Ippolit S. Gromeka

Last updated

Ippolit Stepanovich Gromeka
Born(1851-01-27)27 January 1851
Died13 October 1889(1889-10-13) (aged 38)
Nationality Russian Empire
Alma mater Imperial Moscow University
Kazan University
Known for Beltrami flow
Gromeka–Arnold–Beltrami–Childress flow
Gromeka–Lamb equation
Scientific career
Institutions Kazan University
Thesis Some cases of the motion of an incompressible fluid (1881)
Notable students Aleksandr Kotelnikov

Ippolit Stepanovich Gromeka (or Hippolyte Stepanovich Gromeka) was a 19th century Russian scientist who made significant contributions to the science of fluid mechanics.

Contents

Biography

Ippolit was born on 27 January in 1851, in Berdychiv to Stepan Stepanovich Gromeka, a well-known publicist and a governor (1867–1875) of Siedlce and Yekaterina Fyodorovna Shcherbatska. [1] He grew up in Siedlce and also earned a gold medal in the Siedlce high school. He completed his Bachelors degree from the Imperial Moscow University in 1873 and worked as a teacher in the university for two years. He then worked as a teacher in Moscow High School until 1879, and in Belsk high school from 1879. In 1879, he also completed his Master's degree with a dissertation on capillary phenomena. [2] In 1880, he became an assistant professor at the Kazan University. In 1881, he obtained his PhD with a dissertation on Some cases of the motion of an incompressible fluid. He became a professor in 1882.

In the winter of 1888-1889, Gromeka fell from a sleigh during hunting with a severe bruise in his chest. Due to his injury, he died on 13 October 1889 in Kutaisi at the age of only 38. One of his brother, Mikhail Stepanovich Gromeka, was a well known literary critic, who died in 1883.

Research

During his short research career, just over than 10 years, Gromeka has produced many important contributions to the field of fluid mechanics through 11 works, starting from his Master's thesis on capillary phenomena and his last work in 1889 on the effect of temperature distribution on sound waves. [3] He provided an original and modern description of the capillarity phenomena, settling for the first time the discrepancy that was prevalent between Young's and Laplace's theories. He pioneered the studies on Beltrami flows in his PhD thesis in 1882 [4] and because of it, he is referred as the father of the helical flows. [1] He also studied unsteady flows in tubes, wave motion in elastic tubes and others. [5]

His scientific works were published in Russian in 1952. [6] A special issue in the journal Fluids in honour of Gromeka was produced in 2024. [7]

Published works

Gromeka's published works are [1]

  • Gromeka. I.S. Essay on the Theory of Capillary Phenomena. Theory of Surface Fluid Adhesion (Master’s Thesis). Mat. Sb. 1879, 9, 435–500. [2]
  • Gromeka. I.S. Some Cases of Incompressible Fluid Flow. Ph.D. Thesis, Kazan University, Kazan, Russia, 1882; pp. 1–107.
  • Gromeka. I.S. On the Theory of Fluid Motion in Narrow Cylindrical Tubes; Scientific notes of Kazan University; Kazan University: Kazan, Russia, 1882; pp. 1–32.
  • Gromeka. I.S. On the Velocity of Propagation of Wave-Like Motion of Fluids in Elastic Tubes; Scientific notes of Kazan University; Kazan University: Kazan, Russia, 1883; pp. 1–19.
  • Gromeka. I.S. On the Vortex Motions of a Liquid on a Sphere; Scientific Notes of Kazan University; Kazan University: Kazan, Russia, 1885; pp. 1–35.
  • Gromeka. I.S. On the motion of liquid drops. Bull. De La Société Mathématique De Kasan Kasan 1886, 5, 8–47.
  • Gromeka. I.S. Some cases of equilibrium of a perfect gas. Bull. De La Société Mathématique De Kasan Kasan 1886, 5, 66–82.
  • Gromeka. I.S. Lectures on the Mechanics of Liquid Bodies; Kazan University Press: Kazan, Russia, 1887; pp. 1–174.
  • Gromeka. I.S. On infinite values of integrals of second-order linear differential equations. Bull. De La Société Mathématique De Kasan Kasan 1887, 6, 14–40.
  • Gromeka. I.S. On the Effect of Temperature on Small Variations in Air Masses; Scientific Notes of Kazan University; Kazan University: Kazan, Russia, 1888; pp. 1–40.
  • Gromeka. I.S. Influence of the Uneven Distribution of the Temperature on the Propagation of Sound. Mat. Sb. 1889, 14, 283–302. [3]

