This is the partial parent class for all heat exchangers based on the the effectiveness-NTU method.
For stream dominated applications the following assumptions are made for mass flow regularization close to zero:
The model approximates the transient behavior of the heat
exchanger with a first-order ordinary differential equation.
Based on the conservation of energy one can derive that its time
constant TC can be approximated by the ratio of
thermal inertia (wall + fluid) dU / dT to the enthalpy
flow rate "inertia" dH_flow / dT:
TC ~ (m_HEX * c_HEX + m_FluidA * c_FluidA + m_FluidB *
c_FluidB) / (m_flow_FluidA * c_FluidA + m_flow_FluidB *
c_FluidB) ,
where m is the mass, m_flow is the
mass flow rate, c is the specific heat capacity,
U is the internal energy, T is the
temperature and H_flow = m_flow*h is the enthalpy flow
rate.
The default time constant TC = 0.01 is not
realistic and will be updated in the next major release.
For example a heat exchanger with a mass of 10 kg and
mass flow rates of 0.5 kg/s of air on both sides has a
time constant in the magnitude of about 10 s. The
default time constant can also lead to a stiff system, and thereby
increase simulation time.
Note that the time constant also avoids algebraic loops and may also be beneficial from a numerical point of view.
| Name | Description |
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Medium model A |
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Medium model B |