2019
DOI: 10.1134/s0869864319050068
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Heat generation in a Couette-Taylor flow multicylinder system

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Cited by 7 publications
(12 citation statements)
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“…This work continues the authors' research [1][2][3][4][5][6], presenting the results of experiments on the dependence of the power generated by such a heat generator on the relative angular velocity of rotation, the geometry of the proposed design and the viscosity of the working fluid. These experiments demonstrate that with a viscosity of the working fluid (6-25) • 10 -6 m 2 /s and with a relative rotational velocity of the rotors with a frequency of (4-5) Hz, the heat generator of the proposed design can reach a specific power that is significant for practical use (150-250) kW/m 3 .…”
Section: Introductionsupporting
confidence: 52%
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“…This work continues the authors' research [1][2][3][4][5][6], presenting the results of experiments on the dependence of the power generated by such a heat generator on the relative angular velocity of rotation, the geometry of the proposed design and the viscosity of the working fluid. These experiments demonstrate that with a viscosity of the working fluid (6-25) • 10 -6 m 2 /s and with a relative rotational velocity of the rotors with a frequency of (4-5) Hz, the heat generator of the proposed design can reach a specific power that is significant for practical use (150-250) kW/m 3 .…”
Section: Introductionsupporting
confidence: 52%
“…3 (see table 1) Figure 3 gives the dependence of the specific power of the heat generator on the Reynolds number for a constant relative angular velocity of rotation of the rotors (Ω = 44 rad/s) with decreasing viscosity of the working fluid (with increasing temperature working fluid). The power released by the equivalent system is determined by the formula N = Ω•M [1,6]. Specific power is defined here as the power released by the heat generator, referred to the volume of the working fluid V, located in the annular gaps of the heat generator: In accordance with Figure 3, the power of the heat generator with an increase in the Reynolds number due to viscosity at a constant relative angular velocity of rotation of the rotors decreases according to the dependence close to hyperbola.…”
Section: Resultsmentioning
confidence: 99%
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“…The height of the WW is 400 mm, the diameter of the WW is 300 mm, and the width of the working blades is 75 mm. The used dynamometric system is described in detail in [6,7]. The dynamometer was calibrated in a static mode using exemplary weights.…”
Section: Experimental Setup Design and Techniquementioning
confidence: 99%
“…Structurally, the working part of the heat generator consists of two multi-cylinder rotors nested into each other and forming a system of annular coaxial channels. In such a device, heat is released in the volume of liquid located in narrow annular gaps between coaxial cylinders rotating towards each other (circular Couette-Taylor flow), which allows creation of effective heat sources [4][5][6][7]. The investigations carried out by the authors have shown that the specific thermal power released in a heat generator of such a design can reach values of the order of 1 MW/m 3 , which indicates the competitiveness of such devices among devices based on renewable energy sources.…”
Section: Introductionmentioning
confidence: 99%