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Articles

Ship acceleration motion under the action of a propulsion system: a combined empirical method for simulation and optimisation

, ORCID Icon, & ORCID Icon
Pages 200-215 | Received 18 Jan 2018, Accepted 15 Aug 2020, Published online: 07 Oct 2020

Figures & data

Figure 1. A ship accelerating forward: (a) longitudinal view and (b) top view. The ship initially is at rest, and a thrust force, T0, triggers the motion (right). Then, the speed of ship increases up to the time a dynamic equilibrium between all forces and moments is established (left). (c) shows some geometrical properties of the ship used for computation of the resistance.

Figure 1. A ship accelerating forward: (a) longitudinal view and (b) top view. The ship initially is at rest, and a thrust force, T0, triggers the motion (right). Then, the speed of ship increases up to the time a dynamic equilibrium between all forces and moments is established (left). (c) shows some geometrical properties of the ship used for computation of the resistance.

Figure 2. Body line of the displacement hull, model INSEAN 2340, studied by Olivieri et al. (Citation2003).

Figure 2. Body line of the displacement hull, model INSEAN 2340, studied by Olivieri et al. (Citation2003).

Table 1. Principal characteristics of the displacement hull, model INSEAN 2340, studied by Olivieri et al. (Citation2001).

Figure 3. Comparison of predicted resistance and experimental data of Olivieri et al. Citation2001 for the model with body lines of Figure and principal characteristics of Table .

Figure 3. Comparison of predicted resistance and experimental data of Olivieri et al. Citation2001 for the model with body lines of Figure 2 and principal characteristics of Table 1.

Figure 4. Comparison of predicted total resistance coefficient and experimental data of Olivieri et al. (Citation2001) for the model with body lines of Figure and principal characteristics of Table .

Figure 4. Comparison of predicted total resistance coefficient and experimental data of Olivieri et al. (Citation2001) for the model with body lines of Figure 2 and principal characteristics of Table 1.

Figure 5. Sample of computed KT and KQ for B-Series propellers with AE/Ao = 0.7: (a) Z = 3 and (b) Z = 4.

Figure 5. Sample of computed KT and KQ for B-Series propellers with AE/Ao = 0.7: (a) Z = 3 and (b) Z = 4.

Table 2. Coefficients to be implemented in Equations (41) and (42).

Table 3. Principal characteristics of the investigated ship.

Figure 6. Computed resistance for the investigated displacement ship.

Figure 6. Computed resistance for the investigated displacement ship.

Figure 7. Simulation of acceleration of investigated ship: (a) P/D = 0.9 and (b) P/D = 1.0.

Figure 7. Simulation of acceleration of investigated ship: (a) P/D = 0.9 and (b) P/D = 1.0.

Table 4. Upper and lower bands of the propeller.

Table 5. Upper and lower bands of the propeller.

Figure 8. Comparison of the acceleration performance of the ship with and without optimised propeller.

Figure 8. Comparison of the acceleration performance of the ship with and without optimised propeller.

Figure 9. Comparison of the rotation speed of the ship with and without optimised propeller.

Figure 9. Comparison of the rotation speed of the ship with and without optimised propeller.

Table 6. Initial values and optimised values of parameters.

Figure 10. Comparison of the propeller efficiency of the ship with and without optimised propeller.

Figure 10. Comparison of the propeller efficiency of the ship with and without optimised propeller.

Figure 11. Comparison of thrust force coefficient of the ship with and without optimised propeller.

Figure 11. Comparison of thrust force coefficient of the ship with and without optimised propeller.

Figure 12. Comparison of torque coefficient of the ship with and without optimised propeller.

Figure 12. Comparison of torque coefficient of the ship with and without optimised propeller.

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