Case 5.2: ONRT, trajectories
Case 5.2: ONRT
1. Description of case 5.2
 Free running at model point in calm water (mandatory)
 With propellers and rudders
 With bilge keels
 L_{PP} = 3.147 [m], (model scale 1:48.935)
 Radius of gyration for yaw and pitch 0.246L_{PP} (in air)
 Radius of gyration for roll 0.344B (in air)
 GM=2.068 [m] in fullscale (0.0423 [m] in model)
 Approach speed U_{0} = 15.1 [kn] in fullscale (1.11 [m/s] in model)
 Re∗=3.39×10^{6}, Fr∗=0.20, g = 9.80665 [m/s^{2}]
 Rudder rate 5.0 [deg/s] in fullscale (35.0 [deg/s] in model)
 Water depth: Infinity
Re∗: Nominal Reynolds number, the Reynolds number when ship runs in calm water with constant propeller rate of revolution.
Fr∗: Nominal Froude number, the Froude number when ship runs in calm water with constant propeller rate of revolution.
All quantities are nondimensionalized by desired approach speed (U
_{0}), length between perpendiculars (L
_{PP}):
(1)
where g is the gravitational acceleration and ν is the kinematic viscosity.
2. Experimental data
The submissions in case 5.2 will be compared to model tests carried out by IIHR. Roll decay result will be provided: time series of roll angle versus time.
3. Requested computations
The requested info are 3 submissions. You have to do 5.2.1 before to submit 5.2.2, you have to submit 5.2.2 before to submit 5.2.3.
Table 1: Requested computations

