JP2011220559A - Refrigerating/air conditioning device - Google Patents

Refrigerating/air conditioning device Download PDF

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JP2011220559A
JP2011220559A JP2010087623A JP2010087623A JP2011220559A JP 2011220559 A JP2011220559 A JP 2011220559A JP 2010087623 A JP2010087623 A JP 2010087623A JP 2010087623 A JP2010087623 A JP 2010087623A JP 2011220559 A JP2011220559 A JP 2011220559A
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heat exchanger
temperature
utilization
refrigerant
outlet
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JP5153812B2 (en
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Koyu Tanaka
航祐 田中
Yoshihiro Sumida
嘉裕 隅田
Jun Mieno
純 三重野
Shinichi Asai
慎一 浅井
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Mitsubishi Electric Corp
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F25REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
    • F25BREFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
    • F25B41/00Fluid-circulation arrangements
    • F25B41/30Expansion means; Dispositions thereof
    • F25B41/31Expansion valves
    • F25B41/34Expansion valves with the valve member being actuated by electric means, e.g. by piezoelectric actuators
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F25REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
    • F25BREFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
    • F25B2600/00Control issues
    • F25B2600/25Control of valves
    • F25B2600/2513Expansion valves
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02BCLIMATE CHANGE MITIGATION TECHNOLOGIES RELATED TO BUILDINGS, e.g. HOUSING, HOUSE APPLIANCES OR RELATED END-USER APPLICATIONS
    • Y02B30/00Energy efficient heating, ventilation or air conditioning [HVAC]
    • Y02B30/70Efficient control or regulation technologies, e.g. for control of refrigerant flow, motor or heating

Abstract

PROBLEM TO BE SOLVED: To provide a refrigerating/air conditioning device of high reliability which is controllable and can maintain its performance even when a plurality of use-side units are applied.SOLUTION: This refrigerating/air conditioning device 1000 includes: a heat source unit 100 constituted of a compressor 1 and a heat source-side heat exchanger 2; two or more use units 200a, 200b constituted of expanding mechanisms 5a, 5b, use-side heat exchangers 6a, 6b, and internal heat exchangers 4a, 4b; a suction pressure sensor 12 and a discharge pressure sensor 11 constituted of liquid extension piping 3 and gas extension piping 7 and respectively disposed at an inlet and an outlet of the compressor 1; internal heat exchange low-pressure outlet temperature sensors 13a, 13b disposed at low pressure-side outlets of the use-side heat exchangers 6a, 6b; use-side heat exchange inlet temperature sensors 14a, 14b disposed at inlets of the use-side heat exchangers 6a, 6b; and sucked air temperature sensors 15a, 15b for detecting temperatures of load use fluids flowing into the use-side heat exchangers 6a, 6b.

Description

本発明は冷凍空調装置、特に、冷凍サイクルを実行するものであって、熱源ユニットと複数台の利用ユニットとを有する冷凍空調装置に関するものである。   The present invention relates to a refrigeration air conditioner, and more particularly to a refrigeration air conditioner that executes a refrigeration cycle and includes a heat source unit and a plurality of utilization units.

従来の冷凍空調装置は、冷媒を圧縮する圧縮機と、凝縮器と、減圧装置と、蒸発器と、これらを環状に接続して冷媒を循環させる冷媒配管と、を有し、冷凍サイクルを実行していた。そして、凝縮器において放出される温熱を利用したり、蒸発器において放出される冷熱を利用したりしていた。このとき、冷凍サイクルの効率を高める目的で、凝縮器から出て減圧装置に入る間の冷媒と、蒸発器を出て圧縮機に入る間の冷媒との間で熱交換をする「内部熱交換器」を備え、圧縮機の入口における冷媒の過熱度が所望の目標過熱度になるように減圧装置の流量調整を行う制御装置を備えた発明が開示されている(例えば特許文献1参照)。   A conventional refrigeration air conditioner has a compressor that compresses refrigerant, a condenser, a decompression device, an evaporator, and a refrigerant pipe that circulates the refrigerant by connecting them in a ring shape, and executes a refrigeration cycle. Was. And the warm heat discharge | released in a condenser was utilized, or the cold heat discharge | released in an evaporator was utilized. At this time, for the purpose of increasing the efficiency of the refrigeration cycle, heat exchange is performed between the refrigerant that exits the condenser and enters the decompression device, and the refrigerant that exits the evaporator and enters the compressor. And a control device that adjusts the flow rate of the decompression device so that the superheat degree of the refrigerant at the inlet of the compressor becomes a desired target superheat degree is disclosed (for example, see Patent Document 1).

特開2009−162388号公報(第5−7頁、第1図)JP 2009-162388 A (page 5-7, FIG. 1)

しかしながら、特許文献1に開示された冷凍空調装置には以下のような問題があった。
(あ)利用側ユニットが1台の場合は制御可能であるものの、利用側ユニットが複数台になると、それぞれの利用側ユニットの冷却対象負荷に応じて減圧装置の開口面積を変化させる必要があるため、対応することができず、冷却対象の温度を設定温度に個別に制御することができない。
(い)また、圧縮機入口の冷媒状態を所定の目標過熱度に制御されているときに、場合によっては、冷媒配管(ガス延長配管部)において冷媒が二相となるため、配管長さが長い場合は、ガス単相に対して圧力損失が大きくなる。このため、圧縮機が吸入する冷媒の圧力(低圧圧力)が低下し、性能の低下や信頼性の低下を招く恐れがある。
However, the refrigeration air conditioner disclosed in Patent Document 1 has the following problems.
(A) Although control is possible when there is one usage-side unit, when there are multiple usage-side units, it is necessary to change the opening area of the decompression device according to the cooling target load of each usage-side unit Therefore, it cannot respond and the temperature of the cooling target cannot be individually controlled to the set temperature.
(Ii) Also, when the refrigerant state at the compressor inlet is controlled to a predetermined target superheat degree, depending on the case, the refrigerant has two phases in the refrigerant pipe (gas extension pipe part). When it is long, the pressure loss becomes large with respect to the gas single phase. For this reason, the pressure (low pressure) of the refrigerant sucked by the compressor is lowered, and there is a possibility that performance and reliability are lowered.

本発明は、以上の問題に鑑み、利用側ユニットが複数台になっても、制御可能であって、性能を維持し、信頼性の高い冷凍空調装置を得ることを目的とする。   In view of the above problems, an object of the present invention is to obtain a highly reliable refrigeration air conditioner that can be controlled even when there are a plurality of usage-side units, maintains performance, and has high reliability.

本発明に係る冷凍空調装置は、熱源ユニットと少なくとも2台以上の利用ユニットとを有し、
前記熱源ユニットが、冷媒を圧縮する圧縮機と、該圧縮機から吐出された高圧冷媒が流入する熱源側熱交換器とから構成され、
前記利用ユニットが、前記熱源側熱交換器の出口と液延長配管によって連結され、前記熱源側熱交換器から流出した高圧冷媒が流入する膨張機構と、該膨張機構から流出した低圧冷媒が流入する利用側熱交換器と、前記膨張機構に流入する高圧冷媒と前記利用側熱交換器から流出する低圧冷媒との間で熱交換を行い、前記圧縮機の入口にガス延長配管によって連結された内部熱交換器とから構成され、
前記利用側熱交換器出口における低圧冷媒の過熱度を検出する過熱度検出手段と、
前記利用側熱交換器を通過して低圧冷媒との間で熱交換をする利用流体の前記利用側熱交換器の入口における温度または出口における温度を検出する流入利用流体温度検出手段または流出利用流体温度検出手段と、
前記利用流体の前記利用側熱交換器の入口における温度または出口における温度を設定する流入利用流体温度設定手段または流出利用流体温度設定手段と、
該流入利用流体温度設定手段または流出利用流体温度設定手段から求まるそれぞれの冷却負荷の大小に応じて、前記内部熱交換器の低圧側出口における目標過熱度または目標乾き度を設定する目標冷媒状態量演算手段と、
前記内部熱交換器の低圧側出口において前記過熱度または目標乾き度になるように、前記膨張機構の流量調整を行う流量調整制御手段と、
を備えたことを特徴とする。
The refrigerating and air-conditioning apparatus according to the present invention has a heat source unit and at least two utilization units,
The heat source unit is composed of a compressor that compresses the refrigerant, and a heat source side heat exchanger into which the high-pressure refrigerant discharged from the compressor flows,
The utilization unit is connected to the outlet of the heat source side heat exchanger by a liquid extension pipe, and an expansion mechanism into which the high pressure refrigerant flowing out from the heat source side heat exchanger flows, and the low pressure refrigerant flowing out from the expansion mechanism flows in Heat exchange between the use-side heat exchanger, the high-pressure refrigerant flowing into the expansion mechanism and the low-pressure refrigerant flowing out from the use-side heat exchanger, and connected to the inlet of the compressor by a gas extension pipe It consists of a heat exchanger and
Superheat degree detection means for detecting the superheat degree of the low-pressure refrigerant at the outlet of the use side heat exchanger;
Inflow utilization fluid temperature detection means or outflow utilization fluid that detects the temperature at the inlet or the outlet of the utilization side heat exchanger of the utilization fluid that passes through the utilization side heat exchanger and exchanges heat with the low-pressure refrigerant. Temperature detection means;
Inflow utilization fluid temperature setting means or outflow utilization fluid temperature setting means for setting the temperature at the inlet of the utilization side heat exchanger or the temperature at the outlet of the utilization fluid;
The target refrigerant state quantity for setting the target superheat degree or the target dryness at the low-pressure side outlet of the internal heat exchanger according to the size of each cooling load obtained from the inflow utilization fluid temperature setting means or the outflow utilization fluid temperature setting means Computing means;
Flow rate adjustment control means for adjusting the flow rate of the expansion mechanism so as to achieve the superheat or target dryness at the low pressure side outlet of the internal heat exchanger;
It is provided with.

本発明は前記構成であるから、複数台の利用ユニットのそれぞれの冷却負荷に応じて内部熱交換器の低圧側出口の冷媒状態量を制御することにより、頻繁な発停を防止することで、冷却対象(利用流体)の設定温度に対する温度変動が小さい制御性の高い運転を実現することができる。
また、利用側熱交換器の蒸発温度を高く維持することが可能となるため、高効率な運転を実現することができる。更に、蒸発温度がマイナス(氷点下)となる低温環境下においては、着霜量が低減され、デフロストに必要なエネルギーを低減することができる。
そして、ガス延長配管の冷媒状態量を適切に制御し、圧力損失を最小化することで、冷却性能を維持した信頼性の高い運転も実現することができる。
Since the present invention is configured as described above, by controlling the refrigerant state quantity at the low-pressure side outlet of the internal heat exchanger according to the cooling load of each of the plurality of utilization units, by preventing frequent start and stop, It is possible to realize an operation with high controllability with a small temperature fluctuation with respect to the set temperature of the object to be cooled (used fluid).
In addition, since the evaporation temperature of the use side heat exchanger can be kept high, highly efficient operation can be realized. Furthermore, in a low temperature environment where the evaporation temperature is negative (below freezing point), the amount of frost formation is reduced, and the energy required for defrosting can be reduced.
And by appropriately controlling the refrigerant state quantity in the gas extension pipe and minimizing the pressure loss, it is possible to realize a highly reliable operation maintaining the cooling performance.

