{\partial}{\partial y} and that, being a scalar operator "multiplied" by \vec{u}= u\vec{I}+ v\vec{j} is "multiplied" by both u and v: (\vec{u}\cdot\nabla)\vec{u}= \left(\vec{u}\cdot\nabla(u\vec{i}+ v\vec{j})\right)+ \left(\vec{v}\cdot\nabla(u\vec{i}+ v\vec{j})\right)

Something's gone wrong here. If \mathbf{u} = (u,v) with respect to cartesian coordinates (x,y) then indeed \mathbf{u} \cdot \nabla = u \frac{\partial}{\partial x} + v \frac{\partial}{\partial y} but <br /> (\mathbf{u} \cdot \nabla)\mathbf{u} = \left( u \frac{\partial u}{\partial x} + v \frac{\partial u}{\partial y}, u \frac{\partial v}{\partial x} + v \frac{\partial v}{\partial y} \right) and hence <br /> \frac{D\mathbf{u}}{Dt} = \left(\frac{\partial u}{\partial t} + u \frac{\partial u}{\partial x} + v \frac{\partial u}{\partial y}, \frac{\partial v}{\partial t} + u \frac{\partial v}{\partial x} + v \frac{\partial v}{\partial y} \right).
 
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Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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