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In all new hydronic systems the circulation of water in the distribution and through the
terminals is supported by electric pumps. pre-existing systems may exist in which
such circulation is supported by the earth's gravitational field, through what is called
the thermosiphon effect: hot water (heated by the generator) is lighter than cold water
(cooled in the room terminals) and therefore, in a closed circuit, the latter tends to
move downwards, pushing upwards l warmer water. These systems have now been
abandoned due to the evident difficulty in varying and controlling the flow of water
circulating in the system and therefore the power supplied.). The term water flow,
symbol Q, refers to the quantity of water (expressed in this case as the volume of
water) which passes through the section of a pipe in a unit of time and is expressed in
m3/h (cubic meters per hour).
The term power supplied, symbol Φ, instead refers to the thermal power (i.e. the
amount of heat per unit of time) that the generic plant terminal provides to the
environment in which it is located; the unit of measurement for power is W (watts). In
general, hydronic systems have advantages over other types of system for relatively
low initial installation costs, fluid availability, low operating costs and practically silent
operation. The main disadvantage of hydronic systems is that they are obviously
unable to address and resolve the ventilation requirements of the building occupants.
Humidity control is absent or poor: they are basically only systems for heating or
cooling the environment. These disadvantages can however be overcome by
combining hydronic systems with aeraulic systems, to obtain the best from each of the
different types. The hydronic systems for environmental air conditioning can be
classified by operating temperature (flow temperature of the hydronic distribution
circuit), and can be divided into: -low temperature hot water (BT) <40 ° C; medium
temperature hot water (MT) from 40 ° C to 60 ° C; high temperature hot water (AT)>
60 ° C; chilled water (AR) from 2 ° C to 16 ° C, usually 7 ° C; dual temperature water
(ADT) MT and AR (38-65 ° C, 4-7 ° C). Most of the hydronic systems present in
commercial buildings are medium temperature systems (MT), although today the
trend is to have low temperature systems already used in residential buildings, chilled
water systems (AR) also in these buildings. o dual temperature systems (ADT).
Objectives of balancing
The design and installation of balanced circuits is needed to guarantee the correct flow
rate inside the emitters and inside branches of the hydraulic circuit, in order to: ensure
the correct performance of the emitters; provide the correct amount of thermal power
to the heated/cooled area; prevent excessive water velocities which can cause noise
and abrasion; prevent circulating pumps from operating under low efficiency
conditions, leading to overheating and limit the value of the differential pressures
acting on the regulating valves, thus, preventing damaging.
Example of hydronic circuit
circuit A and circuit B are two independent circuits which
flow into node 1. In this node, the circuits have the same
differential pressure. Circuit A: higher pressure drop
branch Circuit B: lower pressure drop branch Usually,
to size the circulation pump, the design differential pressure
is chosen according to the circuit with the highest pressure
drop. We guarantee that even the most critical emitter is
able to fulfill the thermal energy need of the room. But we
risk to have higher water flow rate in the other emitters with
lower pressure drop: overheating of rooms and excessive
velocity inside circuits.
Network extension
The degree of imbalance of flow rates through circuits depends on the number of
branches served:
if the number of branches is small, the differences between the required flow
rates and those obtained are generally within acceptable margins;
if the number of branches is large, the imbalances in the flow rates can be
considerable.
For medium and small systems with a constant flow rate, proper sizing of the pipework
will normally be adequate to ensure that the circuits are balanced. For systems with
extensive networks, or with variable flow rates, it is necessary to include equipment
capable of regulating water flow. Hydraulic network can be:
Direct return circuit: Elementary hydronic system installed by (1) heat
generator, in this case a boiler for hot water, (2) a circulation pump, (3)
terminals for heating in the spaces served (e.g. heating emitters if system high
temperature or radiant panels if low temperature system or fan coil units if
medium temperature
system), (4) the pipes that
connect the various devices
to each other and (5) an
expansion vessel. The
purpose of the expansion
tank is to allow the
expansion and volumetric contraction of the water due to temperature
variations in the system and to maintain the pressure of the hydraulic circuit at
the required value. It is necessary to cross the continuum from the water, it is
generally insulated at the same level as the pipes to minimize the losses or
thermal gains of the system. Different lengths of circuits of each terminal can
cause high risk of unbalanced pressure drop on different branches. Distance
between pump and emitter E much higher than distance pump-emitter A
→higher resistance to water flow → higher flow rate in emitter A, lower flow rate
in emitter E. Especially for extended network, they need to install balancing
valves to guarantee the nominal flow rate to each terminal.
