Comparison ALTEK SC-LH1-30 vs Atmosfera CBK-A-30

The main application the solar collector is designed for. It is highly undesirable to deviate from these recommendations: the specific features of the design and operation depend on the purpose, and in the “non-native” mode, the device will at best be inefficient, and at worst it may fail and even lead to accidents.

— DHW. Application in domestic hot water supply systems is a classic option, the vast majority of modern solar collectors are made for. The specific method of embedding in the DHW system may be different: in particular, open models use direct water heating, and closed models use indirect heating (for more details, see "Loop system"). Anyway, solar heating can be very handy for providing hot water. It can play both an auxiliary role (to save energy during the main heating or as a backup in case the hot water is turned off), and the main one (for example, in a country cottage or other similar place where there is no hot water initially).

— Heating and DHW. Devices designed for use both for hot water supply and heating. For DHW, see the relevant paragraph for more details; however, not everything described there is true for this category. For the collector to be effectively integrated into the heating system, it must meet certain additional requirements. First of all, such an application is allowed only for closed devices (see "Loop system") — the heating circuit operates unde...r fairly high pressure and forced circulation, an open operation scheme is not applicable here. Secondly, the “heating” collector must allow year-round use (see “More features”) — after all, the heating issue is most acute in the cold season, and not all models can work at low outdoor temperatures.

— Swimming pool heating. This category includes high-performance solar collectors that can be used for heating water in the pool, as well as for other purposes that require a constant supply of large amounts of hot water — for example, the operation of underfloor heating systems or a set of bathtubs. Of course, they can also be used in a more traditional format — for example, for DHW systems; however, the described tasks associated with large consumption of heated water remain the main specialization.

This category includes solar collectors that can be used throughout the year — including in winter, at sub-zero air temperatures. The only condition for the effective operation of such a device is the presence of sunlight.

The main distinguishing feature of such models is a high degree of thermal insulation, designed not only to reduce heat loss but also to protect the heat carrier circulating inside from freezing. In most of these devices, thermal insulation is provided by vacuum (note that these can be not only vacuum but also improved flat collectors — see "Type" for more details). In addition, the principle of indirect heating is often used in year-round collectors: antifreeze with a freezing point well below zero plays the role of a heat carrier, and the heated water receives heat through the heat exchanger wall. However, modern technologies make it possible to make frost-resistant devices with direct heating.

The convenience of collectors of this type is obvious, but they are not cheap.

The total area of the absorbing surface of the collector. For kits with multiple collectors (see "Number of collectors"), the area for one device is indicated.

Note that the meaning of this parameter depends on the type of collector (see the relevant paragraph). In flat devices, we are talking about the working area — the size of the surface that is exposed to sunlight. In tubular models (vacuum, thermosiphon), where tubes play the role of an absorber, the total surface area of the tubes is taken into account — including that which is “in the shade” during operation and is not heated by the sun. Special reflectors can be used to overcome this problem.

All of the above means that only collectors of the same type and similar design can be compared with each other in terms of absorber area. If we talk about such a comparison, then a large area, on the one hand, provides greater efficiency and heating speed, and, on the other hand, it accordingly affects the dimensions of the device and the amount of space required for its installation. Thus, the total area of a flat collector approximately corresponds to the area of the working surface; it is slightly larger, but this difference is small. But in tubular models, there is a paradox when the total area is less than the absorber area.

Collector aperture area; in sets of several devices (see "Number of collectors") is indicated for one collector.

The aperture area is, in fact, the working area of the device: the size of the space directly illuminated by the sun. In flat models (see "Type") this size corresponds to the size of the glass surface on the front side of the collector; in this case, the aperture area is usually either equal to the area of the absorber (see the relevant paragraph) or slightly less (because the edges of the collector can cover the edges of the absorbing surface. But in tubular collectors (vacuum, thermosiphon), the aperture area can be measured in different ways, depending on the presence of a reflector. If it is present, the working area is equal to the absorber area, since the tubes are irradiated from all sides. If a reflector is not provided, then the aperture area is taken as the sum of the projection areas of all tubes; projection length at this corresponds to the length of the tube, the width to the inner diameter of the glass bulb or the outer diameter of the inner tube, depending on the design.

The aperture area is one of the most important parameters for modern solar collectors; many performance specs depend on it. At the same time, by recalculating these specs per 1 m2 of the aperture area, one can compare different models (including those belonging to different types) with each other.

The type of tubes used in the design of the solar collector — vacuum or thermosiphon (see "Type").

— Coaxial vacuum direct heating. The simplest type of vacuum tube: is a hollow absorber tube enclosed in a glass vacuum tube. Such a tube has double walls, between which there is a vacuum, which provides the necessary degree of thermal insulation. And the term "direct heating" means that the heat carrier circulates directly in the inner tube, receiving heat through contact with the walls of the absorber.

The main advantages of direct heating tubes are simplicity and low cost. It is considered that they are poorly suited for year-round collectors. However, modern technologies allow for a very high degree of thermal insulation, due to which year-round systems of this type are also available on the market today. The situation is similar with the use in closed systems (see "Loop system"): direct heating elements are somewhat less suitable for such an application than more advanced vacuum tubes (like a heat pipe). Nevertheless, in addition to open ones, there are also closed systems with direct heating. However, the disadvantage of this option anyway is the relatively low efficiency.

— Coaxial vacuum heat pipes. The outer shell in such an element is glass, with double walls and a vacuum between them (like a thermos), but the inner part is just a heat pipe — a sealed flask (usually copper) filled with a special medium liquid with a low evaporation t...emperature. The upper part of this tube is led into the manifold (heat exchanger case), it has an enlarged size and plays the role of a radiator. The whole system works as follows: sunlight heats the heat pipe, and heating medium vapours rise to its upper part, where they condense and transfer heat through the radiator walls to the water moving along the manifold. The condensate flows back to the bottom of the heat pipe, after which the process is repeated.

