Lakesailor
Well-Known Member
Off the top of my head; the typical approach is to start with the stability derivatives. These are the sensitivity of the forces and moments to changes in the motion, controls, or propulsion.
For example the derivative Ybeta is the change in side force, Y, per degree of sideslip (leeway), beta. Nbeta would be the change in yawing moment per degree of sideslip. Nr is the change in yawing moment due to yaw rate (rate of turn). Etc. There's a stability derivative for each force and moment, for each motion variable.
If you want to figure out how the boat will roll in a turn, you'd have to estimate each of the derivatives and then solve for the solution that simultaneously satisfies each of the equations.
For the example above, in which adding a skeg reduced the roll, here's what was happening. For a given speed, a certain amount of side force is necessary to turn the boat at a given rate, which is equal to m*V*R (mass times velocity times turn rate). This has to be supplied by sideslipping the hull, so that (ignoring rudder forces for the moment) Ybeta * beta = m*V*R. So beta = m*V*R/Ybeta.
There's also a rolling moment derivative, Lbeta, which tends to roll the boat away from the direction of the sideslip. And there's a rolling moment from the boat's buoyancy, which I'll call Lphi (and naval architects would call GM), that is the rolling moment due to heel. For the boat to be in equilibrium in heel, all the moments have to sum to zero; Lbeta*beta + Lphi*phi = 0. From this you can solve for the heel angle: phi = -Lbeta*beta/Lphi.
When you substitute in the result of the side force equation, you get
phi = -m*V*R*Lbeta/(Ybeta*Lphi)
But wait! There's also a yawing moment from beta, Nbeta, which tends to make the boat track straight, and a yawing moment from heel (Nphi) due to the change in underwater shape, and a yawing moment from the rudder (Nrudder). Which you solve to get the rudder required. Unfortunately, there's also roll due to rudder (Lrudder) because the rudder is below the center of gravity, and sideforce due to rudder deflection (Yrudder), too. Not to mention yaw moment due to turn rate (Nr) that gives the boat its yaw damping, and maybe rolling moment due to yaw rate (Lr) and side force due to yaw rate (Yr), too. In particular, the sideforce due to rudder will be to the outside of the turn, requiring more sideslip, and more roll, than indicated above.
So you have three equations (sideforce balance, roll moment, yaw moment) and three unknowns (phi, beta, rudder) to solve simultaneously. The only difficulty is getting the values of those pesky derivatives. They are determined by the hull characteristics. For example, the roll moment due to sideslip, Lbeta, will depend on the deadrise angle of the hull, with a V'd hull tending to roll more with sideslip than a flat bottom hull.
In the example cited, the boat rolled excessively in a turn because the ratio (Lbeta/Ybeta) was too high or the roll stiffness (Lphi) was too small. Adding the skeg produced more sideforce per degree of sideslip, increasing Ybeta. In addition, the skeg was below the c.g., so its contribution to the rolling moment was opposite of that the hull (tending to "trip" the boat and roll to the outside of the turn). So the skeg lowered the ratio (Lbeta/Ybeta) and reduced the roll.
So that's how you predict how a boat will roll in a turn.
For example the derivative Ybeta is the change in side force, Y, per degree of sideslip (leeway), beta. Nbeta would be the change in yawing moment per degree of sideslip. Nr is the change in yawing moment due to yaw rate (rate of turn). Etc. There's a stability derivative for each force and moment, for each motion variable.
If you want to figure out how the boat will roll in a turn, you'd have to estimate each of the derivatives and then solve for the solution that simultaneously satisfies each of the equations.
For the example above, in which adding a skeg reduced the roll, here's what was happening. For a given speed, a certain amount of side force is necessary to turn the boat at a given rate, which is equal to m*V*R (mass times velocity times turn rate). This has to be supplied by sideslipping the hull, so that (ignoring rudder forces for the moment) Ybeta * beta = m*V*R. So beta = m*V*R/Ybeta.
There's also a rolling moment derivative, Lbeta, which tends to roll the boat away from the direction of the sideslip. And there's a rolling moment from the boat's buoyancy, which I'll call Lphi (and naval architects would call GM), that is the rolling moment due to heel. For the boat to be in equilibrium in heel, all the moments have to sum to zero; Lbeta*beta + Lphi*phi = 0. From this you can solve for the heel angle: phi = -Lbeta*beta/Lphi.
When you substitute in the result of the side force equation, you get
phi = -m*V*R*Lbeta/(Ybeta*Lphi)
But wait! There's also a yawing moment from beta, Nbeta, which tends to make the boat track straight, and a yawing moment from heel (Nphi) due to the change in underwater shape, and a yawing moment from the rudder (Nrudder). Which you solve to get the rudder required. Unfortunately, there's also roll due to rudder (Lrudder) because the rudder is below the center of gravity, and sideforce due to rudder deflection (Yrudder), too. Not to mention yaw moment due to turn rate (Nr) that gives the boat its yaw damping, and maybe rolling moment due to yaw rate (Lr) and side force due to yaw rate (Yr), too. In particular, the sideforce due to rudder will be to the outside of the turn, requiring more sideslip, and more roll, than indicated above.
So you have three equations (sideforce balance, roll moment, yaw moment) and three unknowns (phi, beta, rudder) to solve simultaneously. The only difficulty is getting the values of those pesky derivatives. They are determined by the hull characteristics. For example, the roll moment due to sideslip, Lbeta, will depend on the deadrise angle of the hull, with a V'd hull tending to roll more with sideslip than a flat bottom hull.
In the example cited, the boat rolled excessively in a turn because the ratio (Lbeta/Ybeta) was too high or the roll stiffness (Lphi) was too small. Adding the skeg produced more sideforce per degree of sideslip, increasing Ybeta. In addition, the skeg was below the c.g., so its contribution to the rolling moment was opposite of that the hull (tending to "trip" the boat and roll to the outside of the turn). So the skeg lowered the ratio (Lbeta/Ybeta) and reduced the roll.
So that's how you predict how a boat will roll in a turn.