The effects of inertia on the elastic instabilities in Dean and Taylor–Couette flows are investigated through a linear stability analysis. The critical conditions and the structure of the vortex flow at the onset of these instabilities are presented. The results reveal that the purely elastic Dean flow is destabilized by inertial effects. It is also found that inertia destabilizes elastic Taylor–Couette flow if the rotation of the inner cylinder is the flow driving force, while it stabilizes the flow driven by rotation of the outer cylinder. The mechanism of destabilization or stabilization of these viscoelastic instabilities is investigated through an examination of the disturbance‐energy equation. It is shown that Dean flow is destabilized by two separate mechanisms: a purely elastic mechanism discussed previously (i.e., energy production due to the coupling of a perturbation velocity to the polymeric stress gradient in the base state) [see Phys. Fluids A 3, 1691 (1991)] and a purely inertial mechanism discussed by Dean [Proc. R. Soc. London Ser. A 121, 402 (1928)] (i.e., energy production from Reynolds stresses). It is also shown that, when rotation of the inner cylinder drives Taylor–Couette flow, the Reynolds stresses produce energy, and thus are destablizing, while for the flow driven by the rotation of the outer cylinder alone, the Reynolds stresses dissipate energy, thus stabilizing the flow. The elastic forces remain destabilizing in both modes of operation. In a second study, a pressure‐driven viscoelastic coating flow over a curved surface is examined. The results demonstrate the existence of a purely elastic stationary instability in the coating flow on a concave wall which is very similar to that which occurs in viscoelastic Dean flow. It is demonstrated that the mechanisms of instability in Dean flow and the coating flow are the same, again through an examination of the disturbance‐energy equation.

1.
G. I.
Taylor
, “
Stability of a viscous liquid contained between two rotating cylinders
,”
Philos. Trans. R. Soc. London Ser. A
223
,
289
(
1923
).
2.
W. R.
Dean
, “
Fluid motion in a curved channel
,”
Proc. R. Soc. London Ser. A
121
,
402
(
1928
).
3.
R. G.
Larson
,
E. S. G.
Shaqfeh
, and
S. J.
Muller
, “
A purely elastic instability in Taylor-Couette flow
,”
J. Fluid Mech.
218
,
573
(
1990
).
4.
Y. L.
Joo
and
E. S. G.
Shaqfeh
, “
Viscoelastic Poiseuille flow through a curved channel: A new elastic instability
,”
Phys. Fluids A
3
,
1691
(
1991
).
5.
Y. L.
Joo
and
E. S. G.
Shaqfeh
, “
A purely elastic instability in Dean and Taylor-Dean flow
,”
Phys. Fluids A
4
,
524
(
1992
).
6.
N.
Phan-Thien
, “
Coaxial-disk flow of an Oldroyd-B fluid: exact solution and stability
,”
J. Non-Newtonian Fluid Mech.
13
,
325
(
1983
).
7.
N.
Phan-Thien
, “
Cone-and-plate flow of an Oldroyd-B fluid is unstable
,”
J. Non-Newtonian Fluid Mech.
17
,
37
(
1985
).
8.
S. K.
Datta
, “
Note on the stability of an elasticoviscous liquid in Cou-ette flow
,”
Phys. Fluids
7
,
1915
(
1964
).
9.
R. H.
Thomas
and
K.
Walters
, “
The stability of elastico-viscous flow between rotating cylinders. Part 1
,”
J. Fluid Mech.
18
,
33
(
1964
).
10.
H.
Rubin
and
C.
Elata
, “
Stability of Couette flow of dilute polymer solutions
,”
Phys. Fluids
9
,
1929
(
1966
).
11.
R. F.
Ginn
and
M. M.
Denn
, “
Rotational stability in viscoelastic liquids
,”
AIChE J.
15
,
450
(
1969
).
12.
M. M.
Denn
and
J. J.
Roisman
, “
Rotational stability and measurement of normal stress functions in dilute polymer solutions
,”
AIChE J.
15
,
454
(
1969
).
13.
Z.-S.
Sun
and
M. M.
Denn
, “
Stability of rotational Couette flow of polymer solutions
,”
AIChE J.
18
,
1010
(
1972
).
14.
D. W.
Beard
,
M. H.
Davies
, and
K.
Walters
, “
The stability of elastico-viscous flow between rotating cylinders. Part 3
,”
J. Fluid Mech.
24
,
321
(
1966
).
15.
M. Avgousti and A. N. Beris, submitted to J. Fluid Mech.
16.
R. B. Bird, C. F. Curtiss, R. C. Armstrong, and O. Hassager, Dynamics of Polymeric Liquids, 2nd ed. (Wiley-Interscience, New York, 1987), Vol. 2.
17.
D. V.
Boger
, “
A highly elastic constant-viscosity fluid
,”
J. Non-Newtonian Fluid Mech.
3
,
87
(
1977/1978
).
18.
R. K.
Gupta
,
T.
Sridhar
, and
M. E.
Ryan
, “
Model viscoelastic liquids
,”
J. Non-Newtonian Fluid Mech.
12
,
233
(
1983
).
19.
M. E.
Mackay
and
D. V.
Boger
, “
An explanation of the rheological properties of Boger fluids
,”
J. Non-Newtonian Fluid Mech.
22
,
235
(
1987
).
20.
L. M.
Quinzani
,
G. H.
Mckinley
,
R. A.
Brown
, and
R. C.
Armstrong
, “
Modeling the rheology of polyisobutylene solutions
,”
J. Rheol.
34
,
705
(
1991
).
21.
Y. L. Joo, “A viscoelastic instability in Taylor-Dean flow,” Ph.D. thesis, Stanford University, in preparation.
22.
S. Chandrasekar, Hydrodynamic stability (Clarendon, Oxford, 1961).
23.
S. D.
Conte
, “
The numerical solutions of linear boundary value problems
,”
SIAM Rev.
8
,
309
(
1966
).
24.
H. B. Keller, Numerical Methods for Two-Point Boundary-Value Problems (Cinn-Blaisdell, Walfham, MA, 1961).
25.
E. S. G.
Shaqfeh
,
S. J.
Muller
, and
R. G.
Larson
, “
The effects of gap width and dilute solution properties on the viscoelastic Taylor-Couette instability
,”
J. Fluid Mech.
235
, (
1992
).
26.
P. J. Northey, R. C. Armstrong, and R. A. Brown, “Numerical calculation of time-dependent, two-dimensional inertial flows described by a multimode UCM model,” Annual AIChE Meeting, Paper No. 166Adb, November, 1989.
27.
P. J. Northey, R. C. Armstrong, and R. A. Brown, “Finite-element calculation of purely elastic, nonlinear transitions in circular Couette flow,” Annual AIChE Meeting, Paper No. 167j, November, 1990.
28.
S. P.
Lin
, “
Instability of a liquid film flowing down an inclined plane
,”
Phys. Fluids
10
,
308
(
1967
).
29.
R. W.
Chin
,
F. H.
Abernathy
, and
J. R.
Bertschy
, “
Gravity and shear wave stability of free surface flows. Part 1. Numerical calculations
,”
J. Fluid Mech.
168
,
501
(
1986
).
This content is only available via PDF.
You do not currently have access to this content.