Coaxial tubes with a heat pipe are more complex in design than direct heating systems, and, naturally, are more expensive. On the other hand, they are more efficient and can be used without restrictions in high-pressure closed collectors, as well as all-weather systems. In addition, devices with this principle of operation are easy to repair: if one of the tubes breaks, you do not need to change the entire manifold — just replace the tube itself. This does not cause any particular difficulties and can be carried out directly at the installation site, without dismantling the entire structure.

— Coaxial vacuum U-type. Vacuum tubes equipped with U-shaped heat exchangers. Such a heat exchanger has the form of a thin pipeline passing from the manifold body along the entire length of the tube and back; the pipeline is usually shaped like the letter U, hence the name. The manifold itself, usually, is made two-pipe: cold water enters the collector through one pipe (the inputs of U-shaped heat exchangers are connected to it), and the heated water is discharged through the other (the outlets of the heat exchangers are connected to it).

Such a design allows to achieve high efficiency rates in combination with excellent thermal insulation: water does not come into direct contact with the walls of the absorber, which is especially important when used in cold weather. And with the use of U-type tubes in closed systems (see "Loop system"), there are no problems either. Among the drawbacks, in addition to the rather high cost, one can name high hydrodynamic resistance and sensitivity to the quality of the heating medium. In addition, such collectors are difficult to repair: the pipes and manifold are a single unit, and to fix problems it is often necessary to remove the entire structure from the roof, and it is impossible to replace a single pipe. — Feather vacuum tubes. Feather vacuum tubes are a kind of modification of heat pipe systems (see the relevant paragraph). In them, the heat pipe is placed not in the inner tube, but on a flat absorber, and the whole structure is installed inside a glass flask from which the air is evacuated. Feather systems are highly efficient because the absorber does not heat the air inside the flask, but transfers almost all the energy to the heating medium; however, they are not cheap. In addition, such systems are quite difficult to install, and if the tube fails, it will inevitably have to be changed entirely (although there are usually no problems with the replacement itself). It is also worth noting that feather tubes are more dependent on the angle of incidence of light than devices with a traditional round absorber.

The total number of tubes provided in the design of the solar collector (vacuum or thermosyphon, see "Type").

This parameter largely depends on the area of the device: for a large collector, more tubes are required. However, there is no hard dependence here. Devices of similar size may differ in the number of tubes. In general, this parameter is quite specific, it is used in some formulas for calculating the required collector power.

The maximum pressure of the heating medium for which the collector is designed. This parameter is indicated only for closed models (see "Loop system") — by definition, open models operate at atmospheric pressure.

The maximum pressure allowed for the collector must not be lower than the operating pressure in the heating system (DHW, heating, etc.) to which it is planned to be connected. And ideally, you should choose a device with a pressure margin of at least 15 – 20% — this will give an additional guarantee in case of various failures and malfunctions.

Collector efficiency.

Initially, the term "efficiency" refers to a characteristic that describes the overall efficiency of the device — in other words, this coefficient indicates how much of the energy supplied to the device (in this case, solar) goes to useful work (in this case, heating the medium). However, in the case of solar collectors, the actual efficiency depends not only on the properties of the device itself but also on environmental conditions and some features of operation. Therefore, the specs usually indicate the maximum value of this parameter — the so-called optical efficiency, or "efficiency at zero heat loss." It is denoted by the symbol η₀ and depends solely on the properties of the device itself — namely, the absorption coefficient α, the glass transparency coefficient t and the efficiency of heat transfer from the absorber to the coolant Fr. In turn, the real efficiency (η) is calculated for each specific situation using a special formula that takes into account the temperature difference inside and outside the collector, the density of solar radiation entering the device, as well as special heat loss coefficients k1 and k2. Anyway, this indicator will be lower than the maximum — at least because the temperatures inside and outside the device will inevitably be different (and the higher this difference, the higher the heat loss).

Nevertheless, it is most convenient to evaluate the specs of a solar collector and compare it with oth...er models precisely by the maximum efficiency: under the same practical conditions (and with the same values of the coefficients k1 and k2), a device with a higher efficiency will be more efficient than a device with a lower one. .

In general, higher efficiency values allow to achieve the corresponding efficiency, while the collector area can be relatively small (which, accordingly, also has a positive effect on dimensions and price). This parameter is especially important if the device is planned to be used in the cold season, in an area with a relatively small amount of sunlight, or if there is not much space for the collector and it is impossible to use a large-area device. On the other hand, to increase efficiency, specific design solutions are required — and they just complicate and increase the cost of the design. Therefore, when choosing according to this indicator, it is worth considering the features of the use of the collector. For example, if the device is bought for a summer residence in the southern region, where it is planned to visit only in summer, relatively little water is required and there are no problems with sunny weather — you can not pay much attention to efficiency.

The absorption coefficient of the absorber used in the collector design.

This parameter directly affects the overall efficiency of the absorbing coating and the efficiency of the device as a whole. The absorption coefficient describes how much of the solar energy reaching the absorber is absorbed by it and transferred to the heat carrier. Ideally, this parameter should reach 100%. However, it is extremely difficult and unreasonably expensive to achieve this. Therefore, the absorption coefficient is usually somewhat lower — about 95%; this is more than enough for the efficient operation of the collector. The rest of the energy is reflected as radiation; for more details, see “Absorber emissivity coef ε". Also note here that in the design of tubular collectors, tubes with a special inner coating are often used, which returns the reflected rays to the absorber and increases the actual absorption coefficient.