1962
DOI: 10.1016/0017-9310(62)90059-5
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Laminar free convection from a non-isothermal cone

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Cited by 124 publications
(72 citation statements)
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“…For the natural convection from cones, Hering and Grosh [20] examined the laminar free convection from a non-isothermal cone. The laminar natural convection over a frustum convection about a truncated cone was studied by Na and Chiou [21].…”
mentioning
confidence: 99%
“…For the natural convection from cones, Hering and Grosh [20] examined the laminar free convection from a non-isothermal cone. The laminar natural convection over a frustum convection about a truncated cone was studied by Na and Chiou [21].…”
mentioning
confidence: 99%
“…the numerical solutions obtained from the Equations (11)-(13) using boundary conditions (14) are independent of cone semi vertical angle φ) are compared with the available results of Hering and Grosh [3], Hering [4], and Pop et al [9], are found to be in excellent agreement. along surface of the cone from the apex (x = 0) and y measures the distance normally outward.…”
Section: Mathematical Analysismentioning
confidence: 63%
“…In addition, local skin-friction τ X and local Nusselt number N u X values for different Prandtl number and exponent n are compared with the results of Hering [4] in Table 1 and 2 respectively, where f ′′ (0), −θ ′ (0) are the local skin friction and the local Nusselt number obtained by Hering and Grosh [3] and Hering [4]. Here * indicates the values obtained for pure free convection at ξ = 1 by Pop et al [9] in Table 1, 2 and ** indicates the values obtained at X = 1.0 for free convection by Hering and Grosh [3] in Table 2. f ′′ (1, 0), −θ ′ (1, 0) are the local skin friction and the local Nusselt number obtained by Pop et al [9] for free convection flow past a vertical cone at ǫ = 1.…”
Section: Resultsmentioning
confidence: 99%
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“…These studies have included heat transfer (important for thermal treatment), mass transfer (critical to doping modification of polymers), viscous heating, M agnetohydrodynamic (for electro-conductive polymers) and many other phenomena. Hering and Grosh (1962) presented an early classical study on natural convection boundary layers' non-isothermal cone, showing that similarity solutions exist when the wall temperature distribution is a power function of distance along a cone ray. T hey further documented solutions for an isothermal surface as well as for the surface maintained at the temperature varying linearly with the distance measured from the apex of the cone for Prandtl number of 0.7.…”
Section: Introductionmentioning
confidence: 99%