19 research outputs found
ΠΡΠ°Π΅Π²ΡΠ΅ Π·Π°Π΄Π°ΡΠΈ ΡΠ΅ΠΏΠ»ΠΎΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΎΡΡΠΈ ΠΏΡΠΈ ΠΏΠ΅ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΌ Π²ΠΎ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ΅ ΡΠ΅ΠΏΠ»ΠΎΠΎΡΠ΄Π°ΡΠΈ
The practically important problem of unsteady heat conduction with time-varying relative coefficient of heat transfer is considered. Systematization of different approaches for finding the analytical solution of the problem is shown: the method of splitting the generalized Fourier integral; expanding the desired temperature function in a power series; reduction of the problem to an integral Voltaire equation of the second kind. It is shown that in all cases the solution is reduced to an infinite series of successive approximations of various functional forms, and the main goal of each approach is to find the more successful of the first approximations. Particular cases of the time dependence of the relative heat transfer coefficient are considered: linear, exponential, degree, root. The analytical solutions and numerical experiments, the peculiarities of the temperature curves for a number of specified dependencies are given. It was established that in case of the time-linear heat transfer coefficient the temperature curve changes significantly differ in comparison with the classical case of constant coefficient, while exponential dependence makes no substantive difference.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π²Π°ΠΆΠ½ΡΠ΅ Π·Π°Π΄Π°ΡΠΈ Π½Π΅ΡΡΠ°ΡΠΈΠΎΠ½Π°ΡΠ½ΠΎΠΉ ΡΠ΅ΠΏΠ»ΠΎΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΎΡΡΠΈ Ρ ΠΏΠ΅ΡΠ΅ΠΌΠ΅Π½Π½ΡΠΌ Π²ΠΎ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΡΠΌ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠΎΠΌ ΡΠ΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½Π°. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΡΠΈΡΡΠ΅ΠΌΠ°ΡΠΈΠ·Π°ΡΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ΠΎΠ² ΠΏΡΠΈ Π½Π°Ρ
ΠΎΠΆΠ΄Π΅Π½ΠΈΠΈ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π·Π°Π΄Π°ΡΠΈ: ΠΌΠ΅ΡΠΎΠ΄ ΡΠ°ΡΡΠ΅ΠΏΠ»Π΅Π½ΠΈΡ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ Π€ΡΡΡΠ΅; ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠ΅ ΠΈΡΠΊΠΎΠΌΠΎΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΈ Π² ΡΡΠ΅ΠΏΠ΅Π½Π½ΠΎΠΉ ΡΡΠ΄; ΡΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ Π·Π°Π΄Π°ΡΠΈ ΠΊ ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΠΎΠΌΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ ΠΠΎΠ»ΡΡΠ΅ΡΠ° Π²ΡΠΎΡΠΎΠ³ΠΎ ΡΠΎΠ΄Π°. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π²ΠΎ Π²ΡΠ΅Ρ
ΡΠ»ΡΡΠ°ΡΡ
ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΡΠ²ΠΎΠ΄ΠΈΡΡΡ ΠΊ Π±Π΅ΡΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠΌΡ ΡΡΠ΄Ρ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΡΡ
ΠΏΡΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΠΉ ΡΠ°Π·Π»ΠΈΡΠ½ΠΎΠΉ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠΉ ΡΠΎΡΠΌΡ ΠΈ Π³Π»Π°Π²Π½ΠΎΠΉ ΡΠ΅Π»ΡΡ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΈΠ· ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ΠΎΠ² ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΎΡΡΡΠΊΠ°Π½ΠΈΠ΅ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠ΄Π°ΡΠ½ΠΎΠ³ΠΎ ΠΏΠ΅ΡΠ²ΠΎΠ³ΠΎ ΠΏΡΠΈΠ±Π»ΠΈΠΆΠ΅Π½ΠΈΡ. Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ ΡΠ°ΡΡΠ½ΡΠ΅ ΡΠ»ΡΡΠ°ΠΈ Π²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΉ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΡΠ΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½Π°: Π»ΠΈΠ½Π΅ΠΉΠ½Π°Ρ, ΡΠΊΡΠΏΠΎΠ½Π΅Π½ΡΠΈΠ°Π»ΡΠ½Π°Ρ, ΡΡΠ΅ΠΏΠ΅Π½Π½Π°Ρ, ΠΊΠΎΡΠ½Π΅Π²Π°Ρ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΈ ΡΠΈΡΠ»Π΅Π½Π½ΡΠ΅ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΡ, Π²ΡΡΠ²Π»Π΅Π½Ρ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΡΡ
ΠΊΡΠΈΠ²ΡΡ
Π΄Π»Ρ ΡΡΠ΄Π° ΡΠΊΠ°Π·Π°Π½Π½ΡΡ
Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠ΅ΠΉ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Π΄Π»Ρ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠ³ΠΎ Π·Π°ΠΊΠΎΠ½Π° Π²ΠΎ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΡΠ΅ΠΏΠ»ΠΎΠΎΡΠ΄Π°ΡΠΈ ΠΊΠ°ΡΡΠΈΠ½Π° ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠΉ ΠΊΡΠΈΠ²ΠΎΠΉ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠ»ΡΡΠ°Π΅ΠΌ Π΄Π»Ρ ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΠΈΠ·ΠΌΠ΅Π½ΡΠ΅ΡΡΡ, Π² ΡΠΎ Π²ΡΠ΅ΠΌΡ ΠΊΠ°ΠΊ ΡΠΊΡΠΏΠΎΠ½Π΅Π½ΡΠΈΠ°Π»ΡΠ½Π°Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ Π½Π΅ Π²Π½ΠΎΡΠΈΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ
Π’Π΅ΠΏΠ»ΠΎΠ²ΠΎΠΉ Π½Π°Π³ΡΠ΅Π² Π΄ΠΈΡΠΊΠ° Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌ ΠΊΡΡΠ³ΠΎΠ²ΡΠΌ Π²ΡΡΠ΅Π·ΠΎΠΌ
The thermal reaction of infinite disc with internal round neck was studied. The law of thermal elastic stresses with thermal heating was established on surface neck.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠ΅Π°ΠΊΡΠΈΡ Π±Π΅ΡΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠ³ΠΎ Π΄ΠΈΡΠΊΠ° Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌ ΠΊΡΡΠ³ΠΎΠ²ΡΠΌ Π²ΡΡΠ΅Π·ΠΎΠΌ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΡΠ΅ΡΠΌΠΎΡΠΏΡΡΠ³ΠΈΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΡ
ΠΏΡΠΈ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠΌ Π½Π°Π³ΡΠ΅Π²Π΅ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ Π²ΡΡΠ΅Π·Π°
Π’Π΅ΡΠΌΠΎΡΠΏΡΡΠ³Π°Ρ ΡΠ΅Π°ΠΊΡΠΈΡ Π΄Π²ΡΡ ΡΠ»ΠΎΠΉΠ½ΠΎΠ³ΠΎ ΠΊΡΡΠ³ΠΎΠ²ΠΎΠ³ΠΎ Π΄ΠΈΡΠΊΠ° Ρ ΡΠ΅Π½ΡΡΠ°Π»ΡΠ½ΡΠΌ ΠΊΡΡΠ³ΠΎΠ²ΡΠΌ Π²ΡΡΠ΅Π·ΠΎΠΌ
The thermal response of a two-layer disc with an inner circular indention was studied. The regularities of the thermoelastic stresses upon thermal heating of the boundary circular surfaces of the disk were determined.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠ΅Π°ΠΊΡΠΈΡ Π΄Π²ΡΡ
ΡΠ»ΠΎΠΉΠ½ΠΎΠ³ΠΎ Π΄ΠΈΡΠΊΠ° Ρ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠΌ ΠΊΡΡΠ³ΠΎΠ²ΡΠΌ Π²ΡΡΠ΅Π·ΠΎΠΌ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΡΠ΅ΡΠΌΠΎΡΠΏΡΡΠ³ΠΈΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ ΠΏΡΠΈ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠΌ Π½Π°Π³ΡΠ΅Π²Π΅ Π³ΡΠ°Π½ΠΈΡΠ½ΡΡ
ΠΊΡΡΠ³ΠΎΠ²ΡΡ
ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠ΅ΠΉ Π΄ΠΈΡΠΊΠ°
Π’Π΅ΡΠΌΠΎΠ²ΡΠ·ΠΊΠΎΡΠΏΡΡΠ³ΠΎΡΡΡ Π² Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ ΠΌΠΎΠ΄Π΅Π»ΡΡ ΡΠ΅ΠΎΡΠΈΠΈ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ°
While researching the thermal reaction of viscoelastic bodies under heatstroke conditions, the quasi-static HiltonLee-Sternberg theory of viscoelastic analogy generalization to dynamic models given inertial effects in the equations of motion was considered. The thermal reaction to heatstroke of a massive body (area with internal spherical cavity) with a sudden increase of its surface from initial To to Tc > 0 was researched. Numerical experiments were done, which revealed the qualitative difference of modeling results for the elastic body and viscoelastic body from rheological Maxwell and Kelvin models. It was found that the sudden heat of the surface of the viscoelastic body due to inertia force results in short-time stress close enough to the stress of the elastic, medium. Moreover, the difference of these stresses is decreased with increasing viscosity. The addition to this duration of action of inertial effects is about microseconds. During this time stress reaches its thermoelastic value before the growth of significant viscous flow. The qualitative behavior difference of viscoelastic Maxwell and Kelvin mediums on the body surface under conditions of sudden cooling within the quasi-static model of thermoviscoelasticity was described. The beginning of viscous flow in Maxwell medium which results in continuous stress decrease after discontinuous change tending to elastic medium stress was shown. On the contrary, in Kelvin medium jump of stress exceeds the value for the elastic medium, to which these stresses are tending.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Π° ΡΠ΅ΠΎΡΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ° Π²ΡΠ·ΠΊΠΎΡΠΏΡΡΠ³ΠΈΡ