Manoeuvre 
Starting speed 
5.2.1 
Self propulsion information 
Fr = 0.20 (equivalent to 15.1 knots full scale) 
5.2.2 
20°/20° zigzag test, starting to starboard side 
Fr = 0.20 (equivalent to 15.1 knots full scale) 
5.2.3 
35° turning circle test, starting to portside 
Fr = 0.20 (equivalent to 15.1 knots full scale) 
3.1 Submission 5.2.1: Selfpropulsion
This submission is especially interesting for simulations based on URANS CFD. This case shows the “neutral rudder angle”, and the obtained longitudinal equilibrium (the propeller rpm and thrust). For simulations based on coefficient models, the neutral angle will often be zero.
 All results are to be given for model scale conditions.
 All simulations results should be provided in the format described in section 4.
 The propeller rate of revolution should correspond to the selfpropulsion point of the model. When the RPM is unknown (because for example a constant thrust or actuator disk model is used in CFD based simulations) please indicate this.
 Similar to the experiment, the rudders should be controlled by following autopilot during course keeping:
(2)
where δ(t) is rudder angle, proportional gain K_{P} is 1.0, ψ_{C} is the target yaw angle and ψ(t) is yaw angle. The maximum rudder rate should be assigned to 35.0 [deg/s]. Rudder angle should be controlled by P controller during approaching before starting rudder execution for manoeuvring (Target yaw angle: ψ_{C}=0°)
Please see section 6 for an example of the submission.
3.2 Submission 5.2.2: 20°/20° starboard side zigzag manoeuvre
 All results are to be given for model scale conditions.
 All simulations results should be provided in the format described in section 4.
 The propeller rate of revolution should correspond to the selfpropulsion point of the model. When the RPM is unknown (because for example a constant thrust or actuator disk model is used in CFD based simulations) please indicate this.
 Similar to the experiment, the rudders should be controlled by Equation (2) during approaching before starting rudder execution for starboard side zigzag.
 During the zigzag manoeuvre, the rudders should go to the real geometric 20 degrees (not to 20 degrees away from the neutral angle).
Please see section 5 for an example of the submission.
3.3 Submission 5.2.3: 35° portside turning circle manoeuvre
 All calculations are to be conducted for model scale conditions.
 All simulations results should be provided in the format described in section 4.
 The propeller rate of revolution should correspond to the selfpropulsion point of the model. When the RPM is unknown (because for example a constant thrust or actuator disk model is used in CFD based simulations) please indicate this.
 Similar to the experiment, the rudders should be controlled by Equation (2) during approaching before starting rudder execution for starboard side zigzag.
 During the turning circle manoeuvre, the rudders should go to the real geometric 35 degrees (not 35 degrees away from the neutral angle).
Please see section 7 for an example of the submission.
4. Format
 The trajectory and time histories of heave ¸ angular motions , dimensional velocities for 6DOF motions (u,v,w,p,q,r), rudder angle δ, thrust coefficient T and torque coefficient Q for each propeller and propeller rate of revolution n [rps] after the ship was released (t = t_{0}), should be submitted.
 The ship position or trajectory should be given in an Earthfixed coordinate system with X pointing North, Y pointing East, and Z pointing downward as shown in Figure 1. This XY axis system remains horizontal in the earth. The ship was released at (X_{0}, Y_{0}) when t = t_{0} . The roll angle (ϕ) is positive for pushing starboard into the water, pitch (θ) is positive for bow up position and yaw angle (ψ) ) is positive for bow turned to starboard. The reported trajectory is dimensional and angular motions should be reported in degrees. The angular velocities should be reported in degree second. The reported yaw angle should be the deviation of yaw angle respect to the target yaw i.e. ψψ_{C}.
 All velocities for 6DOF motions (u, v, w, p, q, r) should be reported in shipfixed coordinate system with x axis positive toward bow, y axis positive toward starboard and z axis positive downward. This xyz axis system is bodyfixed, which means it rotates with the ship in yaw and pitch and roll. Given this convention, the reported velocities are:
(3)
(4)
In Equation (4), the unit of , and is [deg/s].
 Rudder angle (δ) is positive when trailing edge moves to portside.
 The thrust T and torque Q for each propeller should be reported in shaft coordinate system with x axis positive toward the engine. Values are given dimensional
 All motions should be reported at O. The origin is located on O which is located at midships, the intersection of ordinate 10 the centre line plane and the still water waterline.
Time series of the manoeuvres should be send to the organizers in an excel file. The data shall be give on model scale, and it will be compared to model scale data.
The submission consists of an excel file (example is given) with 19 columns and with rows for every time step. The time step is free to chose, but a small enough time step somewhere around 0.05 to 0.01 is recommended to get sufficient accuracy. The following quantities are asked:
Table 2: Submission variables
Symbol 
Item 
Unit 
t 
time 
s 
X 
X position in earth fixed system 
m 
Y 
Y position in earth fixed system 
m 
Z 
Z position in earth fixed system 
m 
ϕ 
Roll angle 
degrees 
θ 
Pitch angle 
degrees 
ψ 
Yaw angle 
degree 
u 
surge velocity 
m/s 
v 
sway velocity 
m/s 
w 
heave velocity 
m/s 
p 
roll rate 
deg/s 
q 
pitch rate 
deg/s 
r 
yaw rate 
deg/s 
δ 
Rudder angle 
deg 
n 
Propeller revolutions of portside propeller 
rpm 
T_{PS} 
Thrust of portside propeller 
N 
T_{SB} 
Thrust of starboard side propeller 
N 
Q_{PS} 
Torque of portside propeller 
Nm 
Q_{SB} 
Torque of starboard side propeller 
Nm 
These data are illustrated in Figure 1. The origin is located on O. The time t=0 is the time when the steering starts. The initial direction of the model is the direction of Xaxis. Initial conditions at t = 0 are: X
_{0}=0, Y
_{0}=0, ψ=0, ϕ=0, u=U
_{0}, v=0, r=0, δ=0
There is a righthanded earthfixed coordinate system x
_{0}y
_{0}z
_{0}, and a horizontally moving right handed bodyfixed coordinate system xyz. The bodyfixed coordinate system has its origin in O (midship), and the xy plane moves with the ship. The heading angle is defined as the angle between X and x
_{0}axis. u and v are the velocity components in x and y direction. the hull drift angle will be defined as β=atan(v/u), and the total velocity U=√(u
^{2}+v
^{2}).
Figure 1: Illustration of the sign convention of the earthfixed and bodyfixed coordinate system.
5. Elaborated example for test case 5.2.1
For ONRT, we elaborated an actual example of an actual submission compared to actual experimental data.
For case 5.2.1, the comparison will look as displayed in the following figure. On top of the time traces as presented in below Figure 2, the average of the time traces will be determined. The averages are the comparison variables. For the time trace of Figure 3, these averages are given. In the case of unsteady , time domain RANS, these values will be asked. For the case of coefficient based simulations, or simulations based on empirical models, these average values can be given as 1 and 0.
Table 3: EFD values summary for Case 5.2.1
Variable 
Value 
Z[m] 
2.093E03 
ϕ[deg] 
2.952E02 
θ[deg] 
4.134E02 
ψ[deg] 
1.724E01 
u[m/s] 
1.128E+00 
v[m/s] 
4.277E03 
w[m/s] 
2.500E05 
p[deg/s] 
1.585E03 
q[deg/s] 
1.714E03 
r[deg/s] 
1.506E02 
δ[deg] 
1.937E01 
n[rpm] 
5.382E+02 
Figure 2: Example of trajectory of Case 5.2.1
Figure 3: Example of time traces of Case 5.2.1.
6. Elaborated example for case 5.2.2: 20°/20° starboard side zigzag
For case 5.2.2, the time traces will be plotted for comparison and this will look as displayed in Figure 5. From these time traces, the typical characteristics will be determined. These characteristics will be the comparison variables. Table 4 gives these characteristics. The bold variables are the primary validation variable, the nonbold are the secondary validation variables.
Figure 4: Example trajectory of Case 5.2.2
Figure 5: Time traces of several signals for Case 5.2.2
Table 4: Comparison values for Case 5.2.2
Category 
Unit 
Validation Variables 
Overshoot angles 
[deg] 
1^{st} overshoot angle (ψ_{OS1}) 

