6.10. Heat resist¶
Fig. 6.10.1 Schematic of a heat resist.¶
Fall type
type label |
description |
active |
---|---|---|
Heat resist |
Resistance according user-defined polynomial |
No |
6.10.1. Mathematical model¶
The head loss is given by:
with:
variable |
Description |
Units |
---|---|---|
\(\Delta H\) |
Head loss over resist |
m |
\(a\) |
Constant loss |
m |
\(b\) |
Linear loss |
m2/s |
\(c\) |
Quadratic loss |
m5/s2 |
\(Q\) |
Flow rate |
m3/s |
The head loss equation (6.10.1) can be rewritten in terms of pressure and mass flow rate:
variable |
Description |
Units |
---|---|---|
\(\Delta P\) |
Pressure loss over resist |
Pa |
\(\rho\) |
Fluid density at upstream connection point |
kg/m3 |
\(g\) |
Gravitational acceleration |
m/s2 |
\(\dot{m}\) |
Mass flow rate |
kg/s |
\(\Delta z\) |
Height difference over the resist |
m |
The temperature is calculated from an energy balance as:
with:
variable |
Description |
Units |
---|---|---|
\(c_{p1}/c_{p2}\) |
specific head of the fluid |
J/kg/K |
\(T_{1}/T_{2}\) |
upstream/ downstream temperature |
K |
\(Q_{gen}\) |
generated heat |
W |
\(fr\) |
Fraction of generated heat transferred to the fluid |
- |
The heat generated by friction (\(Q_{gen}\)) is defined by:
Note that the coefficient “a” is a constant loss coefficient, that is only valid for positive flow. If the flow is negative, the head loss contribution “a” (defined as H1-H2) is equal to that of a positive flow. This is useful when modeling osmotic membranes.
6.10.2. Heat Resist¶
6.10.2.1. Hydraulic specifications¶
description |
Input |
unit |
range |
default |
remarks |
---|---|---|---|---|---|
a in a+bQ+CQ|Q| |
Real |
[m] |
|||
b in a+bQ+CQ|Q| |
Real |
[s2/m2] |
|||
c in a+bQ+CQ|Q| |
Real |
[s4/m5] |
|||
Frac. Gen. heat to fluid |
Real |
[-] |
0-1 |
0 |
See also the loss equation (6.10.1) in the Mathematical model section.
6.10.2.2. Component specific output¶
Generated heat flux [W]
6.10.2.3. H-actions¶
None
6.10.2.4. Component messages¶
Message |
Type |
Explanation |
References