20.05.2015 Views

DAMAGE PREDICTION OF BALL JOINTS IN ANTI-ROLL BARS

DAMAGE PREDICTION OF BALL JOINTS IN ANTI-ROLL BARS

DAMAGE PREDICTION OF BALL JOINTS IN ANTI-ROLL BARS

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

72<br />

STATIC MIXER<br />

Mixing is a common unit operation in a large number of processes, and it is used<br />

in many different applications where a defined degree of homogeneity of a fluid is<br />

desired. Common mixing devices are dynamic mixers for agitated tanks in batch<br />

operations and static mixers for inline mixing in continuous operations.<br />

Static mixers have been utilized over a wide range of applications such as<br />

continuous mixing, blending, heat transfer processes, chemical reactions, etc. A static<br />

mixer consists of a contacting device with a series of internal stationary mixing<br />

elements of specific and patented geometry, inserted in a pipe. Some of the advantages<br />

of static mixers over dynamic mixers are that they have no moving parts, low<br />

maintenance, low space requirements, no moving parts and a short residence time.<br />

D.1 Theory<br />

D.1.1 Governing Equations.<br />

For steady incompressible flow, the mass conservation equation can be written<br />

as<br />

∂ui<br />

= 0<br />

Eq.D-1<br />

∂xi<br />

and the momentum conservation equation can be written as<br />

∂( uiu<br />

j<br />

) ∂p<br />

∂τ<br />

ij<br />

ρ + = + ρg<br />

i<br />

+ Fi<br />

Eq.D-2<br />

∂x<br />

∂x<br />

∂x<br />

j<br />

i<br />

In the absence of a gravitational body force and any external body force, the two last<br />

terms on the right side of Eq.D-2 are zero. The stress tensor, τ ij , in Eq.D-2 is given by<br />

⎛ u u<br />

j<br />

⎞<br />

i<br />

uk<br />

τ<br />

ij<br />

µ ⎜<br />

∂ ∂<br />

⎟<br />

2 ∂<br />

= + − µ δ<br />

ij<br />

Eq.D-3<br />

x<br />

j<br />

x<br />

⎝ ∂ ∂<br />

i ⎠ 3 ∂xk<br />

Considering the conservation of mass for incompressible flow, ∂u k /∂x k =0, gives<br />

⎛ ⎞<br />

⎜<br />

∂u<br />

∂u<br />

i j<br />

τ + ⎟<br />

ij=<br />

µ<br />

Eq.D-4<br />

⎝ ∂x<br />

j<br />

∂xi<br />

⎠<br />

D.1.2 Pressure drop and Z factor<br />

The pressure drop over the static mixer was computed for the repeating unit of<br />

two mixer elements, and converted to a pressure per meter. The pressure drop for<br />

empty tube, ∆P et , under laminar flow conditions is calculated as<br />

∆l<br />

vx<br />

µ<br />

∆ Pet<br />

= 32<br />

Eq.D-5<br />

2<br />

D<br />

When considering the pressure drop for the static mixer, ∆P sm , a common<br />

approach is to define a dimensionless number comparing the pressure drop over a<br />

static mixer with that over an empty pipe of the same length as the static mixer. The<br />

dimensionless number, referred to as the Z factor, is essentially the increase in energy<br />

input required when the static mixer is installed in the pipe. The Z factor is<br />

Psm<br />

Z & ∆<br />

= Z(Re)<br />

=<br />

∆P<br />

Eq.D-6<br />

At Re ≤ 10, the correlation of Wilkinson and Cliff given by<br />

j<br />

et

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!