• Journal of Ship and Ocean Technology
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• 제7권3호
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• pp.34-55
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• 2003

Explicit Kutta condition approximation, proved useful in existing time-domain solver of the unsteady propeller problem, requires a specified functional behavior of the vorticity in space near the trailing edge. In this paper, the strength of the discrete vortices is controlled to have a specified behavior in space in the frequency domain approach. A new formulation is introduced and is implemented for analysis of a lifting surface of a rectangular planform. Sample computations carried out according to the new formulation compares well with that of existing unsteady lifting problem in the time domain.

• Journal of information and communication convergence engineering
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• 제12권1호
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• pp.39-45
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• 2014

A numerical method for solving Hamiltonian equations is said to be symplectic if it preserves the symplectic structure associated with the equations. Various symplectic methods are widely used in many fields of science and technology. A symplectic method preserves an approximate Hamiltonian perturbed from the original Hamiltonian. It theoretically supports the effectiveness of symplectic methods for long-term integration. Although it is also related to long-term integration, numerical stability of symplectic methods have received little attention. In this paper, we consider explicit symplectic methods defined for Hamiltonian equations with Hamiltonians of the special form, and study their numerical stability using the harmonic oscillator as a test equation. We propose a new stability criterion and clarify the stability of some existing methods that are visually based on the criterion. We also derive a new method that is better than the existing methods with respect to a Courant-Friedrichs-Lewy condition for hyperbolic equations; this new method is tested through a numerical experiment with a nonlinear wave equation.

• 대한조선학회논문집
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• 제38권1호
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• pp.1-8
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• 2001

본 논문에서는 비압축성 Reynolds-Averaged Navier-Stokes 방정식을 수치 해석하여 자유표면을 포함한 선체 주위의 난류 유동을 계산하였다. 정규격자 상에서 공간의 이산화는 2차 정도의 유한차분법을, 시간의 적분에는 4단계 Runge-Kutta법을 이용하였고, 난류 닫힘 조건을 만족시키기 위해 Baldwin-Lomax 난류 모형을 사용하였다. 자유표면의 위치는 운동학적 경계조건식을 Lax-Wendroff법으로 풀어서 구하였고, 자유표면과 격자 경계면을 일치시키기 위해 매 시간마다 새로 계산된 자유표면 위치에 맞추어 격자를 새로 구성하였다. 속도와 압력에 대한 경계조건은 자유표면에서 점성을 무시하여 근사한 동역학적 조건을 적용해서 구하였다. 본 연구에서 개발된 수치해법을 검증하기 위하여 실험자료가 많은 Wigley 선형과 Sries 60 $C_B=0.6$ 선형에 대해 수치계산을 수행하였고 계산된 선체 주위의 파형이 실험 결과와 잘 일치하는 것을 확인하였다.