Related Research Articles

<span class="mw-page-title-main">Aerodynamics</span> Branch of dynamics concerned with studying the motion of air

Aerodynamics is the study of the motion of air, particularly when affected by a solid object, such as an airplane wing. It involves topics covered in the field of fluid dynamics and its subfield of gas dynamics, and is an important domain of study in aeronautics. The term aerodynamics is often used synonymously with gas dynamics, the difference being that "gas dynamics" applies to the study of the motion of all gases, and is not limited to air. The formal study of aerodynamics began in the modern sense in the eighteenth century, although observations of fundamental concepts such as aerodynamic drag were recorded much earlier. Most of the early efforts in aerodynamics were directed toward achieving heavier-than-air flight, which was first demonstrated by Otto Lilienthal in 1891. Since then, the use of aerodynamics through mathematical analysis, empirical approximations, wind tunnel experimentation, and computer simulations has formed a rational basis for the development of heavier-than-air flight and a number of other technologies. Recent work in aerodynamics has focused on issues related to compressible flow, turbulence, and boundary layers and has become increasingly computational in nature.

<span class="mw-page-title-main">Fluid dynamics</span> Aspects of fluid mechanics involving flow

In physics, physical chemistry and engineering, fluid dynamics is a subdiscipline of fluid mechanics that describes the flow of fluids—liquids and gases. It has several subdisciplines, including aerodynamics and hydrodynamics. Fluid dynamics has a wide range of applications, including calculating forces and moments on aircraft, determining the mass flow rate of petroleum through pipelines, predicting weather patterns, understanding nebulae in interstellar space and modelling fission weapon detonation.

<span class="mw-page-title-main">Sir George Stokes, 1st Baronet</span> Anglo-Irish mathematician and physicist (1819–1903)

Sir George Gabriel Stokes, 1st Baronet, was an Irish physicist and mathematician. Born in County Sligo, Ireland, Stokes spent all of his career at the University of Cambridge, where he was the Lucasian Professor of Mathematics from 1849 until his death in 1903. As a physicist, Stokes made seminal contributions to fluid mechanics, including the Navier–Stokes equations; and to physical optics, with notable works on polarization and fluorescence. As a mathematician, he popularised "Stokes' theorem" in vector calculus and contributed to the theory of asymptotic expansions. Stokes, along with Felix Hoppe-Seyler, first demonstrated the oxygen transport function of haemoglobin, and showed colour changes produced by the aeration of haemoglobin solutions.

<span class="mw-page-title-main">Capillary action</span> Ability of a liquid to flow in narrow spaces

Capillary action is the process of a liquid flowing in a narrow space in opposition to or at least without the assistance of any external forces like gravity.

<span class="mw-page-title-main">Osborne Reynolds</span> Anglo-Irish innovator (1842–1912)

Osborne Reynolds was an Irish-born British innovator in the understanding of fluid dynamics. Separately, his studies of heat transfer between solids and fluids brought improvements in boiler and condenser design. He spent his entire career at what is now the University of Manchester.

dAlemberts paradox

In fluid dynamics, d'Alembert's paradox is a contradiction reached in 1752 by French mathematician Jean le Rond d'Alembert. d'Alembert proved that – for incompressible and inviscid potential flow – the drag force is zero on a body moving with constant velocity relative to the fluid. Zero drag is in direct contradiction to the observation of substantial drag on bodies moving relative to fluids, such as air and water; especially at high velocities corresponding with high Reynolds numbers. It is a particular example of the reversibility paradox.

<span class="mw-page-title-main">Hydrostatics</span> Branch of fluid mechanics that studies fluids at rest

Fluid statics or hydrostatics is the branch of fluid mechanics that studies fluids at hydrostatic equilibrium and "the pressure in a fluid or exerted by a fluid on an immersed body".

<span class="mw-page-title-main">Capillary wave</span> Wave on the surface of a fluid, dominated by surface tension

A capillary wave is a wave traveling along the phase boundary of a fluid, whose dynamics and phase velocity are dominated by the effects of surface tension.

