Internal flow modeling is a requisite for obtaining critical parameters in the design and fabrication of modern solid rocket motors. In this work, the analytical formulation of internal flows particular to motors with tapered sidewalls is pursued. The analysis employs the vorticity-streamfunction approach to treat this problem assuming steady, incompressible, inviscid, and nonreactive flow conditions. The resulting solution is rotational following the analyses presented by Culick for a cylindrical motor. In an extension to Culick’s work, Clayton has recently managed to incorporate the effect of tapered walls. Here, an approach similar to that of Clayton is applied to a slab motor in which the chamber is modeled as a rectangular channel with tapered sidewalls. The solutions are shown to be reducible, at leading order, to Taylor’s inviscid profile in a porous channel. The analysis also captures the generation of vorticity at the surface of the propellant and its transport along the streamlines. It is from the axial pressure gradient that the proper form of the vorticity is ascertained. Regular perturbations are then used to solve the vorticity equation that prescribes the mean flow motion. Subsequently, numerical simulations via a finite volume solver are carried out to gain further confidence in the analytical approximations. In illustrating the effects of the taper on flow conditions, comparisons of total pressure and velocity profiles in tapered and nontapered chambers are entertained. Finally, a comparison with the axisymmetric flow analog is presented.

1.
F. E. C.
Culick
, “
Rotational axisymmetric mean flow and damping of acoustic waves in a solid propellant rocket
,”
AIAA J.
4
,
1462
(
1966
).
2.
J.
Majdalani
,
G. A.
Flandro
, and
S. R.
Fischbach
, “
Some rotational corrections to the acoustic energy equation in injection-driven enclosures
,”
Phys. Fluids
17
,
074102
(
2005
).
3.
G. A.
Flandro
,
J.
Majdalani
, and
J. C.
French
, “
Incorporation of nonlinear capabilities in the standard stability prediction program
,” AIAA Paper No. 2004–4182, Fort Lauderdale, FL,
2004
.
4.
J.
Majdalani
and
W. K.
Van Moorhem
, “
Improved time-dependent flowfield solution for solid rocket motors
,”
AIAA J.
36
,
241
(
1998
).
5.
J.
Majdalani
and
W. K.
Van Moorhem
, “
Laminar cold-flow model for the internal gas dynamics of a slab rocket motor
,”
Aerosp. Sci. Technol.
5
,
193
(
2001
).
6.
J.
Majdalani
, “
Physicality of core flow models in rocket motors
,”
J. Propul. Power
19
,
156
(
2003
).
7.
J.
Majdalani
and
G. A.
Flandro
, “
The oscillatory pipe flow with arbitrary wall injection
,”
Proc. R. Soc. London, Ser. A
458
,
1621
(
2002
).
8.
J.
Majdalani
and
W. K.
Van Moorhem
, “
The unsteady boundary layer in solid rocket motors
,” AIAA Paper No. 95–2731, San Diego, CA,
1995
.
9.
D. E.
Coats
and
S. S.
Dunn
, “
Improved motor stability predictions for 3D grains using the SPP code
,” AIAA Paper No. 97–33251, Seattle, WA,
1997
.
10.
C. D.
Clayton
, “
Flowfields in solid rocket motors with tapered bores
,” AIAA Paper No. 96–2643,
1996
.
11.
G. I.
Taylor
, “
Fluid flow in regions bounded by porous surfaces
,”
Proc. R. Soc. London, Ser. A
234
,
456
(
1956
).
12.
S. W.
Yuan
and
A. B.
Finkelstein
, “
Laminar pipe flow with injection and suction through a porous wall
,”
J. Appl. Mech.
78
,
719
(
1956
).
13.
S. W.
Yuan
and
A. B.
Finkelstein
, “
Heat transfer in laminar pipe flow with uniform coolant injection
,”
Jet Propul.
28
,
178
(
1958
).
14.
R. M.
Terrill
and
G. M.
Shrestha
, “
Laminar flow through channels with porous walls and with an applied transverse magnetic field
,”
Appl. Sci. Res., Sect. A
11
,
134
(
1965
).
15.
J.
Majdalani
,
A. B.
Vyas
, and
G. A.
Flandro
, “
Higher mean-flow approximation for a solid rocket motor with radially regressing walls
,”
AIAA J.
40
,
1780
(
2002
).
16.
C.
Zhou
and
J.
Majdalani
, “
Improved mean flow solution for slab rocket motors with regressing walls
,”
J. Propul. Power
18
,
703
(
2002
).
17.
T.
Mu-Kuan
and
L.
Tong-Miin
, “
Fiber optic LDV study of the non-uniform, injection induced flow in a 2-D, divergent, porous-walled channel
,”
J. Chin. Soc. Mech. Eng.
11
,
414
(
1990
).
18.
O. C.
Sams
,
J.
Majdalani
, and
G. A.
Flandro
, “
Higher flowfield approximations for solid rocket motors with tapered bores
,” AIAA Paper No. 2004–4051, Fort Lauderdale, FL,
2004
.
19.
R. S.
Brown
,
A. M.
Blackner
,
P. G.
Willoughby
, and
R.
Dunlap
, “
Coupling between acoustic velocity oscillations and solid propellant combustion
,”
J. Propul. Power
2
,
428
(
1986
).
20.
R. S.
Brown
,
J. E.
Erickson
, and
W. R.
Babcock
, “
Measuring the combustion response of a forced oscillation method
,”
AIAA J.
12
,
1502
(
1974
).
21.
R.
Dunlap
,
A. M.
Blackner
,
R. C.
Waugh
,
R. S.
Brown
, and
P. G.
Willoughby
, “
Internal flow field studies in a simulated cylindrical port rocket chamber
,”
J. Propul. Power
6
,
690
(
1990
).
22.
R.
Dunlap
,
P. G.
Willoughby
, and
R. W.
Hermsen
, “
Flowfield in the combustion chamber of a solid propellant rocket motor
,”
AIAA J.
12
,
1440
(
1974
).
23.
W.-W.
Chu
,
V.
Yang
, and
J.
Majdalani
, “
Premixed flame response to acoustic waves in a porous-walled chamber with surface mass injection
,”
Combust. Flame
133
,
359
(
2003
).
24.
A. B.
Vyas
,
J.
Majdalani
, and
V.
Yang
, “
Estimation of the laminar premixed flame temperature and velocity in injection-driven combustion chambers
,”
Combust. Flame
133
,
371
(
2003
).
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