written 5.6 years ago by | • modified 4.5 years ago |
State assumptions made at each stage. Plot the dimensionless velocity profile for different value of $\frac{dp}{dx}$.
written 5.6 years ago by | • modified 4.5 years ago |
State assumptions made at each stage. Plot the dimensionless velocity profile for different value of $\frac{dp}{dx}$.
written 5.6 years ago by |
Coutte flow:
Navier-stokes equation in x-direction
$u\frac{du}{dx}+v\frac{du}{dy}+w\frac{du}{dz}+\frac{du}{dt}=F_x-\frac{1}{S}\frac{\partial P}{\partial x}+\frac{u}{S}[\frac{\partial ^2u}{\partial x^2}+\frac{\partial ^2u}{\partial y^2}+\frac{\partial ^2u}{\partial z^2}]$...........(1)
Assumptions:
i) Fluid is incompressible (S=constant)
ii) Flow is one dimensional (x-direction)
$\therefore u\ne 0, v=0,w=0$
iii) Flow is steady $\therefore \frac{\partial u}{\partial t}=0$
iv) The flow is independent of any variation in z-diection
v) The body forces per unit mass are zero. $\therefore F_x=F_y=F_x=0$
$\therefore$ From continuity equation
$\frac{\partial u}{\partial x}=\frac{\partial v}{\partial y}+\frac{\partial w}{\partial z}=0$
$\therefore \frac{\partial u}{\partial x}=0$
$\therefore u=f(y)$
Considering above all assumptions equation (1) becomes
$0=-\frac{1}{S}\frac{\partial P}{\partial x}+\frac{u}{S}\frac{\partial ^2u}{\partial y^2}$
$\therefore \frac{\partial ^2u}{\partial y^2}=\frac{1}{u}\frac{\partial P}{\partial x}$
Integrating,
$\frac{\partial u}{\partial y}=\frac{1}{u}\frac{\partial P}{\partial x}\cdot y+c_1$
Again integrating,
$u=\frac{1}{2u}\frac{\partial P}{\partial x}y^2+c_1\cdot y+c_2$............(2)
where $c_1$ & $c_2$ are constants of integration.
Boundary conditions are
i) at y=0,u=0 $\therefore c_2=0$
ii) at y=b,u=U...........Velocity of moving plate
Using boundary conditions
$U=\frac{1}{2u}\cdot \frac{\partial P}{\partial x}b^2 + c_1\cdot b$
$\therefore c_1=\frac{U-\frac{1}{2u}\cdot \frac{\partial P}{\partial x}\cdot b^2}{b}$
$c_1=\frac{U}{b}-\frac{1}{2u}\cdot \frac{\partial P}{\partial x}\cdot b$
Putting $c_1$ and $c_2$ in equation (2)
$U=\frac{1}{2u}\cdot \frac{\partial P}{\partial x}y^2+[\frac{U}{b}-\frac{1}{2u}\cdot \frac{\partial P}{\partial x}\cdot b]y+0$
$u=\frac{U}{b}\cdot y+\frac{1}{2u}(-\frac{\partial P}{\partial x})(by-y^2)$..........Equation for velocity profile in coutte flow
Velocity profile for different $\frac{\partial P}{\partial x}$