The diesel engine is modelled as an inertial element. I2 and a torque source Se1. The flexible coupling is shown to consist of flexibility, C5, and damping, R6, with a common velocity difference, f4. The O-junction between bond 3 and 7 is used to "compute the velocity difference" which is distributed to both C5 and R6. The two gears are shown as transformers (TF) with modulus equal to the gear ratios. The propeller is modelled as an inertial element, 133, with and resistance according to the propeller law, R32. The clutch is shown as a block, which we will treat in detail in the next section.
From the derived bond graph, we see that the causal input to the inertia elements I10 and I19 is different. When effort, e, is input to an I-element, the flow. f, is given by a function of the time integral of the effort, e. When f is input, e is a function of the time derivative of f.
This is called integral and derivative causality, respectively. Integral causality is also called preferred causality since nature only integrates, only mathematicians differentiate. When derivative causality must be assigned to an element, this means that the element is not dynamically independent. Thus, the element gives no state variable. As can be seen in Figure 2, the two inertia elements I10 and I26 have derivative causality, and the momentum belonging to these elements are not state variables. Using the relation for the step up gear and assigned causality the dependency is given by
We will now show how the bond graph deals with the presence of derivative causality when writing the state equation for the inertia element 19 following the standard systematic approach.
The state equation for element 19 is now described by other system state variables and known functions, except for the effort e10, being a dynamically dependent element (e20 is the torque transmitted trough the clutch). We will now eliminate e10 from the state equation using a standard approach.
The effort e10 can be obtained by differentiating p10 in Eq.
Substituting e10 from Eq. (5) into Eq. (4) yields the derivative of p19 on each side of the equation sign, and thus and implicit equation which always results from derivative causality. Rearranging the equation, the state equation for p19 becomes