[0001] The invention relates to a method of operating an installation for refrigerating
products under vacuum, particularly products consisting mainly of water, such as lettuce,
which installation comprises a closable vessel for the products, one or more vacuum
pumps adapted to produce a vacuum in the interior of the vessel, a water vapour condenser
disposed in the vessel and through which a refrigerant can be passed, and a refrigerating
unit comprising a compressor, a condenser and a throttle valve, disposed outside the
vessel and an evaporator being formed by said water vapour condenser disposed in the
vessel, whereby a low-pressure separator is provided for liquid and vaporous refrigerant,
the suction pipe of the compressor and the outlet pipe of the throttle valve as well
as the two pipes of the water vapour condensor, being connected to said separator,
while a high-pressure vessel for liquid refrigerant is disposed between the refrigerant
condensor and the throttle valve.
[0002] Such a method is described in US Patent 2,748,576.
[0003] The desired boiling temperature (flash point) of the water is obtained by lowering
the pressure in the installation with the aid of the vacuum pump or pumps. Heat is
required to evaporate water, and this will be taken from the product.
[0004] A method of this kind is not carried out continuously but by the batch method, that
is to say load by load.
[0005] After the installation has been loaded up, the vessel is closed. The vacuum pump
is operated until the water in the product is evaporated (flash point). The water
vapour formed is condensed on the water vapour condenser, while the vacuum pump draws
off the non-condensable gases, such as air.
[0006] When the desired final temperatur of the product is reached, the vacuum is released
and the installation opened.
[0007] The refrigerated load can then be replaced by a new load for refrigeration.
[0008] The vacuum pump remains in operation even when the flash point has been reached.
From that moment on the compressor is also normally brought into action in order to
pass refrigerant through the condenser and to condense the water vapour.
[0009] As an example a cycle of 20 minutes may be mentioned, comprising 8 minutes for producting
the vacuum, 8 minutes for the refrigeration, and 4 minutes for loading and unloading.
During this cycle time the vacuum pump then operates for 16 minutes and the refrigerating
unit for 8 minutes.
[0010] This means that the refrigerating unit must remove all the heat from the product
in 8 minutes.
[0011] There is little sense in keeping the water vapour condenser at a very low temperature
through operation of the refrigerating unit before the flash point is reached.
[0012] The invention seeks to modify the known method in such a manner that a much smaller
and therefore less expensive refrigerating unit can be used, and the compressor and
the refrigerant condenser may have the half size and the efficiency of the vacuum
pump(s) during vacumation can be highly improved.
[0013] According to the invention this can be achieved in that the compressor is brought
into action, with the throttle valve open, approximately simultaneously with the vacuum
pump or pumps and that the throttle valve is closed at reaching of the evaporation
temperature of the water in the product.
[0014] In this way it is possible to create a "stock" of cold even before the flash point
is reached. This "stock" is used after the flash point has been reached.
[0015] The invention will be explained more fully with the aid of an operating diagram.
[0016] The water vapour condenser disposed in the vacuum tank is designated 1; it is generally
divided into a plurality of condenser sections. From this condenser 1 a pipe 2 extends
to the top gas part of a liquid-gas separator 3 for a refrigerant, for example R 22.
[0017] From the bottom liquid part of the separator 3 a pipe 4 extends back to the water
vapour condenser 1.
[0018] A pump 5 is provided in this pipe 4. This pump 5 circulates refrigerant through 1,
2, 3, 4 and 5.
[0019] This forms one branch of the refrigerant circuit. The other branch is formed by asuction
pipe 6 connected to the end of the separator 3, a compressor 7, a pressure pipe 8,
a refrigerant condenser 9, a pipe 10, a reservoir 11 for liquid refrigerant, a pipe
12, a throttle valve 13 for liquid refrigerant, and a pipe 14 returning to the gas
part of the separator 3.
[0020] As soon as the installation is filled with a load for refrigeration and the formation
of the vacuum starts, the compressor 7 is also put into action.
[0021] This compressor 7 ensures that liquid refrigerant contained in the high-pressure
vessel 11, and having for example a temperature of + 35° C, is conducted to the low-pressure
vessel 3. The temperature of the refrigerant is thus lowered to, for example, -5°
C or even lower, for example -20°.