<span class="mw-page-title-main">History of fluid mechanics</span>

The history of fluid mechanics is a fundamental strand of the history of physics and engineering. The study of the movement of fluids and the forces that act upon them dates back to pre-history. The field has undergone a continuous evolution, driven by human dependence on water, meteorological conditions and internal biological processes.

Fluid mechanics is the branch of physics concerned with the mechanics of fluids and the forces on them. It has applications in a wide range of disciplines, including mechanical, aerospace, civil, chemical, and biomedical engineering, as well as geophysics, oceanography, meteorology, astrophysics, and biology.

<span class="mw-page-title-main">Viktor Bunyakovsky</span> Russian mathematician

Viktor Yakovlevich Bunyakovsky was a Russian mathematician, member and later vice president of the Petersburg Academy of Sciences.

Pierre-Henri Hugoniot was an inventor, mathematician, and physicist who worked on fluid mechanics, especially on issues related to material shock. He mostly lived in Montbéliard, (Franche-Comté).

Volume viscosity is a material property relevant for characterizing fluid flow. Common symbols are or . It has dimensions, and the corresponding SI unit is the pascal-second (Pa·s).

<span class="mw-page-title-main">Liquid</span> State of matter

A liquid is a nearly incompressible fluid that conforms to the shape of its container but retains a nearly constant volume independent of pressure. It is one of the four fundamental states of matter, and is the only state with a definite volume but no fixed shape.

In fluid dynamics, Airy wave theory gives a linearised description of the propagation of gravity waves on the surface of a homogeneous fluid layer. The theory assumes that the fluid layer has a uniform mean depth, and that the fluid flow is inviscid, incompressible and irrotational. This theory was first published, in correct form, by George Biddell Airy in the 19th century.

<span class="mw-page-title-main">August Davidov</span> Russian mathematician (1823–1886)

August Yulevich Davidov was a Russian mathematician and engineer, professor at Moscow University, and author of works on differential equations with partial derivatives, definite integrals, and the application of probability theory to statistics, and textbooks on elementary mathematics which were repeatedly reprinted from the 1860s to the 1920s. He was president of the Moscow Mathematical Society from 1866 to 1885.

<span class="mw-page-title-main">Rayleigh–Bénard convection</span> Type of heat transfer within fluids

In fluid thermodynamics, Rayleigh–Bénard convection is a type of natural convection, occurring in a planar horizontal layer of fluid heated from below, in which the fluid develops a regular pattern of convection cells known as Bénard cells. This phenomenon can also manifest where a species denser than the electrolyte is consumed from below and generated at the top. Bénard–Rayleigh convection is one of the most commonly studied convection phenomena because of its analytical and experimental accessibility. The convection patterns are the most carefully examined example of self-organizing nonlinear systems.

The Arnold–Beltrami–Childress (ABC) flow or Gromeka–Arnold–Beltrami–Childress (GABC) flow is a three-dimensional incompressible velocity field which is an exact solution of Euler's equation. Its representation in Cartesian coordinates is the following:

Yves Pomeau, born in 1942, is a French mathematician and physicist, emeritus research director at the CNRS and corresponding member of the French Academy of sciences. He was one of the founders of the Laboratoire de Physique Statistique, École Normale Supérieure, Paris. He is the son of literature professor René Pomeau.

Nader Masmoudi is a Tunisian mathematician.

References

  1. 1 2 3 Urbanowicz, Kamil; Tijsseling, Arris S. (2024). "Ten Years of Passion: I.S. Gromeka's Contribution to Science". Fluids. 9 (4): 57. doi: 10.3390/fluids9030057 .
  2. 1 2 "Essay on the Theory of Capillary Phenomena:Theory of surface adhesion by liquid" (PDF).
  3. 1 2 "On the influence of uneven temperature distribution on the propagation of sound" (PDF).
  4. Gromeka, I. S. (1881). Some Cases of Incompressible Fluid Flow. Collected Works.
  5. Saqr, Khalid (22 September 2022). "The forgotten legacy of I.S. Gromeka".
  6. Gromeka, I. S. (1952). Collected Works, Akad. Nauk SSSR, Moscow, 15-89.
  7. "Vortical Flows in Memory of Professor Ippolit Stepanovich Gromeka".