Paper 2, Section II, C

Fluid Dynamics II | Part II, 2018

An initially unperturbed two-dimensional inviscid jet in h<y<h-h<y<h has uniform speed UU in the xx direction, while the surrounding fluid is stationary. The unperturbed velocity field u=(u,v)\mathbf{u}=(u, v) is therefore given by

u=0 in y>hu=U in h<y<hu=0 in y<h\begin{array}{ll} u=0 & \text { in } \quad y>h \\ u=U & \text { in } \quad-h<y<h \\ u=0 & \text { in } \quad y<-h \end{array}

Consider separately disturbances in which the layer occupies hη<y<h+η(-h-\eta<y<h+\eta( varicose disturbances) and disturbances in which the layer occupies h+η<y<h+η(-h+\eta<y<h+\eta( sinuous disturbances )), where η(x,t)=η^eikx+σt\eta(x, t)=\hat{\eta} e^{i k x+\sigma t}, and determine the dispersion relation σ(k)\sigma(k) in each case.

Find asymptotic expressions for the real part σR\sigma_{R} of σ\sigma in the limits k0k \rightarrow 0 and kk \rightarrow \infty and draw sketches of σR(k)\sigma_{R}(k) in each case.

Compare the rates of growth of the two types of disturbance.

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