本発明の実施の形態1に係る冷凍空調装置の冷媒回路を示す構成図。The block diagram which shows the refrigerant circuit of the refrigerating air-conditioning apparatus which concerns on Embodiment 1 of this invention. 図1に示す冷凍空調装置の内部熱交換器の効果を説明するp−h線図。The ph diagram explaining the effect of the internal heat exchanger of the refrigeration air conditioner shown in FIG. 利用側熱交換器出口における乾き度に対する冷却能力の関係を表す特性図。The characteristic view showing the relationship of the cooling capacity with respect to the dryness in a use side heat exchanger exit. 内部熱交換器の冷媒質量流量に対する伝熱係数の関係を表す特性図。The characteristic view showing the relationship of the heat transfer coefficient with respect to the refrigerant | coolant mass flow rate of an internal heat exchanger. 内部熱交換器の低圧側における入口から出口に至る部分を表すp−h線図。The ph diagram showing the part from the inlet_port | entrance in the low voltage | pressure side of an internal heat exchanger to an exit. 図1に示す冷凍空調装置の冷凍サイクルを表すp−h線図。The ph diagram showing the refrigerating cycle of the refrigerating air-conditioner shown in FIG. 低負荷側利用ユニットの膨張機構の開度による作用を表す特性図。The characteristic view showing the effect | action by the opening degree of the expansion mechanism of a low load side utilization unit. 本発明の実施の形態2に係る冷凍空調装置の冷媒回路を示す構成図。The block diagram which shows the refrigerant circuit of the refrigerating air conditioning apparatus which concerns on Embodiment 2 of this invention. 本発明の実施の形態3に係る冷凍空調装置の冷媒回路を示す構成図。The block diagram which shows the refrigerant circuit of the refrigerating air conditioning apparatus which concerns on Embodiment 3 of this invention. 図9に示す冷凍空調装置における乾き度と圧力損失の関係を示す特性図。The characteristic view which shows the relationship between the dryness in the refrigeration air conditioner shown in FIG. 9, and a pressure loss.

[実施の形態1]
図1〜図7は本発明の実施の形態1に係る冷凍空調装置を説明するものであって、図1は冷媒回路を示す構成図、図2は内部熱交換器の効果を説明するp−h線図(モリエル線図)、図3は利用側熱交換器の出口における乾き度に対する冷却能力の関係を表す特性図、図4は内部熱交換器の冷媒質量流量に対する伝熱係数(液側熱伝達率、ガス側熱伝達率、および熱通過率)の関係を表す特性図、図5は内部熱交換器の低圧側における入口から出口に至る部分を拡大して表すp−h線図(モリエル線図)、図6は冷凍サイクルを表すp−h線図、図7は低負荷側利用ユニットの膨張機構の開度を変化させた場合の作用(冷却能力と利用側熱交換器出口過熱度および内部熱交換器の低圧側出口過熱度の関係)を表す特性図である。なお、各図において同じ部分または相当する部分には同じ符号を付し、一部の説明を省略する。
[Embodiment 1]
1 to 7 illustrate a refrigerating and air-conditioning apparatus according to Embodiment 1 of the present invention. FIG. 1 is a configuration diagram illustrating a refrigerant circuit, and FIG. 2 is a p-type illustrating the effect of an internal heat exchanger. h diagram (Mollier diagram), FIG. 3 is a characteristic diagram showing the relationship of the cooling capacity to the dryness at the outlet of the use side heat exchanger, and FIG. 4 is a heat transfer coefficient (liquid side) with respect to the refrigerant mass flow rate of the internal heat exchanger. Fig. 5 is a characteristic diagram showing the relationship between the heat transfer rate, the gas side heat transfer rate, and the heat transfer rate. Fig. 5 is a ph diagram showing an enlarged portion from the inlet to the outlet on the low pressure side of the internal heat exchanger. 6 is a ph diagram representing the refrigeration cycle, and FIG. 7 is an action when the opening degree of the expansion mechanism of the low load side use unit is changed (cooling capacity and use side heat exchanger outlet overheating). It is a characteristic view showing the relationship between the degree of pressure and the low pressure side outlet superheat degree of the internal heat exchanger. In the drawings, the same or corresponding parts are denoted by the same reference numerals, and a part of the description is omitted.

(冷媒回路)
図1は、冷凍空調装置1000、熱源ユニット100と、並列に設置された利用ユニット200a、200bとを有し、両者が液延長配管3およびガス延長配管7によって環状に接続されている。熱源ユニット100は、圧縮機1と熱源側熱交換器2とよって構成されている。利用ユニット200a、200bは、それぞれ冷蔵室300a、300bに設置され、それぞれ、内部熱交換器4a、4b、膨張機構5a、5b、利用側熱交換器6a、6bによって構成されている。膨張機構5a、5bは、開度が可変に制御される電子膨張弁である。
(Refrigerant circuit)
FIG. 1 includes a refrigerating and air-conditioning apparatus 1000, a heat source unit 100, and utilization units 200a and 200b installed in parallel, and both are connected in an annular shape by a liquid extension pipe 3 and a gas extension pipe 7. The heat source unit 100 includes a compressor 1 and a heat source side heat exchanger 2. The usage units 200a and 200b are installed in the refrigerator compartments 300a and 300b, respectively, and are configured by internal heat exchangers 4a and 4b, expansion mechanisms 5a and 5b, and usage-side heat exchangers 6a and 6b, respectively. The expansion mechanisms 5a and 5b are electronic expansion valves whose opening degrees are variably controlled.

また、熱源側熱交換器2および利用側熱交換器6a、6bはファン、ポンプ等(図示せず)で供給される空気、水あるいはブライン等の流体(本発明において、「利用流体」と称す)との間で熱交換をする。なお、実施の形態1では、空気との間で熱交換するものを構成として説明するが、本発明は利用流体をこれに限定するものではない。
また、熱源ユニット100が1台に、利用ユニット200a、200bが2台を接続した場合について説明するが、3台以上の利用ユニットを接続した場合でも同様に実施できることは言うまでもない。なお、冷凍空調装置1000に用いられる冷媒は、例えば、R410A、R407C、R404AなどのHFC冷媒、R22、R134aなどのHCFC冷媒、もしくは炭化水素、ヘリウムのような自然冷媒などである。
The heat source side heat exchanger 2 and the use side heat exchangers 6a and 6b are fluids such as air, water or brine supplied by a fan, a pump or the like (not shown) (referred to as “use fluid” in the present invention). ) To exchange heat. In addition, although Embodiment 1 demonstrates as a structure what heat-exchanges between air, this invention does not limit a utilization fluid to this.
Moreover, although the case where the heat source unit 100 is connected to one unit and the two usage units 200a and 200b are connected will be described, it goes without saying that the same can be implemented even when three or more usage units are connected. The refrigerant used in the refrigerating and air-conditioning apparatus 1000 is, for example, an HFC refrigerant such as R410A, R407C, or R404A, an HCFC refrigerant such as R22 or R134a, or a natural refrigerant such as hydrocarbon or helium.

(センサー)
また、冷媒回路の圧力、温度を検出するセンサーとして、熱源ユニット100には、圧縮機1の吐出部の圧力を検出する吐出圧力センサー11と、圧縮機1の吸入部の圧力を検出する吸入圧力センサー12とが設置されている。
また、利用ユニット200a、200bには、それぞれ内部熱交換器4a、4bの低圧側出口における冷媒温度(以下、「内部熱交低圧出口温度」と称す)を検出する内部熱交低圧出口温度センサー13a、13bと、利用側熱交換器6a、6bの入口における冷媒温度(蒸発温度に同じ、以下、「利用側熱交入口温度」と称す)を検出する利用側熱交入口温度センサー14a、14bと、が設けられている。
さらに、冷蔵室300a、300bのそれぞれには、利用側熱交換器6a、6bに流入する利用流体(庫内空気に同じ)の温度を検出する吸込み空気温度センサー15a、15bと、利用温度(庫内空気の温度に同じ)が所望の温度になるよう設定する庫内温度設定手段24a、24bとが設けられている。
(sensor)
Further, as a sensor for detecting the pressure and temperature of the refrigerant circuit, the heat source unit 100 includes a discharge pressure sensor 11 for detecting the pressure of the discharge portion of the compressor 1 and a suction pressure for detecting the pressure of the suction portion of the compressor 1. A sensor 12 is installed.
The utilization units 200a and 200b include an internal heat exchanger low-pressure outlet temperature sensor 13a that detects a refrigerant temperature at the low-pressure outlet of each of the internal heat exchangers 4a and 4b (hereinafter referred to as “internal heat exchanger low-pressure outlet temperature”). , 13b, and utilization side heat exchange inlet temperature sensors 14a, 14b for detecting refrigerant temperatures at the inlets of the utilization side heat exchangers 6a, 6b (same as the evaporation temperature, hereinafter referred to as “use side heat exchange inlet temperature”); , Is provided.
Furthermore, in each of the refrigerator compartments 300a and 300b, suction air temperature sensors 15a and 15b for detecting the temperature of the use fluid (same as the inside air) flowing into the use side heat exchangers 6a and 6b, and a use temperature (warehouse). In-chamber temperature setting means 24a and 24b are set so as to set the desired temperature to be the same as the temperature of the internal air.

(計測制御装置)
そして、熱源ユニット100内には、前記各センサーや、庫内温度設定手段24a、24bおよび膨張機構5a、5bに接続された計測制御装置20が設置されている。
計測制御装置20には、前記各センサーによって検出された各箇所における計測情報(圧力および温度)や、使用者が設定した設定情報(庫内設定温度および運転内容)が入力され、かかる計測情報や設定情報に基づいて、圧縮機1の運転方法、熱源側熱交換器2や利用側熱交換器6a、6bに向けて送風する各ファンの送風量、および膨張機構5a、5bの開度などの制御信号が出力される。
(Measurement control device)
In the heat source unit 100, the measurement control device 20 connected to the sensors, the internal temperature setting means 24a and 24b, and the expansion mechanisms 5a and 5b is installed.
The measurement control device 20 receives measurement information (pressure and temperature) at each location detected by each sensor and setting information (in-house set temperature and operation details) set by the user. Based on the setting information, such as the operation method of the compressor 1, the air flow rate of each fan blown toward the heat source side heat exchanger 2 and the use side heat exchangers 6a and 6b, and the opening degrees of the expansion mechanisms 5a and 5b, etc. A control signal is output.

なお、計測制御装置20は、前記のような制御装置として機能するだけではなく、冷媒状態量演算手段21、目標冷媒状態量演算手段22、および補正手段23の演算処理部としての機能を果たす(但し、図1においては、これらが内蔵されているかのように便宜上記載されている。   The measurement control device 20 not only functions as the control device as described above, but also functions as a calculation processing unit of the refrigerant state quantity calculation means 21, the target refrigerant state quantity calculation means 22, and the correction means 23 ( However, in FIG. 1, they are described for convenience as if they were incorporated.

