In this section, we’ll discuss relatively simple engineering domains.
These are ones where a
connector deals with only one through and
one across variable. Conceptually, this means that only one
conserved quantity is involved with that connector.
The following table covers four different engineering domains. In each domain, we see the choice of through and across variables that we will be using along with the SI units for those quantities.
|Domain||Through Variable||Across Variable|
|Electrical||Current [A]||Voltage [V]|
|Thermal||Heat [W]||Temperature [K]|
|Translational||Force [N]||Position [m]|
|Rotational||Torque [N.m]||Angle [rad]|
You may have seen a similar table before with slightly different choices. For example, you will sometimes see velocity (in ) chosen as the across variable for translational motion. The choices above are guided by two constraints.
The first constraint is that the through variable should be the time derivative of some conserved quantity. The reason for this constraint is that the through variable will be used to formulate generalized conservation equations in our system. As such, it is essential that the through variables be conserved quantities.
The second constraint is that the across variable should be the lowest order derivative to appear in any of our constitutive or empirical equations in the domain. So, for example, we chose position for translational motion because position is used in describing the behavior of a spring (i.e., Hooke’s law). If we had chosen velocity (the derivative of position with respect to time), then we would have been in the awkward situation of trying to describe the behavior of a spring in terms of velocities, not positions. An essential point here is that differentiation is lossy. If we know position, we can easily express velocity. But if we only know velocity, we cannot compute position without knowing an additional integration constant. This is why we want to work with across variables that have not been overly differentiated.
Now let’s look at each domain individually.
We can define a
connector for the electrical domain as follows:
connector Electrical Modelica.SIunits.Voltage v; flow Modelica.SIunits.Current i; end Electrical;
Here we see that the variable
v in this connector represents the
voltage and the variable
i represents the current.
Note the presence of the
flow qualifier in the declaration of
i, the current. The
flow qualifier is what tells the Modelica
i is the through variable. Recall from our
discussion on Acausal Connections that the
should be the time derivative of a conserved quantity. We can see
that this connector follows that convention, since
Current is the
time derivative of charge (and charge is a conserved quantity).
Note the absence of any qualifier in the declaration of
voltage. A variable without any qualifier is assumed to be the
across variable. You will find a more complete discussion about
Variables (including the various qualifiers that can
applied to them) later in this chapter.
The interested reader may wish to jump ahead to our discussion of Electrical Components to see how we build on the connector definition to create electrical circuit components.
A connector for modeling lumped heat transfer isn’t much different from an electrical connector:
connector Thermal Modelica.SIunits.Temperature T; flow Modelica.SIunits.HeatFlowRate q; end Thermal;
Current, this connector includes
HeatFlowRate. While the names are different,
the overall structure is essentially the same. The
includes one through variable (
q, indicated by the presence of the
flow qualifier) and one across variable (
T, indicated by the
lack of any qualifier). Again, we see that the type of the variable
HeatFlowRate, is the time derivative
of a conserved quantity, energy.
An example of how such a connector can be used to build components for
lumped thermal network modeling can be found in the upcoming
discussion on Heat Transfer Components. If you feel
comfortable with this
connector definition, feel free to jump
ahead. It would still be a good idea to read the
Review section of the Connectors chapter at
To model translational motion, we would define a connector as follows:
connector Translational Modelica.SIunits.Position x; flow Modelica.SIunits.Force f; end Translational;
Again, we see the same basic structure as before. The connector
contains one through variable,
f, and one across variable
Note that, although this is a one-dimensional mechanical connector,
the physical types are specific to translational motion and distinct
from the physical types used from the Rotational
case to be presented next.
An important fact about mechanical connectors that is often overlooked
is that the
flow variable is the time derivative of a
conserved quantity. For example, in the case of translational motion
f, is a force and force is the time
derivative of (linear) momentum and momentum is a conserved quantity.
For systems whose motion is constrained to be rotational, the
connector definition should be used:
connector Rotational Modelica.SIunits.Angle phi; flow Modelica.SIunits.Torque tau; end Rotational;
Here we see that the across variable is
phi (representing the
angular displacement) and the through variable is
torque. As with
all previous examples, the
flow variable is the time derivative of
a conserved quantity. In this case, that conserved quantity is
All the connectors defined in this section are grouped, for future reference, into a single package:
within ModelicaByExample.Connectors; package SimpleDomains "Examples of connectors for simple domains" connector Electrical Modelica.SIunits.Voltage v; flow Modelica.SIunits.Current i; end Electrical; connector Thermal Modelica.SIunits.Temperature T; flow Modelica.SIunits.HeatFlowRate q; end Thermal; connector Translational Modelica.SIunits.Position x; flow Modelica.SIunits.Force f; end Translational; connector Rotational Modelica.SIunits.Angle phi; flow Modelica.SIunits.Torque tau; end Rotational; end SimpleDomains;