Emmons problem explained

In combustion, Emmons problem describes the flame structure which develops inside the boundary layer, created by a flowing oxidizer stream on flat fuel (solid or liquid) surfaces. The problem was first studied by Howard Wilson Emmons in 1956.[1] [2] [3] The flame is of diffusion flame type because it separates fuel and oxygen by a flame sheet. The corresponding problem in a quiescent oxidizer environment is known as Clarke–Riley diffusion flame.

Burning rate

Source:[4]

Consider a semi-infinite fuel surface with leading edge located at

x=0

and let the free stream oxidizer velocity be

Uinfty

. Through the solution

f(η)

of Blasius equation

f'''+ff''=0

(

η

is the self-similar Howarth–Dorodnitsyn coordinate), the mass flux

\rhov

(

\rho

is density and

v

is vertical velocity) in the vertical direction can be obtained

\rhov=\rhoinfty\muinfty\sqrt{

2\xi
Uinfty
} \left(f'\rho \int_0^\eta \rho^ \ d\eta - f\right),

where

\xi=

x
\int
0

\rhoinfty\muinftydx.

In deriving this, it is assumed that the density

\rho\sim1/T

and the viscosity

\mu\simT

, where

T

is the temperature. The subscript

infty

describes the values far away from the fuel surface. The main interest in combustion process is the fuel burning rate, which is obtained by evaluating

\rhov

at

η=0

, as given below,

\rhoovo=\rhoinfty\muinfty\left[

2Uinfty
2
\mu
infty
x
\int
0

\rhoinfty\muinftydx\right]-1/2[-f(0)].

See also

Notes and References

  1. Emmons, H. W. (1956). The film combustion of liquid fuel. ZAMM‐Journal of Applied Mathematics and Mechanics/Zeitschrift für Angewandte Mathematik und Mechanik, 36(1‐2), 60-71.
  2. Clarke, J. F. (1969). Emmons' problem according to the Oseen approximation. The Physics of Fluids, 12(1), 241-243.
  3. Baum, H. R., & Atreya, A. (2015). The Elliptic Emmons Problem. In ICHMT DIGITAL LIBRARY ONLINE. Begel House Inc.
  4. Williams, F. A. (2018). Combustion theory. CRC Press.