(冷媒状態量演算手段)
冷媒状態量演算手段21は、内部熱交低圧出口温度センサー13a、13b、利用側熱交入口温度センサー14a、14bおよび計測制御装置20から構成されており、内部熱交低圧出口温度センサー13a、13b、利用側熱交入口温度センサー14a、14bの出力に基づいて内部熱交換器4a、4b出口の過熱度を求める。なお、冷媒状態量演算手段21の演算処理についての詳細は後述する。
(Refrigerant state quantity calculation means)
The refrigerant state quantity calculation means 21 includes internal heat exchange low-pressure outlet temperature sensors 13a and 13b, use side heat exchange inlet temperature sensors 14a and 14b, and a measurement control device 20, and the internal heat exchange low-pressure outlet temperature sensors 13a and 13b. The degree of superheat at the outlets of the internal heat exchangers 4a and 4b is obtained based on the outputs of the use side heat exchange inlet temperature sensors 14a and 14b. Details of the calculation process of the refrigerant state quantity calculation means 21 will be described later.

(目標冷媒状態量演算手段)
目標冷媒状態量演算手段22は、吸込み空気温度センサー15a、15b、庫内温度設定手段24a、24bおよび計測制御装置20から構成されており、吸込み空気温度センサー15a、15bの検出した温度と、庫内温度設定手段24a、24bの設定した温度との偏差と、冷媒状態量演算手段21の結果とに基づいて目標冷媒状態量を設定する。なお、目標冷媒状態量演算手段22の演算処理についての詳細は後述する。
(Target refrigerant state quantity calculation means)
The target refrigerant state quantity calculation means 22 is composed of intake air temperature sensors 15a and 15b, internal temperature setting means 24a and 24b, and a measurement control device 20, and the temperatures detected by the intake air temperature sensors 15a and 15b, The target refrigerant state quantity is set based on the deviation from the temperature set by the internal temperature setting means 24a, 24b and the result of the refrigerant state quantity calculating means 21. Details of the calculation process of the target refrigerant state quantity calculation means 22 will be described later.

(補正手段)
補正手段23は、膨張機構5a、5bおよび計測制御装置20から構成されており、膨張機構5a、5bの開度と冷媒状態量演算手段21の結果とに基づいて、膨張機構5a、5bの全閉開度を補正する。なお、補正手段23の演算処理についての詳細は後述する。
(Correction means)
The correction unit 23 includes the expansion mechanisms 5a and 5b and the measurement control device 20. Based on the opening degree of the expansion mechanisms 5a and 5b and the result of the refrigerant state quantity calculation unit 21, all of the expansion mechanisms 5a and 5b are corrected. Correct the opening. The details of the calculation process of the correction means 23 will be described later.

なお、図1では熱源ユニット100が1台に、並列配置された利用ユニット200a、200bが2台を接続した場合について説明するが、3台以上の利用ユニットを接続した場合でも同様に実施できることは言うまでもない。また、冷凍空調装置1000に用いられる冷媒は、例えば、R410A、R407C、R404AなどのHFC冷媒、R22、R134aなどのHCFC冷媒、もしくは炭化水素、ヘリウムのような自然冷媒などがある。   In addition, although FIG. 1 demonstrates the case where the heat source unit 100 is connected to one unit and two usage units 200a and 200b arranged in parallel are connected, it can be similarly implemented even when three or more usage units are connected. Needless to say. The refrigerant used in the refrigerating and air-conditioning apparatus 1000 includes, for example, HFC refrigerants such as R410A, R407C, and R404A, HCFC refrigerants such as R22 and R134a, or natural refrigerants such as hydrocarbon and helium.

(内部熱交換器が無い場合の運転動作)
次に、冷凍空調装置1000の内部熱交換器4a、4bの有無による運転動作の違いをp−h線図(モリエル線図)に基づいて説明する。
図2の(a)において、内部熱交換器4a、4bが無い場合、圧縮機1から吐出された高圧高温のガス冷媒(状態B0、以下「高圧高温冷媒」と称す)は熱源側熱交換器2に流入し、ここで放熱しながら凝縮液化し、高圧中温の冷媒となる(状態C0、以下「高圧中温冷媒」と称す)。
そして、熱源側熱交換器2を出た冷媒は、液延長配管3を通り、利用ユニット200a、200bへ分流され、それぞれ膨張機構5a、5bにおいて低圧まで減圧され二相冷媒となる(状態D0、以下「低圧低温冷媒」と称す)。その後、利用側熱交換器6a、6bに流入し、そこで吸熱し、蒸発ガス化しながら利用流体(空気や水などの負荷側媒体)に冷熱を供給する(状態A0、以下「低圧中温冷媒」と称す)。
(Driving operation without internal heat exchanger)
Next, the difference of the driving | operation operation | movement by the presence or absence of the internal heat exchangers 4a and 4b of the refrigerating and air-conditioning apparatus 1000 is demonstrated based on a ph diagram (Mollier diagram).
In FIG. 2A, when there are no internal heat exchangers 4a and 4b, the high-pressure and high-temperature gas refrigerant discharged from the compressor 1 (state B0, hereinafter referred to as “high-pressure and high-temperature refrigerant”) is a heat source side heat exchanger. 2 is condensed and liquefied while dissipating heat to become a high-pressure medium-temperature refrigerant (state C0, hereinafter referred to as “high-pressure medium-temperature refrigerant”).
Then, the refrigerant that has exited the heat source side heat exchanger 2 passes through the liquid extension pipe 3 and is divided into use units 200a and 200b, and is decompressed to a low pressure in the expansion mechanisms 5a and 5b, respectively, to become a two-phase refrigerant (state D0, Hereinafter referred to as “low pressure low temperature refrigerant”). After that, it flows into the use side heat exchangers 6a and 6b, absorbs heat there, and supplies cold energy to the use fluid (load side medium such as air or water) while evaporating gas (state A0, hereinafter referred to as “low pressure medium temperature refrigerant”) Called).

冷媒の熱伝達率は、一般的に、ガス冷媒よりも二相冷媒の方が高いため、熱交換性能が向上し、冷凍空調装置の性能が向上する。
また、圧縮機1が吸入する低圧中温冷媒(吸入冷媒に同じ)は、圧縮機1が液圧縮を原因とする圧縮機故障によって損傷することを防止するため、「正値」となるように膨張機構5a、5bにおける流量を調整する必要がある。
内部熱交換器4a、4bが無い場合は、利用側熱交換器6a、6bの出口における「過熱度SHe(飽和ガス線との交点である状態E0と、状態A0との温度差)」を図2の(a)に示すように、例えば「SHe=5℃」を制御目標として膨張機構5a、5bの開度を制御する。
Since the heat transfer coefficient of the refrigerant is generally higher in the two-phase refrigerant than in the gas refrigerant, the heat exchange performance is improved and the performance of the refrigeration air conditioner is improved.
Further, the low-pressure intermediate temperature refrigerant (same as the intake refrigerant) sucked by the compressor 1 expands to become “positive value” in order to prevent the compressor 1 from being damaged due to a compressor failure caused by liquid compression. It is necessary to adjust the flow rate in the mechanisms 5a and 5b.
When the internal heat exchangers 4a and 4b are not provided, the “superheat degree SHe (temperature difference between the state E0 that is an intersection with the saturated gas line and the state A0)” at the outlets of the use side heat exchangers 6a and 6b is illustrated. As shown in (a) of 2, for example, the opening degree of the expansion mechanisms 5a and 5b is controlled with “SHe = 5 ° C.” as a control target.

このとき、「庫内温度RT」と「蒸発温度Te」との温度差を「利用温度差TD」とすると、「TD>SHe」の関係がある。
このため、蒸発温度Teは庫内温度RTよりも少なくとも過熱度SHeだけ低温になる。すなわち、庫内温度RT=−30℃、過熱度SHe=5℃、のとき、蒸発温度Teは−35(=−30−5)℃以下の温度となる。図2の(a)には、利用温度差TD=10℃として、蒸発温度Te=−40(−30−10)℃を示している。
At this time, if the temperature difference between “internal temperature RT” and “evaporation temperature Te” is “utilization temperature difference TD”, there is a relationship of “TD> SHe”.
For this reason, the evaporation temperature Te is lower than the internal temperature RT by at least the degree of superheat SHe. That is, when the internal temperature RT = −30 ° C. and the superheat degree SHe = 5 ° C., the evaporation temperature Te is a temperature of −35 (= −30−5) ° C. or lower. FIG. 2 (a) shows the evaporation temperature Te = −40 (−30−10) ° C. with the use temperature difference TD = 10 ° C.

さらに、利用側熱交換器6a、6bを出た低圧中温冷媒は合流し、ガス延長配管7を通り、圧縮機1に吸入される。したがって、状態A0、状態B0、状態C0および状態D0を順次経由して、再度状態A0に戻る冷凍サイクル(冷媒が循環回路)が形成される。
図2の(b)において、内部熱交換器4a、4bが無い場合は、利用側熱交換器6a、6b内の冷媒の状態変化は、利用側熱交換器6a、6bの出口において過熱度が確保されるように膨張機構5a、5bの開度を調整し制御される。このため、利用側熱交換器6a、6bの一部が過熱ガスになる。
Further, the low-pressure and medium-temperature refrigerants that have exited from the use side heat exchangers 6 a and 6 b join together and are sucked into the compressor 1 through the gas extension pipe 7. Therefore, a refrigeration cycle (refrigerant is a circulation circuit) that returns to state A0 again through state A0, state B0, state C0, and state D0 is formed.
In FIG. 2B, when there is no internal heat exchanger 4a, 4b, the state change of the refrigerant in the use side heat exchangers 6a, 6b is caused by the degree of superheat at the outlets of the use side heat exchangers 6a, 6b. The opening degree of the expansion mechanisms 5a and 5b is adjusted and controlled so as to be secured. For this reason, a part of utilization side heat exchanger 6a, 6b becomes superheated gas.

(内部熱交換器が有る場合の運転動作)
図2の(c)において、内部熱交換器4a、4bが有る場合、熱源側熱交換器2において冷却された冷媒(以下、「高圧中温冷媒」と称す)は、利用ユニット200a、200bのそれぞれに分流された後、内部熱交換器4a、4bにおいて、利用側熱交換器6a、6bにおいて蒸発した冷媒(以下、「低圧低温冷媒」と称す)と熱交換をし(冷熱を受け取り)、冷却される(状態C1)。
そして、膨張機構5a、5bにおいて断熱膨張した低圧冷温冷媒(状態D1)は、利用側熱交換器6a、6bに流入し、蒸発して低圧中温の冷媒となる(状態E1)。さらに、内部熱交換器4a、4bにおいて高圧中温冷媒と熱交換をし(温熱を受け取り)、加熱される(状態A1)。
(Operations when there is an internal heat exchanger)
In FIG. 2C, when there are internal heat exchangers 4a and 4b, the refrigerant cooled in the heat source side heat exchanger 2 (hereinafter referred to as “high pressure / intermediate temperature refrigerant”) is used in each of the usage units 200a and 200b. Then, in the internal heat exchangers 4a and 4b, heat is exchanged with the refrigerant evaporated in the use side heat exchangers 6a and 6b (hereinafter referred to as “low-pressure low-temperature refrigerant”) (cooling is received), and cooling is performed. (State C1).
The low-pressure cold / warm refrigerant (state D1) adiabatically expanded in the expansion mechanisms 5a, 5b flows into the use-side heat exchangers 6a, 6b and evaporates to become low-pressure medium-temperature refrigerant (state E1). Further, the internal heat exchangers 4a and 4b exchange heat with the high-pressure intermediate-temperature refrigerant (receive the heat) and are heated (state A1).