[0022] A large amount of refrigerant is thus put into stock before the product gives up
its heat. This thus takes place during the first 8 minutes of the cycle time of 20
minutes taken as an example and including aeration, loading and unloading.
[0023] During this so-called prerefrigeration period the pipes of the water vapour condenser
1 are thereby brought for example to a temperature of -5° or even lower. The vapour
pressure of the water vapour in the installation thus falls to below 4 millibars.
This means that with a pressure of about 46 millibars in the vessel the vacuum pump
must draw in a gas mixture consisting of about 10% water vapour and 90% air. The rate
at which the vacuum is produced is thereby approximately doubled, in the ratio of
50 : 90.
[0024] When the pipes of the water vapour condenser 1 are not precooled, they have a temperature
of, for example, + 20° , corresponding to a pressure of the water vapour in the gas
mixture of 23 millibars. This means that when the totale pressure has been reduced
to 46 millibars by the vacuum pump the mixture flowing over the pipes of the water
vapour condenser 1 then consists of 50 parts by volume of air.
[0025] In the case of precooling the mixture consists of 10% water vapour and 90% air.
[0026] Because of the precooling, moreover, the water vapour is deposited on the pipes of
the condenser in the form of ice. A coating of ice is thus formed. The adhering water
drops also freeze, assisted by the low temperature of the material of the pipes.
[0027] When the flash point is reached, the throttle valve 13 is closed and the compressor
7 continues to operate. No further warm liquid refrigerant is thus conducted from
the high-pressure vessel 11 to the separator 3, and consequently no more expansion
vapour is produced in the low-pressure separator 3.
[0028] The vaporous refrigerant extracted from the separator 3 by the compressor 7 via the
pipe 6 consists solely of vapour generated by heat from the product.
[0029] This heat is removed from the product via the water vapour condenser 1.
[0030] The ballast of the flash vapour and the warm refrigerant liquid has thus been eliminated.
[0031] The vapour compressed by the compressor 7 is condensed in the condenser 9 and then
deposited as a liquid in the high-pressure vessel 11, where it is kept for the next
cycle.
[0032] A conventional refrigeration circuit is in fact divided into two incomplete circuits.
[0033] In the circuit 7, 8, 9, 10, 11, 12, 13, 14, 3, 6 warm liquid refrigerant is converted
into cold liquid and flash vapour, and in the circuit 1, 2, 3, 4, 5 cold liquid refrigerant
is converted back into vapour by the supply of heat from the product.
[0034] The effect is thereby achieved that the compressor 7 and the condenser 9 can be about
half the size in comparison with a conventional vacuum refrigeration installation,
as calculated in the following example.
[0035] Assuming that during the cooling of the product 200 kg of R22 refrigerant are evaporated,
then
200 x 209 = 41,800 kJ of heat
are extracted from the product.
[0036] If the liquid in the high-pressure vessel 11 is at + 35°, the enthalpy of the liquid
R22 is equal to 243 kJ/kg.
[0037] When this liquid flows through the throttle valve 13 about 27% of gas is formed downstream
of the throttle valve 13 with a mean evaporation temperature of -5°C in the low-pressure
vessel 3. In order to obtain 200 kg nett of R22 in the low-pressure vessel 3, 200/73
x 27 = 73 kg more must be added.
[0038] The enthalpy of R22 gas at -5°C is 403 kJ/kg. For the cooling of the warm R22 liquid
the compressor takes off 73(403-243) = 11,680 kJ in the vacuum production period.
[0039] In the low-pressure vessel 3 there are for example still 800 kg of R22 from the previous
refrigeration cycle, with a temperature of -5°C. After the low-pressure vessel 3 has
been filled with the required 200 kg of R22, R22 can be further cooled to, for example,
-15°C, for which purpose the compressor must take off 1000 . 11.5 = 11,500 kJ.
[0040] All in all, the compressor can already produce in the first 8 minutes of the process
(the product not yet giving up heat) 11,680 + 11,500 + 23,180 kJ, which is more than
half the total amount of "heat" required, so that the refrigeration installation is
about half the size.
[0041] The consumption of energy remains approximately the same, but the installation becomes
much smaller.