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Sharp inequalities for the coefficients of concave schlicht functions on such functions f the second normalization f(1) = ∞. We call these functions concave schlicht functions
A problem of steady-state electrochemical shaping with a non-Schlicht velocity hodograph characteristic feature of this problem is a non-schlicht velocity hodograph. © 2010 Allerton Press, Inc.
Concave schlicht functions with bounded opening angle at infinityConcave schlicht functions with bounded opening angle at infinity
Numerical simulation of Schlichting streaming induced by standing wave in rectangular enclosure© Published under licence by IOP Publishing Ltd. Acoustic streaming of incompressible fluid induced
Numerical simulation of Schlichting streaming induced by standing wave in rectangular enclosure© Published under licence by IOP Publishing Ltd. Acoustic streaming of incompressible fluid induced
A problem of steady-state electrochemical shaping with a non-Schlicht velocity hodograph characteristic feature of this problem is a non-schlicht velocity hodograph. © 2010 Allerton Press, Inc.
Особенности акустического течения при изотермических граничных условиях в полостях разного диаметра that with a decrease in the vibration frequency at a fixed cavity diameter, the Schlichting streaming vortices
Sharp inequalities for the coefficients of concave schlicht functions on such functions f the second normalization f(1) = ∞. We call these functions concave schlicht functions
Related results in the introduction for the higher derivatives of schlicht functions. He proved the following theorem (compare Landau
Concave schlicht functions with bounded opening angle at infinityConcave schlicht functions with bounded opening angle at infinity
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