ここで、内部熱交換器4a、4bが有る場合は、内部熱交換器4a、4bの出口における低圧中温冷媒の「過熱度SHL」を、例えば「SHL=5℃」に制御する。このとき、利用側熱交換器6a、6bの出口における低圧中温冷媒の過熱度は「過熱度SHL」よりも小さくなり、飽和ガスに近い状態を実現できる。
したがって、蒸発温度Teは庫内温度RT−0℃以下、つまり、蒸発温度Teを庫内温度近くまで上昇するため、低圧圧力が上昇し、冷凍サイクル上、高効率な運転が実現できる。また、冷凍空調装置1000が冷凍倉庫のような蒸発温度Teが氷点下(0℃以下)となるような環境で使用される場合は、利用側熱交換器6a、6bに着霜が発生するが、内部熱交換器4a、4bによって蒸発温度Teが上昇するため、着霜量が低減し、ヒータ等による除霜に必要なエネルギーを低減することが可能になる。
Here, when there are the internal heat exchangers 4a and 4b, the “superheat degree SHL” of the low-pressure intermediate temperature refrigerant at the outlet of the internal heat exchangers 4a and 4b is controlled to, for example, “SHL = 5 ° C.”. At this time, the superheat degree of the low-pressure intermediate temperature refrigerant at the outlets of the use side heat exchangers 6a and 6b becomes smaller than the “superheat degree SHL”, and a state close to saturated gas can be realized.
Therefore, the evaporating temperature Te is equal to or lower than the internal temperature RT-0 ° C., that is, the evaporating temperature Te is increased to near the internal temperature, so that the low-pressure pressure is increased, and a highly efficient operation can be realized on the refrigeration cycle. In addition, when the refrigeration air conditioner 1000 is used in an environment where the evaporation temperature Te is below freezing (0 ° C. or lower) as in a refrigerated warehouse, frost formation occurs on the use side heat exchangers 6a and 6b. Since the evaporating temperature Te is increased by the internal heat exchangers 4a and 4b, the amount of frost formation is reduced, and the energy required for defrosting by a heater or the like can be reduced.

また、内部熱交換器4a、4bにおいて、高圧中温冷媒は冷却されることで、エンタルピーが低下し、「過冷却度SC(飽和ガス線との交点である状態C0と、状態C1との温度差)」が増加する。このため、冷凍効果が増加し、同一冷却能力を発揮するために必要な冷媒循環量を低減することができるから、圧縮機の運転容量の低減によって高効率な運転を実現することができる。   In addition, in the internal heat exchangers 4a and 4b, the high-pressure intermediate temperature refrigerant is cooled, so that the enthalpy is reduced, and “the degree of supercooling SC (the temperature difference between the state C0 that is the intersection with the saturated gas line and the state C1). ) "Increases. For this reason, since the refrigerating effect is increased and the refrigerant circulation amount necessary for exhibiting the same cooling capacity can be reduced, a highly efficient operation can be realized by reducing the operating capacity of the compressor.

図2の(d)において、内部熱交換器4a、4bが有る場合は、内部熱交換器4a、4bの出口において過熱度が確保されるように膨張機構5a、5bの開度を調整し制御すれば、利用側熱交換器6a、6b内全体が二相となる冷媒状態を実現することができる。   In FIG. 2D, when there are internal heat exchangers 4a and 4b, the opening degree of the expansion mechanisms 5a and 5b is adjusted and controlled so that the degree of superheat is secured at the outlets of the internal heat exchangers 4a and 4b. By doing so, it is possible to realize a refrigerant state in which the entire use side heat exchangers 6a and 6b are in two phases.

(膨張機構の制御方法)
次に、内部熱交換器4a、4bを搭載した冷媒回路における、膨張機構5a、5bの制御方法について説明する。膨張機構5a、5bは、内部熱交低圧出口温度センサー13a、13bで検知される「内部熱交低圧出口温度(状態A1)」と利用側熱交入口温度センサー14a、14bで検知される「低圧低温冷媒の飽和温度(状態E1)」との差温である「内部熱交換器出口の過熱度SHL」が予め設定された「制御目標値SHLm」、例えば、「SHLm=5℃」になるように制御される。
過熱度SHLが制御目標値SHLmより大きい(SHL>SHLm)場合には、膨張機構5a、5bの開度は大きく、反対に、過熱度SHLが制御目標値SHLmより小さい(SHL>SHLm)場合には、膨張機構5a、5bの開度は小さく制御される。
(Expansion mechanism control method)
Next, a method for controlling the expansion mechanisms 5a and 5b in the refrigerant circuit equipped with the internal heat exchangers 4a and 4b will be described. The expansion mechanisms 5a and 5b are connected to the "internal heat exchanger low pressure outlet temperature (state A1)" detected by the internal heat exchanger low pressure outlet temperature sensors 13a and 13b and "low pressure" detected by the use side heat exchanger inlet temperature sensors 14a and 14b. The “superheat degree SHL at the outlet of the internal heat exchanger”, which is a temperature difference from the saturation temperature of the low-temperature refrigerant (state E1), becomes a preset “control target value SHLm”, for example, “SHLm = 5 ° C.” Controlled.
When the degree of superheat SHL is larger than the control target value SHLm (SHL> SHLm), the opening degree of the expansion mechanisms 5a and 5b is large, and conversely, when the degree of superheat SHL is smaller than the control target value SHLm (SHL> SHLm). The opening degree of the expansion mechanisms 5a and 5b is controlled to be small.

すなわち、膨張機構5a、5bの制御目標である、冷媒過熱度の目標値が、内部熱交換器4a、4bでの熱交換によって生じる冷媒過熱度よりも大きく設定された場合には、利用側熱交換器6a、6bの出口冷媒状態は「乾き度x」が1よりも大きい過熱ガス状態(x>1.0))となり、性能の低下が生じる。
反対に、冷媒過熱度の目標値が小さく設定された場合には、利用側熱交換器6a、6bの出口における冷媒状態は乾き度xが1以下の二相状態(x<1.0)となる。
That is, when the target value of the refrigerant superheat degree, which is the control target of the expansion mechanisms 5a and 5b, is set larger than the refrigerant superheat degree generated by the heat exchange in the internal heat exchangers 4a and 4b, the use side heat The outlet refrigerant state of the exchangers 6a and 6b becomes a superheated gas state (x> 1.0) in which “dryness x” is greater than 1, and performance is deteriorated.
On the other hand, when the target value of the refrigerant superheat degree is set to be small, the refrigerant state at the outlet of the use side heat exchangers 6a and 6b is a two-phase state (x <1.0) with a dryness x of 1 or less. Become.

図3に示す利用側熱交換器6a、6bの出口における乾き度と冷却能力の関係において、利用側熱交換器6a、6bの出口における冷媒状態が「乾き度xが1以下の二相(x<1.0)」となる場合、冷却能力は最大となる。このため、冷凍サイクルの高効率化の観点より、内部熱交換量に応じて、利用側熱交換器6a、6bの出口における冷媒状態が「乾き度xが1以下」となる様に、冷媒過熱度の目標値を設定することが望ましい。
この冷凍サイクルにおいて、内部熱交換器4a、4bの出口における過熱度SHLは、内部熱交換器4a、4bにおける高圧中温冷媒との熱交換によって生じるものであるため、熱交換量に応じて変化する。
In the relationship between the dryness and the cooling capacity at the outlets of the use side heat exchangers 6a and 6b shown in FIG. 3, the refrigerant state at the outlet of the use side heat exchangers 6a and 6b is “two-phase (x <1.0) ", the cooling capacity is maximized. For this reason, from the viewpoint of increasing the efficiency of the refrigeration cycle, the refrigerant is overheated so that the refrigerant state at the outlets of the use side heat exchangers 6a and 6b becomes “dryness x is 1 or less” according to the internal heat exchange amount. It is desirable to set a target value for the degree.
In this refrigeration cycle, the degree of superheat SHL at the outlets of the internal heat exchangers 4a and 4b is generated by heat exchange with the high-pressure medium-temperature refrigerant in the internal heat exchangers 4a and 4b, and thus changes according to the amount of heat exchange. .

(内部熱交換器の温度効率)
次に、内部熱交換器4a、4bの温度効率εについて説明する。内部熱交換器の温度効率は一般的に(式1)で定義できる。また、(式2)でも表すことができ、(式2)における熱通過率Kは(式3)にて示される。
(Temperature efficiency of internal heat exchanger)
Next, the temperature efficiency ε of the internal heat exchangers 4a and 4b will be described. The temperature efficiency of the internal heat exchanger can generally be defined by (Equation 1). Also, it can be expressed by (Expression 2), and the heat transmission rate K in (Expression 2) is expressed by (Expression 3).

Figure 2011220559
Figure 2011220559

ここで、
TLO:内部熱交低圧側出口温度、
TLI:内部熱交低圧側入口温度、
THI:内部熱交高圧入口温度、
A :内部熱交換器において高圧中温冷媒と低圧中温冷媒とが熱交換を行う伝熱面積
[m2]、
K :内部熱交換器の熱通過率[kW/m2K]、
Gr :低圧ガス冷媒の冷媒循環量[kg/s]、
Cpg:低圧側の定圧ガス比熱[kJ/kgK]、である。
here,
TLO: Internal heat exchange low pressure side outlet temperature,
TLI: Internal heat exchange low pressure side inlet temperature,
THI: Internal heat exchange high pressure inlet temperature,
A: Heat transfer area in which heat exchange is performed between the high-pressure intermediate temperature refrigerant and the low-pressure intermediate temperature refrigerant in the internal heat exchanger
[m2],
K: heat passage rate of internal heat exchanger [kW / m2K],
Gr: refrigerant circulation amount of low-pressure gas refrigerant [kg / s],
Cpg: constant-pressure gas specific heat [kJ / kgK] on the low-pressure side.

すなわち、(式3)に示されるように熱通過率Kは、高圧液側熱伝達率α1[kW/m2K]、低圧ガス側熱伝達率αg[kW/m2K]、内部熱交換器の伝熱面の厚さL[m]、伝熱面の熱伝導率λ[kW/mK]によって定義される。
図4において、熱通過率Kは冷媒循環量Grに対して、略比例関係となる。すなわち、K/Grの値は一定となる。定圧ガス比熱は、庫内の使用環境条件が同じであれば、蒸発温度Teが略一定となるため、一定値と仮定することができる。また、伝熱面積Aは内部熱交換器の仕様によって決まるものであるため一定値である、したがって、(式2)の温度効率εは、常に一定値となる。
That is, as shown in (Equation 3), the heat transfer rate K includes the high pressure liquid side heat transfer rate α1 [kW / m2K], the low pressure gas side heat transfer rate αg [kW / m2K], and the heat transfer rate of the internal heat exchanger. It is defined by the thickness L [m] of the surface and the thermal conductivity λ [kW / mK] of the heat transfer surface.
In FIG. 4, the heat passage rate K is substantially proportional to the refrigerant circulation amount Gr. That is, the value of K / Gr is constant. The constant-pressure gas specific heat can be assumed to be a constant value because the evaporation temperature Te is substantially constant if the use environment conditions in the storage are the same. Further, since the heat transfer area A is determined by the specifications of the internal heat exchanger, it is a constant value. Therefore, the temperature efficiency ε in (Equation 2) is always a constant value.