[deg] 
2^{nd} overshoot angle (ψ_{OS2}) 

[deg] 
3^{nd} overshoot angle (ψ_{OS3}) 

[s] 
Time of 2^{nd} rudder execute (t_{2}) 

[s] 
Time of 3^{rd} rudder execute (t_{3}) 

[s] 
Time of 4^{th} rudder execute (t_{4}) 

[s] 
Time of 5^{th} rudder execute (t_{5}) 
Times 
[s] 
Period (time between the 4^{th} and 2^{nd} rudder execute = t_{4}t_{2}) 

[s] 
1^{st} overshoot time (t_{OS1}) 

[s] 
2^{nd} overshoot time (t_{OS2}) 

[s] 
3^{rd} overshoot time (t_{OS3}) 
Maximum yaw rate 
[deg/s] 
Maximum yaw rate during 1^{st} overshoot between t_{2} and t_{3} (r_{1}) 

[deg/s] 
Maximum yaw rate during 2^{nd} overshoot between t_{3} and t_{4} (r_{2}) 

[deg/s] 
Maximum yaw rate during 3^{rd} overshoot between t_{4} and t_{5} (r_{3}) 
Maximum drift angle 
[deg] 
Maximum drift angle during 1^{st} overshoot between t_{2} and t_{3} (β_{1}) 

[deg] 
Maximum drift angle during 2^{nd} overshoot between t_{3} and t_{4} (β_{2}) 

[deg] 
Maximum drift angle during 3^{rd} overshoot between t_{4} and t_{5} (β_{3}) 
Maximum roll angle 
[deg] 
Maximum roll angle during 1^{st} overshoot between t_{2} and t_{3} (ϕ_{1}) 

[deg] 
Maximum roll angle during 2^{nd} overshoot between t_{3} and t_{4} (ϕ_{2}) 

[deg] 
Maximum roll angle during 3^{rd} overshoot between t_{4} and t_{5} (ϕ_{3}) 
Table 5: EFD values summary for Case 5.2.2
7. Elaborated example for case 5.2.3: 35° turning circle manoeuvre to portside
For case 5.2.3, the time traces and a birdeye view will be plotted for comparison as Figure 6 and this will look as displayed in Figure 7. From these time traces, the typical characteristics will be determined. These characteristics will be the comparison variables. Table 6 gives these characteristics. The bold variables are the primary validation variable, the nonbold are the secondary validation variables.
Figure 6: Example trajectory of Case 5.2.3
Figure 7: Time traces and birdeye views of Case 5.2.3
Table 6: Comparison values for the 35° turning circle manoeuvre
Category 
Unit 
Validation Variables 
Dimensions 
[] 
Advance / L_{PP} (AD/L_{PP}) 

[] 
Tactical diameter / L_{PP} (AD/L_{PP}) 

[] 
Transfer / L_{PP} (AD/L_{PP}) 
Times 
[s] 
Time to reach 90° (t_{90}°) 
Yaw rate 
[deg/s] 
Maximum yaw rate (r_{max}) 

[deg/s] 
Average yaw rate in the constant part of the turn (r_{C}) 
Speed 
[m/s] 
Speed in the steady part of the turn (U_{C}) 
Roll angles 
[deg] 
Maximum inward roll angle (ϕ_{inmax}) 

[deg] 
Maximum outward roll angle (ϕ_{outmax}) 

[deg] 
Roll angle in the constant part of the turn (ϕ_{c}) 
Nondimensional values 
[] 
Nondimensional yaw rate in the constant part of the turn (r’) 

[deg] 
Drift angle in the constant part of the turn (β_{C}) 

[] 
Pivot point (sin(β_{C})/r’) 

[] 
Speed ratio (U_{C}/U_{0}) 
Table 7: EFD values summary for Case 5.2.3