The Euler Equation and Incompressible Fluid Theorems

[aclaret]

Homework Statement

Let $u: R^3 \times R \rightarrow R^3$ be flow velocity of incompressible fluid. Let fluid be subject to potential force $-\nabla \chi$. To prove
$$\frac{d}{dt} \int_{V} \frac{1}{2} \rho \langle u, u \rangle dV + \int_{\partial V} H \langle u, n \rangle dA = 0$$where $H := \frac{1}{2}\rho \langle u, u \rangle + p + \chi$, and notation $\langle x, y \rangle$ denote standard inner product on $R^3$.

Relevant Equations

fluid dynamic, euler's equation of the motion

$$\frac{Du}{Dt} = -\frac{\nabla p}{\rho} - \nabla \chi$$I re-write the Euler equation for incompressible fluid using suffix notation
$$\frac{\partial u_i}{\partial t} + u_j \frac{\partial u_i}{\partial x_j} + \frac{\partial}{\partial x_i} \left(\frac{p}{\rho} + \chi \right) = 0$$what theorems applies to the problem?

 

[pasmith]

You have integrals involving a volume and a surface. That would suggest the divergence theorem.

 

[aclaret]

divergence theorem I can write$$\int_{\partial V} \langle u, n \rangle dA = \int_V \frac{\partial u_j}{\partial x_j} dV$$try multiply equation by $u_i$ and then do implicit summation also over $i$

$$u_i \frac{\partial u_i}{\partial t} + u_i u_j \frac{\partial u_i}{\partial x_j} + u_i \frac{\partial}{\partial x_i} \left(\frac{p}{\rho} + \chi \right) = 0$$get for second term$$u_i u_j \frac{\partial u_i}{\partial x_j} = \frac{1}{2}u_j \frac{\partial}{\partial x_j} \langle u, u \rangle$$first term also

$$u_i \frac{\partial u_i}{\partial t} = \frac{1}{2} \frac{\partial}{\partial t} \langle u,u \rangle$$do I effect the volume integral to both sides?

$$\int_V \frac{1}{2} \frac{\partial}{\partial t} \langle u,u \rangle dV + \int_V \frac{1}{2}u_j \frac{\partial}{\partial x_j} \langle u, u \rangle dV + \int_V u_i \frac{\partial}{\partial x_i} \left(\frac{p}{\rho} + \chi \right) dV = 0$$can I make use of divergence theorem here?

 

[aclaret]

$$\frac{d}{dt} \int_V \frac{1}{2} \rho \langle u,u \rangle dV + \int_V u_i \frac{\partial}{\partial x_i} \left[ \frac{1}{2} \rho \langle u, u \rangle + \left(p + \rho \chi \right) \right] dV = K, \quad K \, \mathrm{= constant}$$I can try integrate second term by parts,$$\int_V u_i \frac{\partial}{\partial x_i} \left[ \frac{1}{2} \rho \langle u, u \rangle + \left(p + \rho \chi \right) \right] dV = \int_{\partial V} \left[ \frac{1}{2} \rho \langle u, u \rangle + \left(p + \rho \chi \right) \right] \langle u, n \rangle dA - \int_{V} \left[ \frac{1}{2} \rho \langle u, u \rangle + \left(p + \rho \chi \right) \right] \frac{\partial u_i}{\partial x_i} dV$$does second term vanish? even if, the first term still incorrect. I wonder if you can tell second hint @pasmith :), I'm in a little confusion ;)

 

[pasmith]

What is the divergence of an incompressible fluid?

 

[aclaret]

let me see... clearly from equation of continuity it follow that if $(\forall x,t) \, \rho(x,t) = \text{constant}$, then $\nabla \cdot u = 0$. hence, second integral vanish, and get$$\frac{d}{dt} \int_V \frac{1}{2} \rho \langle u,u \rangle dV + \int_{\partial V} \left[ \frac{1}{2} \rho \langle u, u \rangle + \left(p + \rho \chi \right) \right] \langle u, n \rangle dA = K, \quad K \, \mathrm{= constant}$$but this would give me $H := \frac{1}{2} \rho \langle u, u \rangle + p + \rho \chi$, which tiny bit different to problem statement. would you agree my work is correct, or did I do a mistake somewhere...

 

[pasmith]

The problem statement says that the fluid is subject ot a potential force of -\nabla\chi, not -\rho\nabla\chi. Other than that your work is correct.

The constant K is zero; it were not there would be some point where <br /> \rho \frac{Du}{Dt} + \nabla p + \nabla \chi \neq 0.

 

[aclaret]

parfait! yes I see, thank for point out my mistake with the factor of $\rho$. I also was not certain how to "convince myself" that $K$ indeed vanish.

i think necessary for me do lot more of these problem to learn the tricks of the trade :), the simple realize that $\nabla \cdot u = 0$ was enough here to reveal how to finish the solution!

thank for your assistance :)