(飽和ガスになる状態)
ここで、冷凍空調装置1000の高効率運転を実現することができる利用側熱交換器6a、6bの出口における「乾き度xが1の飽和ガス」になっている場合の状態について説明する。
(式1)において、THIは、内部熱交換器4a、4bの高圧側入口における高圧中温冷媒の温度(内部熱交高圧入口温度)であるが、これは、吐出圧力センサー11から換算される飽和温度にほぼ等しい。また、TLIは、内部熱交換器4a、4bの低圧側入口における低圧中温冷媒の温度(内部熱交低圧側入口温度)であるが、利用側熱交換器6a、6bの出口における「乾き度xが1」であるため、利用側熱交入口温度センサー14a、14bによって検出される飽和温度と等しくなる。
(Saturated gas state)
Here, the state in the case where “the dryness x is a saturated gas of 1” at the outlets of the use side heat exchangers 6a and 6b capable of realizing the highly efficient operation of the refrigeration air conditioner 1000 will be described.
In (Expression 1), THI is the temperature of the high-pressure intermediate temperature refrigerant (internal heat exchange high-pressure inlet temperature) at the high-pressure side inlets of the internal heat exchangers 4a and 4b, and this is the saturation converted from the discharge pressure sensor 11. Approximately equal to temperature. TLI is the temperature of the low-pressure intermediate temperature refrigerant at the low-pressure side inlets of the internal heat exchangers 4a and 4b (internal heat exchange low-pressure side inlet temperature), but the “dryness x” at the outlets of the use-side heat exchangers 6a and 6b. Is equal to 1 ”, which is equal to the saturation temperature detected by the use side heat exchange inlet temperature sensors 14a and 14b.

以上から、温度効率εは一定であるため、冷凍サイクル装置付属の圧力、温度情報から内部熱交換器の低圧側の温度変化量ΔSH(=TLO-TLI)を(式4)を用いて算出することができる。   From the above, since the temperature efficiency ε is constant, the temperature change amount ΔSH (= TLO−TLI) on the low pressure side of the internal heat exchanger is calculated using (Expression 4) from the pressure and temperature information attached to the refrigeration cycle apparatus. be able to.

Figure 2011220559
Figure 2011220559

図5に示すように、利用側熱交換器6a、6bの出口の過熱度を「SHe」とし、内部熱交換器4a、4bの低圧側出口の過熱度を「低圧側出口過熱度SHL」とした場合、低圧側出口過熱度SHLの制御目標値を「制御目標値ΔSH」になるように制御すれば、利用側熱交換器6a、6bの冷却能力を最大に発揮させることができ、効率の高い運転を実現することができる。
なお、図5では、「SHL>ΔSH」となっているため、利用側熱交換器6a、6bの出口における過熱度SHeを0(ゼロ)にするためには、膨張機構5a、5bの開度を開けばよいことになる。
As shown in FIG. 5, the superheat degree of the outlets of the use side heat exchangers 6a and 6b is “SHe”, and the superheat degree of the low pressure side outlets of the internal heat exchangers 4a and 4b is “low pressure side outlet superheat degree SHL”. In this case, if the control target value of the low pressure side outlet superheat degree SHL is controlled to be “control target value ΔSH”, the cooling capacity of the use side heat exchangers 6a and 6b can be maximized, and the efficiency can be improved. High driving can be realized.
In FIG. 5, since “SHL> ΔSH” is satisfied, in order to set the superheat degree SHe at the outlets of the use side heat exchangers 6a and 6b to 0 (zero), the opening degrees of the expansion mechanisms 5a and 5b. You can open it.

(利用ユニットの負荷が相違する場合)
次に、本発明の特徴である、利用ユニットが複数台ある場合において、それぞれの利用液体(冷却対象)の冷却負荷が異なる場合の制御方法について図6、図7を用いて説明する。ここでは、便宜上、利用ユニット200aに対して、利用ユニット200bの冷却対象の負荷が小さい場合の運転状態を想定して説明する。
(When the load on the used unit is different)
Next, a control method in the case where there are a plurality of utilization units, which is a feature of the present invention, and the cooling load of each utilization liquid (cooling target) is different will be described with reference to FIGS. Here, for the sake of convenience, a description will be given assuming an operating state when the load to be cooled of the usage unit 200b is small with respect to the usage unit 200a.

まず、熱源側熱交換器2を出て、液延長配管3を通過した高圧中温冷媒は、分流され、利用ユニット200a、200bにそれぞれ流入する。低圧圧力はそれぞれ等しいため、冷却負荷が大きい利用ユニット200a側は最大冷却能力を発揮する必要があるため、膨張機構5aの開度を制御し、内部熱交換器4aの出口の過熱度SHLaを制御目標値ΔSHになるよう(SHLa≒ΔSH)に制御すればよい。
一方、冷却負荷の小さい利用ユニット200bは、冷却能力を減少させるために、内部熱交換器4bの出口における過熱度SHLbが制御目標値ΔSH以上(SHLa>ΔSH)になるように制御し、膨張機構5bの開度を絞り、冷媒循環量を低下させ冷却能力を低下させればよい。
First, the high-pressure intermediate temperature refrigerant that has exited the heat source side heat exchanger 2 and passed through the liquid extension pipe 3 is divided and flows into the utilization units 200a and 200b, respectively. Since the low pressures are equal, the use unit 200a side with a large cooling load needs to exhibit the maximum cooling capacity, so the degree of superheat SHLa at the outlet of the internal heat exchanger 4a is controlled by controlling the opening of the expansion mechanism 5a. The target value ΔSH may be controlled (SHLa≈ΔSH).
On the other hand, in order to reduce the cooling capacity, the utilization unit 200b having a small cooling load controls the superheat degree SHLb at the outlet of the internal heat exchanger 4b to be equal to or greater than the control target value ΔSH (SHLa> ΔSH), thereby expanding the expansion mechanism. What is necessary is just to restrict | squeeze the opening degree of 5b, to reduce a refrigerant | coolant circulation amount, and to reduce cooling capacity.

ここで、冷却負荷の大小は、庫内温度設定手段24a、24bにて設定される温度に対する、現在の吸込み空気温度センサー15a、15bにて検知される温度によって決定される。例えば、庫内設定温度に対して吸込み空気温度が大きい場合は、冷却負荷が大きく、その偏差量が大きいほど負荷が大きい。   Here, the magnitude of the cooling load is determined by the temperature detected by the current intake air temperature sensors 15a and 15b with respect to the temperature set by the internal temperature setting means 24a and 24b. For example, when the intake air temperature is higher than the internal set temperature, the cooling load is large, and the larger the deviation amount, the larger the load.

(冷却能力を小さくする制御方法)
次に、冷却能力を小さくする制御方法について、図7を用いて説明する。図7は利用ユニット200bの冷却能力に対する、膨張機構5bの開度、利用側熱交換器出口過熱度SHe、および内部熱交換器出口過熱度SHLの関係を示したものである。
図7より、膨張機構5bの開度を小さくし、冷媒流量を低下させれば、冷却能力が小さくなることがわかる。冷却能力は、利用側熱交換器出口過熱度SHeが0(ゼロ)の時に冷却能力が最大となり、利用側熱交換器出口過熱度SHeの増加とともに冷却能力が低下する。
(Control method to reduce cooling capacity)
Next, a control method for reducing the cooling capacity will be described with reference to FIG. FIG. 7 shows the relationship of the opening degree of the expansion mechanism 5b, the use side heat exchanger outlet superheat degree SHe, and the internal heat exchanger outlet superheat degree SHL with respect to the cooling capacity of the use unit 200b.
From FIG. 7, it can be seen that if the opening of the expansion mechanism 5b is reduced and the refrigerant flow rate is reduced, the cooling capacity is reduced. The cooling capacity is maximized when the utilization side heat exchanger outlet superheat degree SHe is 0 (zero), and the cooling capacity decreases as the utilization side heat exchanger outlet superheat degree SHe increases.

この利用側熱交換器出口過熱度SHeの上限値は図6で示した「利用温度差TD=庫内温度RT−蒸発温度Te」となる。また、内部熱交換器出口過熱度SHLは「SHL=SHe+ΔSH」の関係を満たして変化するが、冷却能力が0(ゼロ)、すなわち、冷媒循環量が殆ど流れていない状態では、温度効率εが1に近くなるため、(式3)より、内部熱交低圧側出口温度TLOは内部熱交高圧側入口温度THIまで上昇する。したがって、内部熱交換器出口過熱度SHLの上限値は図で示した「利用温度差TD=内部熱交高圧側入口温度THI−蒸発温度Te」となる。   The upper limit value of the use side heat exchanger outlet superheat degree She is “use temperature difference TD = internal temperature RT−evaporation temperature Te” shown in FIG. In addition, the internal heat exchanger outlet superheat degree SHL changes while satisfying the relationship of “SHL = SHe + ΔSH”, but in the state where the cooling capacity is 0 (zero), that is, the refrigerant circulation amount hardly flows, the temperature efficiency Since ε is close to 1, the internal heat exchanger low pressure side outlet temperature TLO rises to the internal heat exchanger high pressure side inlet temperature THI from (Equation 3). Therefore, the upper limit value of the internal heat exchanger outlet superheat degree SHL is “utilization temperature difference TD = internal heat exchange high pressure side inlet temperature THI−evaporation temperature Te” shown in the figure.

このように、内部熱交換器6a、6bの出口における過熱度SHLに応じて冷却能力を制御することが可能となるため、最大冷却能力に対する要求冷却能力比をQR[%]とすると、過熱度SHLの目標過熱度SHLmは(式5)で定義し、その過熱度を目標に制御すれば冷却能力を冷却負荷に応じて制御することができる。   Thus, since it becomes possible to control cooling capacity according to superheat degree SHL in the exit of internal heat exchanger 6a, 6b, when the required cooling capacity ratio with respect to maximum cooling capacity is set to QR [%], superheat degree The SHL target superheat degree SHLm is defined by (Equation 5), and if the superheat degree is controlled to the target, the cooling capacity can be controlled according to the cooling load.

Figure 2011220559
Figure 2011220559

また、図7から分かるように膨張機構5bの開度が閉塞に近い状態になった場合は、「SHL>TD+ΔSH」の関係が成り立つため、計測制御装置20の指令開度において、「SHL>TD+ΔSH」の関係を満たした場合は、膨張機構5bの開口率が閉塞する開度であるとすることができる。
したがって、そのような条件を満たした膨張機構5bの開度SJを「閉塞開度SJmin」として記憶しておけば、冷却能力が0(ゼロ)となる開度は閉塞開度SJminである。そして、冷却能力は、冷媒循環量すなわち開度に比例するので、現在の冷却能力に対して、冷却能力比を要求冷却能力比QR[%]にしたい場合は、現在の膨張機構の開度SJnowに対して(式6)で定義した開度SJに設定すればよい。
Further, as can be seen from FIG. 7, when the opening degree of the expansion mechanism 5b is close to closing, the relationship of “SHL> TD + ΔSH” is established, and therefore, the command opening degree of the measurement control device 20 is “SHL”. When the relationship of “> TD + ΔSH” is satisfied, the opening ratio of the expansion mechanism 5b can be determined to be an opening degree that closes.
Therefore, if the opening degree SJ of the expansion mechanism 5b satisfying such a condition is stored as “closing opening degree SJmin”, the opening degree at which the cooling capacity becomes 0 (zero) is the closing opening degree SJmin. Since the cooling capacity is proportional to the refrigerant circulation amount, that is, the opening degree, when it is desired to set the cooling capacity ratio to the required cooling capacity ratio QR [%] with respect to the current cooling capacity, the opening degree SJnow of the current expansion mechanism. On the other hand, the opening degree SJ defined by (Equation 6) may be set.

