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Unsteady Flows of a Maxwell Viscoelastic Fluid near a Critical Point with a Countercurrent at the Initial Moment. / Moshkin, N. P.
In: Journal of Applied and Industrial Mathematics, Vol. 16, No. 1, 02.2022, p. 105-115.Research output: Contribution to journal › Article › peer-review
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TY - JOUR
T1 - Unsteady Flows of a Maxwell Viscoelastic Fluid near a Critical Point with a Countercurrent at the Initial Moment
AU - Moshkin, N. P.
N1 - Funding Information: This work was supported by the Russian Foundation for Basic Research, project no. 19-01-00096. Publisher Copyright: © 2022, Pleiades Publishing, Ltd.
PY - 2022/2
Y1 - 2022/2
N2 - Two-dimensional unsteady stagnation-point flow of a viscoelastic fluid is studied assumingthat it obeys the upper-convected Maxwell (UCM) model. The solutions of constitutive equationsare found under the assumption that the components of the extra stress tensor are polynomials inthe spatial variable along a rigid wall. The class of solutions for unsteady flows in aneighbourhood of the front or rear stagnation point on a plane boundary is considered, and therange of possible behaviors is revealed depending on the initial stage (initial data) and on whetherthe pressure gradient is an accelerating or decelerating function of time. The velocity and stresstensor component profiles are obtained by numerical integration of the system of nonlinearordinary differential equations. The solutions of the equations exhibit finite-time singularitiesdepending on the initial data and the type of dependence of pressure gradient on time.
AB - Two-dimensional unsteady stagnation-point flow of a viscoelastic fluid is studied assumingthat it obeys the upper-convected Maxwell (UCM) model. The solutions of constitutive equationsare found under the assumption that the components of the extra stress tensor are polynomials inthe spatial variable along a rigid wall. The class of solutions for unsteady flows in aneighbourhood of the front or rear stagnation point on a plane boundary is considered, and therange of possible behaviors is revealed depending on the initial stage (initial data) and on whetherthe pressure gradient is an accelerating or decelerating function of time. The velocity and stresstensor component profiles are obtained by numerical integration of the system of nonlinearordinary differential equations. The solutions of the equations exhibit finite-time singularitiesdepending on the initial data and the type of dependence of pressure gradient on time.
KW - blow-up solution
KW - Maxwell viscoelastic medium
KW - Riccati equation
KW - unsteady critical-point flow
KW - upper convective derivative
UR - http://www.scopus.com/inward/record.url?scp=85134224318&partnerID=8YFLogxK
UR - https://www.mendeley.com/catalogue/266650b8-9ae6-3f11-a618-409d89c33312/
U2 - 10.1134/S1990478922010100
DO - 10.1134/S1990478922010100
M3 - Article
AN - SCOPUS:85134224318
VL - 16
SP - 105
EP - 115
JO - Journal of Applied and Industrial Mathematics
JF - Journal of Applied and Industrial Mathematics
SN - 1990-4789
IS - 1
ER -
ID: 36770798