2017
DOI: 10.12691/ajme-5-3-1
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Propeller Efficiency Enhancement by the Blade's Tip Reformation

Abstract: Many devices are designed to augment thrust and efficiency. Propeller's blade plays a fundamental role in order to enhance efficiency. In this paper, DTMB4382 is selected as reference propeller in which blade reformation has been applied on the tip toward suction and pressure side and hydrodynamic performance have been discussed by using numerical investigation. Numerical results of the hydrodynamic characteristics of the propeller at the different blade tip angles are presented and discussed.

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Cited by 8 publications
(7 citation statements)
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“…where P is the static pressure, g i is the gravitational acceleration, F i is the external body force in an averaged Cartesian component of the velocity-vector in ith direction (i = 1, 2, 3) and ij is the Kroneker delta, which is equal to unity i = j and zero when i ≠ j [20].…”
Section: Mass Conservation Equationmentioning
confidence: 99%
See 1 more Smart Citation
“…where P is the static pressure, g i is the gravitational acceleration, F i is the external body force in an averaged Cartesian component of the velocity-vector in ith direction (i = 1, 2, 3) and ij is the Kroneker delta, which is equal to unity i = j and zero when i ≠ j [20].…”
Section: Mass Conservation Equationmentioning
confidence: 99%
“…Corresponding to the physical conservation laws above, the finite volume cell-centred discretization model for structure meshes is applied as a volume integral formulation with a finite partitioning set of volumes to discretize the equations; and is expressed in Eqs. 3and (4) [21]. Meanwhilst, the current numerical solution approach is solved using Runge-Kutta method of time discretization, dU∕dT = F(U).…”
Section: Numerical Schemementioning
confidence: 99%
“…where p = static pressure, = gravitational acceleration, = external body force in an averaged Cartesian component of the velocity-vector in i th direction (i=1,2,3) and ij  = Kroneker delta and is equal to unity i = j and zero when ≠ j [12]. Finally, defined Reynolds-stress tensor presented below as Eq.…”
Section: Governing Equationmentioning
confidence: 99%
“…This experimental method is very expensive, time-consuming, and have a complex procedure for various hydrodynamics analysis test configuration. Following the works of [12][13][14][15][16], the numerical methods are adopted to solve and analyze the fluid problem. The computational fluid dynamics (CFD) simulation are the best alternative with several advantages such as allow to simulate using actual and model geometry scale in extreme condition of the fluid flow and the CFD simulation also have a good agreement with experimental data [17][18][19][20].…”
Section: Introductionmentioning
confidence: 99%
“…During recent years, Ghassemi et al worked on the different propulsor (poded propeller, ducted propeller, surface propeller and propeller with augmentation devices) numerical analysis by BEM and CFD [23][24][25], ship hullpropeller interaction [26], calculations of the sound pressure level of the marine propeller in low frequency [27], hydrodynamic characteristics of the ducted propeller and its different geometries effect [28] as well as the propeller efficiency enhancement of the blade's tip reformation [29]. Based on cited works, mathematical functions of the nonuniform wake flow entered to the propeller geometries is not well known.…”
Section: Introductionmentioning
confidence: 99%