Figure 2011220559
Figure 2011220559

膨張機構5a、5bの閉塞開度SJminは、製品バラツキがあるため、あらかじめ所定の値を入れておき、過熱度が「SHL>TD+ΔSH」の条件を満たした時の開度をSJminとして、補正することによって、製品バラツキを排除した冷却能力の制御性の高い運転が実現できる。   Since the closing opening SJmin of the expansion mechanisms 5a and 5b has a product variation, a predetermined value is set in advance, and the opening when the superheat degree satisfies the condition of “SHL> TD + ΔSH” is SJmin. By correcting, it is possible to realize an operation with high controllability of cooling capacity that eliminates product variations.

以上のように、本実施の形態1によれば、利用側熱交換器6a、6bの出口における低圧中温冷媒の過熱度の状態によって膨張機構5a、5bを制御することにより、冷却対象の負荷が大きい場合は、高効率な運転を行い、負荷が小さい場合は、冷却能力を負荷に合わせた運転が可能となる。このため、頻繁な発停を防止することで、冷却対象の設定温度に対する温度変動を小さく抑え、制御性の高い運転を実現することができる冷凍空調装置1000を得ることができる。   As described above, according to the first embodiment, by controlling the expansion mechanisms 5a and 5b according to the degree of superheat of the low-pressure intermediate temperature refrigerant at the outlets of the use side heat exchangers 6a and 6b, the load to be cooled is reduced. When the load is large, high-efficiency operation is performed, and when the load is small, the cooling capacity can be adjusted to the load. For this reason, by preventing frequent start / stop, it is possible to obtain a refrigeration air conditioner 1000 that can suppress temperature fluctuation with respect to the set temperature of the cooling target to be small and can realize highly controllable operation.

[実施の形態2]
図8は本発明の実施の形態2に係る冷凍空調装置を説明する冷媒回路を示す構成図である。なお、実施の形態1と同じ部分にはこれと同じ符号を付し、一部の説明を省略する。 図8において、冷凍空調装置2000は、実施の形態1における冷凍空調装置1000に、内部熱交換器4a、4bの高圧側入口に内部熱交高圧入口温度センサー16a、16bと、高圧側出口に内部熱交高圧出口温度センサー17a、17bとを付加したものである。高圧側の熱交換量QH[kW]は、(式7)により、低圧側の熱交換量QL[kW]は、(式8)によりそれぞれ求めることができる。そして、内部熱交換器4a、4bでは、「QH=QL」の関係が成り立つため、(式9)が導かれる。
[Embodiment 2]
FIG. 8 is a configuration diagram showing a refrigerant circuit for explaining a refrigerating and air-conditioning apparatus according to Embodiment 2 of the present invention. The same parts as those in the first embodiment are denoted by the same reference numerals, and a part of the description is omitted. In FIG. 8, the refrigerating and air-conditioning apparatus 2000 is different from the refrigerating and air-conditioning apparatus 1000 according to the first embodiment in that the internal heat exchangers 4a and 4b have internal heat exchange high-pressure inlet temperature sensors 16a and 16b at the high-pressure side inlet and the high-pressure side outlet. Heat exchanger high pressure outlet temperature sensors 17a and 17b are added. The heat exchange amount QH [kW] on the high pressure side can be obtained from (Equation 7), and the heat exchange amount QL [kW] on the low pressure side can be obtained from (Equation 8). In the internal heat exchangers 4a and 4b, since the relationship of “QH = QL” is established, (Equation 9) is derived.

Figure 2011220559
Figure 2011220559

ここで、
GrH :高圧側冷媒循環量[kg/s]、
hHO:内部熱交高圧側出口エンタルピー[kJ/kg]、
hHI:内部熱交高圧側入口エンタルピー[kJ/kg]、
GrL :低圧側冷媒循環量[kg/s]、
hLO:内部熱交低圧側出口エンタルピー[kJ/kg]、
TLI:内部熱交低圧側入口エンタルピー[kJ/kg]を表す。
here,
GrH: High-pressure side refrigerant circulation rate [kg / s],
hHO: Internal heat exchange high pressure side outlet enthalpy [kJ / kg],
hHI: Internal heat exchange high pressure side inlet enthalpy [kJ / kg],
GrL: Low-pressure side refrigerant circulation rate [kg / s],
hLO: Internal heat exchange low pressure side outlet enthalpy [kJ / kg]
TLI: Internal heat exchange low pressure side inlet enthalpy [kJ / kg].

hLOは、利用側熱交入口温度センサー14a、14bにて検出される蒸発温度から換算される圧力もしくは吸入圧力と、内部熱交低圧出口温度センサー13a、13bにて検出される温度から冷媒物性式にて演算可能である。また、hHIは、吐出圧力と、内部熱交高圧入口温度センサー16a、16bにて検出される温度から冷媒物性式にて演算可能である。また、hHOは、吐出圧力と、内部熱交高圧出口温度センサー17a、17bにて検出される温度から冷媒物性式にて演算可能である。
よって、以上から内部熱交入口エンタルピー、すなわち利用側熱交換器6a、6bの出口エンタルピーhLIを演算することができる。出口エンタルピーhLIが求まれば(式10)によって、内部熱交入口乾き度x、すなわち利用側熱交換器6a、6bの「出口乾き度xLO」を演算することができる。
hLO is a refrigerant physical property formula based on the pressure or suction pressure converted from the evaporation temperature detected by the use side heat exchange inlet temperature sensors 14a and 14b and the temperature detected by the internal heat exchange low pressure outlet temperature sensors 13a and 13b. It is possible to calculate with. The hHI can be calculated from the discharge pressure and the temperature detected by the internal heat exchange high pressure inlet temperature sensors 16a and 16b by the refrigerant physical property formula. Further, hHO can be calculated from the discharge pressure and the temperature detected by the internal heat exchange high pressure outlet temperature sensors 17a and 17b by the refrigerant physical property formula.
Therefore, the internal heat exchange inlet enthalpy, that is, the outlet enthalpy hLI of the use side heat exchangers 6a and 6b can be calculated from the above. If the exit enthalpy hLI is obtained, the internal heat exchange inlet dryness x, that is, the “exit dryness xLO” of the use side heat exchangers 6a and 6b can be calculated by (Equation 10).

Figure 2011220559
ここで、
hsl:蒸発温度に対する飽和液エンタルピー、
hsg:蒸発温度に対する飽和ガスエンタルピー、を表す。
Figure 2011220559
here,
hsl: saturated liquid enthalpy with respect to the evaporation temperature,
hsg: Saturated gas enthalpy with respect to the evaporation temperature.

以上のように、実施の形態2によれば、内部熱交換器4a、4bの高圧側入口および出口にそれぞれ温度センサーを配置し、内部熱交換器4a、4bにおける高圧側と低圧側の熱バランス式から、利用側熱交換器6a、6bの出口の冷媒の「乾き度xの状態」を計測することができるため、運転状態が負荷によって変動した場合でも、利用側熱交換器6a、6bの出口における乾き度xの状態に応じて膨張機構5a、5bを制御すること可能となる。
これにより、冷却対象の負荷が大きい場合は、高効率な運転を行い、負荷が小さい場合は、冷却能力を負荷に合わせる運転が可能となる。このため、頻繁な発停を防止することで、冷却対象の設定温度に対する温度変動が小さい制御性の高い運転を実現することができる冷凍空調装置2000を得ることができる。
As described above, according to the second embodiment, the temperature sensors are arranged at the high-pressure side inlet and the outlet of the internal heat exchangers 4a and 4b, respectively, and the heat balance between the high-pressure side and the low-pressure side in the internal heat exchangers 4a and 4b. From the equation, since the “dryness x state” of the refrigerant at the outlet of the use side heat exchangers 6a and 6b can be measured, even when the operation state varies depending on the load, the use side heat exchangers 6a and 6b The expansion mechanisms 5a and 5b can be controlled in accordance with the state of the dryness x at the outlet.
As a result, when the load to be cooled is large, high-efficiency operation is performed, and when the load is small, operation that matches the cooling capacity to the load is possible. For this reason, the refrigeration air conditioner 2000 which can implement | achieve operation with high controllability with small temperature fluctuation with respect to preset temperature of cooling object can be obtained by preventing frequent start / stop.

[実施の形態3:冷凍空調装置]
図9および図10は本発明の実施の形態3に係る冷凍空調装置を説明するものであって、図9は冷媒回路を示す構成図、図10は冷媒の乾き度と配管の圧力損失の関係を示す特性図である。なお、実施の形態1と同じ部分にはこれと同じ符号を付し、一部の説明を省略する。
[Embodiment 3: Refrigeration air conditioner]
9 and 10 illustrate a refrigeration and air-conditioning apparatus according to Embodiment 3 of the present invention. FIG. 9 is a configuration diagram showing a refrigerant circuit, and FIG. 10 is a relationship between the dryness of the refrigerant and the pressure loss of the piping. FIG. The same parts as those in the first embodiment are denoted by the same reference numerals, and a part of the description is omitted.

図9において、冷凍空調装置3000は、冷凍空調装置1000(実施の形態1)に、熱源側熱交換器2と液延長配管3の間に熱源側内部熱交換器9を付加し、その高圧側入口に熱源側内部熱交高圧入口温度センサー18、その高圧側出口に熱源側内部熱交高圧出口温度センサー19を付加し、その低圧側出口に熱源側内部熱交低圧出口温度センサー30を、それぞれ付加したものである。   In FIG. 9, the refrigeration air conditioner 3000 adds a heat source side internal heat exchanger 9 between the heat source side heat exchanger 2 and the liquid extension pipe 3 to the refrigeration air conditioner 1000 (Embodiment 1). A heat source side internal heat exchanger high pressure inlet temperature sensor 18 is added to the inlet, a heat source side internal heat exchanger high pressure outlet temperature sensor 19 is added to the high pressure side outlet, and a heat source side internal heat exchanger low pressure outlet temperature sensor 30 is connected to the low pressure side outlet. It is added.

図10に示す、配管入口の冷媒の乾き度に対する、配管の圧力損失との関係において、冷媒の乾き度が1付近では、冷媒の乾き度が1の時が最も圧力損失が小さいことが分かる。したがって、ガス延長配管7の入口の乾き度が1となるようにすることで、圧力損失が少ない高効率な運転を実現することができる。   In the relationship between the pressure loss of the pipe with respect to the dryness of the refrigerant at the pipe inlet shown in FIG. 10, it can be seen that when the dryness of the refrigerant is near 1, the pressure loss is the smallest when the dryness of the refrigerant is 1. Therefore, when the dryness of the inlet of the gas extension pipe 7 is set to 1, a highly efficient operation with little pressure loss can be realized.