ΡΠ΅Π» Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ. ΠΠΏΠΈΡΠ°Π½Π° ΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ ΡΠ΅Π°ΠΊΡΠΈΡ Π½Π° ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠΉ ΡΠ΄Π°Ρ ΠΌΠ°ΡΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΠ΅Π»Π° (ΠΏΠΎΠ»ΡΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²ΠΎ). Π£ΠΊΠ°Π·Π°Π½ΠΎ ΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ ΠΎΡΠ»ΠΈΡΠΈΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π΄Π»Ρ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΠΊΠ²Π°Π·ΠΈΡΡΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ»ΡΡΠ°Π΅Π²
Π’Π΅ΠΏΠ»ΠΎΠ²ΠΎΠΉ ΡΠ΄Π°Ρ ΠΌΠ°ΡΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΠ΅Π»Π° Ρ Π²Π½ΡΡΡΠ΅Π½Π½Π΅ΠΉ ΡΡΠ΅ΡΠΎΠΎΠ±ΡΠ°Π·Π½ΠΎΠΉ ΡΡΠ΅ΡΠΈΠ½ΠΎΠΉ
The role of inertial effects in the problem of heat stroke with a massive body having an internal spherical crack as an example was studied. An interrelationship for the calculation of the maximum dynamic stress, which is of great practical importance, is suggested.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° ΡΠΎΠ»Ρ ΠΈΠ½Π΅ΡΡΠΈΠΎΠ½Π½ΡΡ
ΡΡΡΠ΅ΠΊΡΠΎΠ² Π² ΠΏΡΠΎΠ±Π»Π΅ΠΌΠ΅ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ° Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΠΌΠ°ΡΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΠ΅Π»Π° Ρ Π²Π½ΡΡΡΠ΅Π½Π½Π΅ΠΉ ΡΡΠ΅ΡΠΎΠΎΠ±ΡΠ°Π·Π½ΠΎΠΉ ΡΡΠ΅ΡΠΈΠ½ΠΎΠΉ. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ΠΎ ΡΠΎΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎ ΡΠ°ΡΡΠ΅ΡΡ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌΠ° Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ, ΠΈΠΌΠ΅ΡΡΠ΅Π΅ Π²Π°ΠΆΠ½ΠΎΠ΅ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π·Π½Π°ΡΠ΅Π½ΠΈΠ΅
Changes in the reactivity of the vertebrobasilar arteries when using glucose-electrolyte drink with antioxidant plant extracts during submaximal exercise test
The aim. To assess the effect of glucose-electrolyte composition with plant extracts having antioxidant activity on the hemodynamic parameters of vertebrobasilar system during the incrementally increasing submaximal exercise test.Materials and methods. The study included 12Β athletes (6 candidates for master ofΒ sports and 6Β masters of sports) aged 18β22, who have been engaged in orienteering for 10Β years and more. Time of aerobic exercise β 2Β hours a day, five days a week. The study subjects performed anΒ incrementally increasing submaximal exercise test and also submaximal exercise test with the preventive intake of a glucose-electrolyte composition with plant extracts having antioxidant properties. To assess the hemodynamic parameters in all study subjects we used Doppler ultrasound ofΒ the cerebral vessels, evaluating vertebrobasilar system blood flow, exercise gas test in the modification of hypo- and hyperventilation, and also positional test.Results. A single intake of glucose-electrolyte drink under conditions of incrementally increasing exercise test contributed to the manifestation of a homeostatic effect in hemodynamic parameters of the vertebrobasilar arteries. It is evidenced byΒ theΒ approximation to the pre-exercise level ofΒ maximum systolic velocity andΒ average blood velocity in the breath-holding test, of the diastolic blood velocity inΒ theΒ hyperventilation test, and of the pulsatility index in the torsion test, as compared toΒ theΒ isolated submaximal exercise test which caused the change in both velocity indicators andΒ calculated indices during the functional tests.The article considers the main mechanisms underlying the change in arterial hemodynamic parameters caused by incrementally increasing load, as well as describes the proposed mechanisms arising from the combined effect of an incrementally increasing load and the intake of a glucose-electrolyte composition with plant extracts having antioxidant activity.Conclusion. It was shown that using glucose-electrolyte drink contributed to the restoration of hemodynamic parameters of the vertebrobasilar arteries after an incrementally increasing submaximal exercise test
