Bhoraniya, RameshRameshBhoraniyaNarayanan, VinodVinodNarayanan2025-08-312025-08-312019-11-0110.1134/S00154628190600282-s2.0-85077068650https://d8.irins.org/handle/IITG2025/24366The paper presents a global stability analysis of the two-dimensional incompressible boundary layer with the effect of streamwise pressure gradient. A symmetric wedge flow is considered at different values of the dimensionless pressure gradient parameter β<inf>H</inf>. The pressure gradient dp/dx in the flow direction is zero, when β<inf>H</inf> = 0, favorable (negative) for β<inf>H</inf> > 0, and adverse (positive) for β<inf>H</inf> < 0. The base flow is computed by numerical solution of Falkner—Skan equation. The Reynolds number is based on the displacement thickness δ* at the inflow boundary. The stability equations governing the flow are derived in body-fitted coordinates. The stability equations are discretized using the Chebyshev spectral collocation method. The discretized equations, together with boundary conditions, form a general eigenvalue problem and are solved using Arnoldi’s algorithm. The temporal global modes are computed for β<inf>H</inf> = 0.022, 0.044, and 0.066, for favorable and adverse pressure gradients. The temporal growth rate ω<inf>i</inf> is found to be negative for all the global modes. The ω<inf>i</inf> value is smaller for the favorable pressure gradient (FPG) than for the adverse pressure gradient (APG) at the same Reynolds number (Re = 340). Thus, the FPG has a stabilizing effect on the boundary layer. The comparison of the spatial eigenmodes and spatial amplification rates for FPG and APG show that FPG has a stabilizing effect, whereas APG has a destabilizing effect on the disturbances.falseboundary layer | global stability | incompressible fluid | numerical solutions | streamwise pressure gradientArticle15738507821-8341 November 20198arJournal8WOS:000511668700008