なお、冷凍空調装置1000、2000(実施の形態1、2)においてガス延長配管7は利用ユニット200a、200bの過熱ガス冷媒が合流するため乾き度は1より大きくなる。このため、圧力損失は、ガス延長配管7に「乾き度xが1」で流入する場合に比較して圧力損失が大きくなる。
そこで、熱源側内部熱交換器9を追加することで、冷凍空調装置2000(実施の形態2)と同様の方法で、熱源側内部熱交高圧入口温度センサー18、熱源側内部熱交高圧出口温度センサー19、および熱源側内部熱交低圧出口温度センサー30がそれぞれ検出した温度に基づいて、ガス延長配管7の乾き度を計測することができる。
In the refrigerating and air-conditioning apparatuses 1000 and 2000 (Embodiments 1 and 2), the gas extension pipe 7 has a dryness greater than 1 because the superheated gas refrigerant of the use units 200a and 200b merges. For this reason, the pressure loss becomes larger than the case where the pressure loss flows into the gas extension pipe 7 with “dryness x = 1”.
Therefore, by adding the heat source side internal heat exchanger 9, the heat source side internal heat exchange high pressure inlet temperature sensor 18 and the heat source side internal heat exchange high pressure outlet temperature are obtained in the same manner as in the refrigeration air conditioner 2000 (Embodiment 2). The dryness of the gas extension pipe 7 can be measured based on the temperatures detected by the sensor 19 and the heat source side internal heat exchanger low-pressure outlet temperature sensor 30, respectively.

したがって、ガス延長配管7の流入乾き度は、冷却負荷の大きい利用ユニット200aの利用側熱交換器出口乾き度を1より小さく制御し、冷却負荷の小さい利用ユニット200bから流出する過熱ガスと合流した冷媒の「乾き度xが1」となるように膨張機構5a、5bを制御することで最も高効率な運転を実現することができる。
冷凍空調装置3000においては、ガス延長配管7が長いほどその制御の効果が大きくなることは言うまでもない。
Therefore, the inflow dryness of the gas extension pipe 7 is controlled so that the utilization side heat exchanger outlet dryness of the utilization unit 200a having a large cooling load is less than 1, and merged with the superheated gas flowing out from the utilization unit 200b having a small cooling load. The most efficient operation can be achieved by controlling the expansion mechanisms 5a and 5b so that the “dryness x of the refrigerant is 1”.
In the refrigeration air conditioner 3000, it goes without saying that the longer the gas extension pipe 7, the greater the control effect.

以上のように、冷凍空調装置3000によれば、熱源側内部熱交換器9における熱バランス式からガス延長配管7を流通する冷媒の「乾き度xが1」となるように、膨張機構5a、5bを制御することで、ガス延長配管7における圧力損失が少ない高効率な運転を実現することができる。   As described above, according to the refrigeration air conditioner 3000, the expansion mechanism 5a, the “dryness x of the refrigerant flowing through the gas extension pipe 7 from the heat balance type in the heat source side internal heat exchanger 9 is 1”, By controlling 5b, a highly efficient operation with little pressure loss in the gas extension pipe 7 can be realized.

1:圧縮機、2:熱源側熱交換器、3:液延長配管、4a:内部熱交換器、4b:内部熱交換器、5a:膨張機構、5b:膨張機構、6a:利用側熱交換器、6b:利用側熱交換器、7:ガス延長配管、9:熱源側内部熱交換器、11:吐出圧力センサー、12:吸入圧力センサー、13a:内部熱交低圧出口温度センサー、13b:内部熱交低圧出口温度センサー、14a:利用側熱交入口温度センサー、14b:利用側熱交入口温度センサー、15a:空気温度センサー、15b:空気温度センサー、16a:内部熱交高圧入口温度センサー、16b:内部熱交高圧入口温度センサー、17a:内部熱交高圧出口温度センサー、17b:内部熱交高圧出口温度センサー、18:熱源側内部熱交高圧入口温度センサー、19:熱源側内部熱交高圧出口温度センサー、20:計測制御装置、21:冷媒状態量演算手段、22:目標冷媒状態量演算手段、23:補正手段、24a:庫内温度設定手段、24b:庫内温度設定手段、30:熱源側内部熱交低圧出口温度センサー、ΔSH:制御目標値(温度変化量)、α1:高圧液側熱伝達率、αg:低圧ガス側熱伝達率、ε:温度効率、λ:熱伝導率、100:熱源ユニット、200a:利用ユニット、200b:利用ユニット、300a:冷蔵室、300b:冷蔵室、1000:冷凍空調装置、2000:冷凍空調装置、3000:冷凍空調装置、A:伝熱面積、Gr:冷媒循環量、K:熱通過率、QH:熱交換量、QL:熱交換量、QR:要求冷却能力比、RT:庫内温度、SC:過冷却度、SHL:内部熱交換器出口過熱度、SHLa:過熱度、SHLb:過熱度、SHLm:目標過熱度(制御目標値)、SHe:利用側熱交換器出口過熱度、SJ:開度、SJmin:閉塞開度、SJnow:現在の開度、TD:利用温度差、THI:内部熱交高圧側入口温度、TLO:内部熱交低圧側出口温度、Te:蒸発温度、hLI:出口エンタルピー、x:乾き度。   1: compressor, 2: heat source side heat exchanger, 3: liquid extension pipe, 4a: internal heat exchanger, 4b: internal heat exchanger, 5a: expansion mechanism, 5b: expansion mechanism, 6a: utilization side heat exchanger 6b: use side heat exchanger, 7: gas extension pipe, 9: heat source side internal heat exchanger, 11: discharge pressure sensor, 12: suction pressure sensor, 13a: internal heat exchanger low pressure outlet temperature sensor, 13b: internal heat AC low pressure outlet temperature sensor, 14a: user side heat exchanger inlet temperature sensor, 14b: user side heat exchanger inlet temperature sensor, 15a: air temperature sensor, 15b: air temperature sensor, 16a: internal heat exchanger high pressure inlet temperature sensor, 16b: Internal heat exchanger high pressure inlet temperature sensor, 17a: Internal heat exchanger high pressure outlet temperature sensor, 17b: Internal heat exchanger high pressure outlet temperature sensor, 18: Heat source side internal heat exchanger high pressure inlet temperature sensor, 19: Heat source side internal heat High pressure outlet temperature sensor, 20: measurement control device, 21: refrigerant state quantity calculating means, 22: target refrigerant state quantity calculating means, 23: correcting means, 24a: inside temperature setting means, 24b: inside temperature setting means, 30 : Heat source side internal heat exchange low pressure outlet temperature sensor, ΔSH: control target value (temperature change amount), α1: high pressure liquid side heat transfer coefficient, αg: low pressure gas side heat transfer coefficient, ε: temperature efficiency, λ: heat conductivity , 100: heat source unit, 200a: utilization unit, 200b: utilization unit, 300a: refrigerator compartment, 300b: refrigerator compartment, 1000: refrigeration air conditioner, 2000: refrigeration air conditioner, 3000: refrigeration air conditioner, A: heat transfer area, Gr: refrigerant circulation rate, K: heat passage rate, QH: heat exchange rate, QL: heat exchange rate, QR: required cooling capacity ratio, RT: internal temperature, SC: supercooling degree, SHL: internal heat exchanger outlet Superheat, SHL : Superheat degree, SHLb: superheat degree, SHLm: target superheat degree (control target value), SHe: utilization side heat exchanger outlet superheat degree, SJ: opening degree, SJmin: closed opening degree, SJnow: current opening degree, TD : Use temperature difference, THI: internal heat exchange high pressure side inlet temperature, TLO: internal heat exchange low pressure side outlet temperature, Te: evaporation temperature, hLI: outlet enthalpy, x: dryness.

Claims (9)