Reverse return circuit: The advantage of a reverse return system is that the
resistance to water flow for each of the individual paths is approximately equal,
so the system is essentially self-balancing. However, the reverse return piping
system is more expensive due to the additional length of return pipes required,
and it may be more costly than the direct return system with balancing valves.
Control system
An hydronic system shall be designed and controlled in order to properly fulfill energy
needs of the building, which vary along the heating/cooling season according to
external conditions (e.g. external temperature, solar radiation) and internal gains. The
control system is composed of all devices (e.g. 3 way
valves, autoflow regulators, BMS) which allow to adapt
the thermal energy provided by the system to the
actual conditions, in order to reach indoor comfort
(e.g. avoiding under-heating or over-heating). In Figure
12, you can see one of the most common and
widespread hydronic heating systems: a residential
boiler that feeds radiators placed in different rooms. In
this case, the control system consists of thermostatic valves that, based on the preset
temperature (position of the valve's rotating head) and the detected ambient
temperature, open and close, increasing or decreasing the quantity of water (flow)
passing through the individual radiator per unit of time. Figure 13 shows the typical
trend of the power emitted by a radiator based on the percentage of water flow for an
assigned supply temperature (60 °C) and ambient temperature (20°C). The almost
proportional relationship is due to the fact that a reduction in flow also corresponds to
a decrease in the water's outlet temperature from the radiator (the water stays longer
inside it and, therefore, has more time to transfer heat to the surrounding environment
and cool down more). This lower temperature at the outlet causes an increase in the
temperature difference between the inlet and outlet water, and therefore a greater
temperature rise that partially counteracts the flow reduction. The thermal power
transferred from water to the radiator, and thus to the environment, is indeed given by
the product of the mass flow by the temperature difference between the inlet and
outlet: Φ = ��(��� − ����).
Balancing of hydronic system
The control of the system is something different from balancing, but they can
influence each other. Also for balancing, the aim is to control the proper amount of
thermal energy given by each emitter... Emitters are designed to fulfill the nominal
thermal power in design conditions, with specific operating temperatures and water
flow rate. When the flow rate is different from the nominal value, the thermal energy
provided by emitters will be lower or higher than actual needs. For this reason
balancing is a key point for the design of an hydronic system. Aim of balancing →
supplying emitters with the flow rate required by design specification.
In practice, balancing flow rates in the two branch circuits is not as straightforward as
this simplified discussion suggests. In the presence of a constant-speed pump, varying
the resistance of one circuit also affects the available pressure and, consequently, the
flow rate in the other circuit. In fact, the operating point of the entire system (i.e., the
flow rate provided with the pressure difference) is determined by the intersection of
the pump's characteristic curve with the hydronic circuit's characteristic curve, as
shown in Figure 16. The pump's characteristic curve is a property of the specific
pump employed (Water flow rate provided by pump is inversely proportional (non-
linear) to pressure drop) , while the circuit's characteristic curve depends on the
hydraulic resistance of the circuit, which, in turn, varies with the flow rate �(�): the
higher the resistance, the steeper the curve, and this steepness increases with the
flow rate. The characteristic curve of the circuit is defined as a parabolic curve
which passes from the orgin
and the theoretical point
(Q-∆p) of the circuit. The
hydronic resistance is not a
characteristic quantity of
the constant circuit, but
depends on the flow rate
circulating in it. The bond
between resistance and
flow rate can be considered as a linear approximation, that is R (Q) ≅Z Q, with the
characteristic constant Z of the circuit, called pressure drop coefficient.
Changing of characteristic curve of the circuit
The slope of the characteristic curve of the circuit increases with higher ∆p, which, in
turn, depends on the water flow rate Q → ∆p(Q). When, in order to balance a branch of
the circuit, a balancing valve is introduced, it increases the overall resistance of the
hydronic circuit, which passes from R to R+ΔR, and there will be a reduction in the
overall flow rate delivered: in the next picture,
the operating point moves from P to P1 and the
total volume flow changes from Q to Q1 <Q.
Consequently, the available pressure increases
and while the plant terminal on which the
balancing valve has been introduced has the
desired flow rate, the others see the pressure
increase and therefore the supply flow rate,
delivering more thermal power than required.
When a balancing valve is introduced, the total
hydronic