ΠΠ±ΠΎΠ±ΡΠ΅Π½Π½Π°Ρ ΠΌΠΎΠ΄Π΅Π»Ρ ΡΠ΅ΡΠΌΠΎΠ²ΡΠ·ΠΊΠΎΡΠΏΡΡΠ³ΠΎΡΡΠΈ Π² ΡΠ΅ΠΎΡΠΈΠΈ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ°
The theory of heat stress for viscoelastic bodies based on linear rheological models of Maxwell and Kelvin for infinite domain bounded from inside by surfaces of either flat or cylindrical, or spherical shape together was examined. The influence of the geometrical factor and features of viscoelastic substances were found.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π° ΠΎΠ±ΠΎΠ±ΡΠ΅Π½Π½Π°Ρ ΡΠ΅ΠΎΡΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ° Π²ΡΠ·ΠΊΠΎΡΠΏΡΡΠ³ΠΈΡ
ΡΠ΅Π» Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
ΡΠ΅ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΠΠ°ΠΊΡΠ²Π΅Π»Π»Π° ΠΈ ΠΠ΅Π»ΡΠ²ΠΈΠ½Π° ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎ Π΄Π»Ρ Π±Π΅ΡΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ, ΠΎΠ³ΡΠ°Π½ΠΈΡΠ΅Π½Π½ΠΎΠΉ ΠΈΠ·Π½ΡΡΡΠΈ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΡΠΌΠΈ: Π»ΠΈΠ±ΠΎ ΠΏΠ»ΠΎΡΠΊΠΎΠΉ, Π»ΠΈΠ±ΠΎ ΡΠΈΠ»ΠΈΠ½Π΄ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ, Π»ΠΈΠ±ΠΎ ΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ. ΠΡΡΡΠ½Π΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°ΠΊΡΠΎΡΠ° ΠΈ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ Π²ΡΠ·ΠΊΠΎΡΠΏΡΡΠ³ΠΈΡ
ΡΡΠ΅Π΄
TΠ½Π΅rmal heating of dick with internal round neck
The thermal reaction of infinite disc with internal round neck was studied. The law of thermal elastic stresses with thermal heating was established on surface neck
Thermoelastic reaction of a two-layer circular disk with a central circular indention
The thermal response of a two-layer disc with an inner circular indention was studied. The regularities of the thermoelastic stresses upon thermal heating of the boundary circular surfaces of the disk were determined
Thermoviscoelasticity theory in the dynamic models of thermal shock
While researching the thermal reaction of viscoelastic bodies under heatstroke conditions, the quasi-static HiltonLee-Sternberg theory of viscoelastic analogy generalization to dynamic models given inertial effects in the equations of motion was considered. The thermal reaction to heatstroke of a massive body (area with internal spherical cavity) with a sudden increase of its surface from initial To to Tc > 0 was researched. Numerical experiments were done, which revealed the qualitative difference of modeling results for the elastic body and viscoelastic body from rheological Maxwell and Kelvin models. It was found that the sudden heat of the surface of the viscoelastic body due to inertia force results in short-time stress close enough to the stress of the elastic, medium. Moreover, the difference of these stresses is decreased with increasing viscosity. The addition to this duration of action of inertial effects is about microseconds. During this time stress reaches its thermoelastic value before the growth of significant viscous flow. The qualitative behavior difference of viscoelastic Maxwell and Kelvin mediums on the body surface under conditions of sudden cooling within the quasi-static model of thermoviscoelasticity was described. The beginning of viscous flow in Maxwell medium which results in continuous stress decrease after discontinuous change tending to elastic medium stress was shown. On the contrary, in Kelvin medium jump of stress exceeds the value for the elastic medium, to which these stresses are tending