熱源ユニットと少なくとも2台以上の利用ユニットとを有し、
前記熱源ユニットが、冷媒を圧縮する圧縮機と、該圧縮機から吐出された高圧冷媒が流入する熱源側熱交換器とから構成され、
前記利用ユニットが、前記熱源側熱交換器の出口と液延長配管によって連結され、前記熱源側熱交換器から流出した高圧冷媒が流入する膨張機構と、該膨張機構から流出した低圧冷媒が流入する利用側熱交換器と、前記膨張機構に流入する高圧冷媒と前記利用側熱交換器から流出する低圧冷媒との間で熱交換を行い、前記圧縮機の入口にガス延長配管によって連結された内部熱交換器とから構成され、
前記利用側熱交換器出口における低圧冷媒の過熱度を検出する過熱度検出手段と、
前記利用側熱交換器を通過して低圧冷媒との間で熱交換をする利用流体の前記利用側熱交換器の入口における温度または出口における温度を検出する流入利用流体温度検出手段または流出利用流体温度検出手段と、
前記利用流体の前記利用側熱交換器の入口における温度または出口における温度を設定する流入利用流体温度設定手段または流出利用流体温度設定手段と、
該流入利用流体温度設定手段または流出利用流体温度設定手段から求まるそれぞれの冷却負荷の大小に応じて、前記内部熱交換器の低圧側出口における目標過熱度または目標乾き度を設定する目標冷媒状態量演算手段と、
前記内部熱交換器の低圧側出口において前記過熱度または目標乾き度になるように、前記膨張機構の流量調整を行う流量調整制御手段と、
を備えたことを特徴とする冷凍空調装置。
A heat source unit and at least two or more utilization units;
The heat source unit is composed of a compressor that compresses the refrigerant, and a heat source side heat exchanger into which the high-pressure refrigerant discharged from the compressor flows,
The utilization unit is connected to the outlet of the heat source side heat exchanger by a liquid extension pipe, and an expansion mechanism into which the high pressure refrigerant flowing out from the heat source side heat exchanger flows, and the low pressure refrigerant flowing out from the expansion mechanism flows in Heat exchange between the use-side heat exchanger, the high-pressure refrigerant flowing into the expansion mechanism and the low-pressure refrigerant flowing out from the use-side heat exchanger, and connected to the inlet of the compressor by a gas extension pipe It consists of a heat exchanger and
Superheat degree detection means for detecting the superheat degree of the low-pressure refrigerant at the outlet of the use side heat exchanger;
Inflow utilization fluid temperature detection means or outflow utilization fluid that detects the temperature at the inlet or the outlet of the utilization side heat exchanger of the utilization fluid that passes through the utilization side heat exchanger and exchanges heat with the low-pressure refrigerant. Temperature detection means;
Inflow utilization fluid temperature setting means or outflow utilization fluid temperature setting means for setting the temperature at the inlet of the utilization side heat exchanger or the temperature at the outlet of the utilization fluid;
The target refrigerant state quantity for setting the target superheat degree or the target dryness at the low-pressure side outlet of the internal heat exchanger according to the size of each cooling load obtained from the inflow utilization fluid temperature setting means or the outflow utilization fluid temperature setting means Computing means;
Flow rate adjustment control means for adjusting the flow rate of the expansion mechanism so as to achieve the superheat or target dryness at the low pressure side outlet of the internal heat exchanger;
A refrigeration air conditioner characterized by comprising:
前記内部熱交換器の低圧側出口における冷媒の過熱度から、前記利用側熱交換器の出口における冷媒の過熱度または乾き度を演算する利用側熱交換器出口冷媒状態量演算手段と、
前記利用側熱交換器において冷媒が前記利用流体との間で熱交換をする冷却負荷を演算する冷却負荷演算手段と、を有し、
前記目標冷媒状態量演算手段が、前記それぞれの冷却負荷の大小に替えて、前記冷却負荷演算手段の演算結果から、前記内部熱交換器の低圧側出口の過熱度または目標乾き度を設定することを特徴とする請求項1記載の冷凍空調装置。
From the superheat degree of the refrigerant at the low pressure side outlet of the internal heat exchanger, the use side heat exchanger outlet refrigerant state quantity calculating means for calculating the superheat degree or dryness of the refrigerant at the outlet of the use side heat exchanger;
Cooling load calculating means for calculating a cooling load for heat exchange between the refrigerant and the use fluid in the use side heat exchanger,
The target refrigerant state quantity calculation means sets the degree of superheat or the target dryness of the low-pressure side outlet of the internal heat exchanger from the calculation result of the cooling load calculation means instead of the magnitude of the respective cooling loads. The refrigerating and air-conditioning apparatus according to claim 1.
前記内部熱交換器の高圧側入口における冷媒温度と高圧側出口における冷媒温度との温度差を検出する温度差検出手段を備え、
該温度差検出手段の検出した温度差に基づいて、前記利用側熱交換器の出口の冷媒状態量として、前記内部熱交換器のエンタルピーまたは乾き度が演算されることを特徴とする請求項1に記載の冷凍空調装置。
A temperature difference detecting means for detecting a temperature difference between the refrigerant temperature at the high-pressure side inlet of the internal heat exchanger and the refrigerant temperature at the high-pressure side outlet;
The enthalpy or dryness of the internal heat exchanger is calculated as the refrigerant state quantity at the outlet of the use side heat exchanger based on the temperature difference detected by the temperature difference detecting means. The refrigeration air conditioner described in 1.
前記2台以上の利用ユニットのそれぞれにおいて、前記流入利用流体温度検出手段が検出した流入温度と前記流入利用流体温度設定手段が設定した流入温度との温度差、または前記流出利用流体温度検出手段が検出した流出温度と前記流出利用流体温度設定手段が設定した流出温度との温度差を求め、該温度差が最も大きい利用ユニットについて、前記内部熱交換器の低圧側出口の目標過熱度もしくは乾き度が最も小さく設定されることを特徴とする請求項1乃至3の何れかに記載の冷凍空調装置。   In each of the two or more usage units, the temperature difference between the inflow temperature detected by the inflow utilization fluid temperature detection means and the inflow temperature set by the inflow utilization fluid temperature setting means, or the outflow utilization fluid temperature detection means A temperature difference between the detected outflow temperature and the outflow temperature set by the outflow utilization fluid temperature setting means is obtained, and for the utilization unit having the largest temperature difference, the target superheat or dryness of the low pressure side outlet of the internal heat exchanger The refrigeration air conditioner according to any one of claims 1 to 3, wherein is set to be the smallest. 前記温度差が最も大きい利用ユニットにおいて、前記内部熱交換器の低圧側出口の目標過熱度もしくは乾き度は、前記利用側熱交換器出口の冷媒を乾き度1以下にすることを特徴とする請求項4に記載の冷凍空調装置。   In the utilization unit with the largest temperature difference, the target superheat degree or dryness of the low-pressure side outlet of the internal heat exchanger is such that the refrigerant at the outlet of the utilization side heat exchanger has a dryness of 1 or less. Item 5. A refrigeration air conditioner according to item 4. 前記2台以上の利用ユニットのそれぞれにおいて、前記流入利用流体温度検出手段が検出した流入温度と前記流入利用流体温度設定手段が設定した流入温度との温度差、または前記流出利用流体温度検出手段が検出した流出温度と前記流出利用流体温度設定手段が設定した流出温度との温度差を求め、該温度差が最も小さい利用ユニットについて、前記内部熱交換器の低圧側出口の目標過熱度または乾き度を最も大きく設定することを特徴とする請求項1乃至3の何れかに記載の冷凍空調装置。   In each of the two or more usage units, the temperature difference between the inflow temperature detected by the inflow utilization fluid temperature detection means and the inflow temperature set by the inflow utilization fluid temperature setting means, or the outflow utilization fluid temperature detection means The temperature difference between the detected outflow temperature and the outflow temperature set by the outflow utilization fluid temperature setting means is obtained, and the target superheat or dryness of the low-pressure side outlet of the internal heat exchanger is determined for the utilization unit having the smallest temperature difference. The refrigerating and air-conditioning apparatus according to any one of claims 1 to 3, wherein is set to a maximum. 前記内部熱交換器の低圧側出口の目標過熱度は、前記流入利用流体温度検出手段によって検出される温度または前記流出利用流体温度検出手段によって検出される温度と、前記利用側熱交換器の温度との間の温度差よりも小さいことを特徴とする請求項6に記載の冷凍空調装置。   The target superheat degree at the low-pressure side outlet of the internal heat exchanger is the temperature detected by the inflow utilization fluid temperature detection means or the temperature detected by the outflow utilization fluid temperature detection means, and the temperature of the utilization side heat exchanger. The refrigerating and air-conditioning apparatus according to claim 6, wherein the temperature difference is smaller than the temperature difference between the refrigerating and air-conditioning apparatus. 熱源ユニットと少なくとも2台以上の利用ユニットとを有し、
前記熱源ユニットが、冷媒を圧縮する圧縮機と、該圧縮機から吐出された高圧冷媒が流入する熱源側熱交換器とから構成され、
前記利用ユニットが、前記熱源側熱交換器の出口と液延長配管によって連結され、前記熱源側熱交換器から流出した高圧冷媒が流入する膨張機構と、該膨張機構から流出した低圧冷媒が流入する利用側熱交換器と、前記膨張機構に流入する高圧冷媒と前記利用側熱交換器から流出する低圧冷媒との間で熱交換を行い、前記圧縮機の入口にガス延長配管によって連結された内部熱交換器とから構成され、
前記熱源側熱交換器から流出した高圧冷媒と前記圧縮機に流入する低圧冷媒との間で熱交換をさせる熱源側内部熱交換器と、
前記熱源側内部熱交換器の低圧側出口における低圧冷媒の過熱度を検出する過熱度検出手段と、
前記熱源側内部熱交換器における熱交換量から、前記熱源側熱交換器の低圧側入口における低圧冷媒の過熱度または乾き度を演算する演算手段と、
前記利用側熱交換器を通過して低圧冷媒との間で熱交換をする利用流体の前記利用側熱交換器の入口における温度または出口における温度を検出する流入利用流体温度検出手段または流出利用流体温度検出手段と、
前記膨張機構の流量調整を行う流量調整制御手段と、を備え、
該流量調整制御手段は、前記2台以上の利用ユニットのそれぞれにおいて、前記流入利用流体温度検出手段が検出した流入温度と前記流入利用流体温度設定手段が設定した流入温度との温度差、または前記流出利用流体温度検出手段が検出した流出温度と前記流出利用流体温度設定手段が設定した流出温度との温度差を求め、該温度差が最も大きい利用ユニットについて、前記熱源側熱交換器の低圧側入口の冷媒の過熱度または乾き度を1に近づけるように前記膨張機構の流量調整を行うことを特徴とする冷凍空調装置。
A heat source unit and at least two or more utilization units;
The heat source unit is composed of a compressor that compresses the refrigerant, and a heat source side heat exchanger into which the high-pressure refrigerant discharged from the compressor flows,
The utilization unit is connected to the outlet of the heat source side heat exchanger by a liquid extension pipe, and an expansion mechanism into which the high pressure refrigerant flowing out from the heat source side heat exchanger flows, and the low pressure refrigerant flowing out from the expansion mechanism flows in Heat exchange between the use-side heat exchanger, the high-pressure refrigerant flowing into the expansion mechanism and the low-pressure refrigerant flowing out from the use-side heat exchanger, and connected to the inlet of the compressor by a gas extension pipe It consists of a heat exchanger and
A heat source side internal heat exchanger that exchanges heat between the high pressure refrigerant that has flowed out of the heat source side heat exchanger and the low pressure refrigerant that flows into the compressor;
Superheat degree detecting means for detecting the degree of superheat of the low pressure refrigerant at the low pressure side outlet of the heat source side internal heat exchanger;
Calculation means for calculating the degree of superheat or dryness of the low-pressure refrigerant at the low-pressure side inlet of the heat source-side heat exchanger from the amount of heat exchange in the heat source-side internal heat exchanger;
Inflow utilization fluid temperature detection means or outflow utilization fluid that detects the temperature at the inlet or the outlet of the utilization side heat exchanger of the utilization fluid that passes through the utilization side heat exchanger and exchanges heat with the low-pressure refrigerant. Temperature detection means;
Flow rate adjustment control means for adjusting the flow rate of the expansion mechanism,
The flow rate adjustment control means is configured such that, in each of the two or more usage units, the temperature difference between the inflow temperature detected by the inflow utilization fluid temperature detection means and the inflow temperature set by the inflow utilization fluid temperature setting means, or The temperature difference between the outflow temperature detected by the outflow use fluid temperature detection means and the outflow temperature set by the outflow use fluid temperature setting means is obtained, and the use unit having the largest temperature difference is used for the low pressure side of the heat source side heat exchanger. A refrigerating and air-conditioning apparatus, wherein the flow rate of the expansion mechanism is adjusted so that the degree of superheat or dryness of the refrigerant at the inlet approaches 1.
前記流量調整制御手段は、前記膨張機構の開口面積が閉塞する状態を、前記利用側熱交換器の出口における低圧冷媒の過熱度または前記内部熱交換器の低圧側出口の低圧冷媒の過熱度によって推測し、該推測された状態に基づいて、前記膨張機構の開口面積を補正することを特徴とする請求項1及至8の何れかに記載の冷凍空調装置。
The flow rate adjustment control means determines whether the opening area of the expansion mechanism is closed depending on the degree of superheat of the low-pressure refrigerant at the outlet of the use side heat exchanger or the degree of superheat of the low-pressure refrigerant at the low-pressure side outlet of the internal heat exchanger. The refrigerating and air-conditioning apparatus according to claim 1, wherein the refrigerating and air-conditioning apparatus according to any one of claims 1 to 8, wherein the refrigerating and air-conditioning apparatus corrects an opening area of the expansion mechanism based on the estimated state.
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JP2013164213A (en) * 2012-02-10 2013-08-22 Mitsubishi Heavy Ind Ltd Control device for heat pump, heat pump, and method of controlling heat pump
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JP2008530500A (en) * 2005-02-18 2008-08-07 キャリア コーポレイション Control of cooling circuit with internal heat exchanger
JP2009162388A (en) * 2007-12-28 2009-07-23 Mitsubishi Electric Corp Refrigerating/air-conditioning device, outdoor unit of refrigerating/air-conditioning device, and control device of refrigerating/air-conditioning device

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JP2013104620A (en) * 2011-11-14 2013-05-30 Daikin Industries Ltd Refrigeration device
JP2013164213A (en) * 2012-02-10 2013-08-22 Mitsubishi Heavy Ind Ltd Control device for heat pump, heat pump, and method of controlling heat pump
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WO2016063770A1 (en) * 2014-10-22 2016-04-28 ダイキン工業株式会社 Air conditioner
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