• Tidak ada hasil yang ditemukan

Thermal Systems

N/A
N/A
Nguyễn Gia Hào

Academic year: 2023

Membagikan "Thermal Systems"

Copied!
182
0
0

Teks penuh

Application of the 2-D Trefftz Method for the Identification of Wave Flow Heat Transfer Coefficient in a Rectangular Minichannel. Energies. A Feasibility Study of Vehicle Air Conditioning System Application Using Vortex Tube.Energies.

Thermo-Economic Assessment of a Gas

Microturbine-Absorption Chiller Trigeneration System under Different Compressor Inlet

Air Temperatures

  • Introduction
  • Methodology
  • Results and Discussion
  • Conclusions

The turbine outlet gases (state 6) are directed to the preheater device where its temperature is reduced, and then to the heat recovery steam generator (HRSG) the heat transfer process allows us to generate steam (state 10), from water at ambient temperature (state 9). In the thermodynamic modeling of the trigeneration system [33], the components of the system are considered as open systems where a steady-state mass balance is applied according to equation (1).

Figure 1. Physical structure of the trigeneration system.
Figure 1. Physical structure of the trigeneration system.

Advance Exergo-Economic Analysis of a Waste Heat Recovery System Using ORC for a Bottoming Natural

On the other hand, the exogenous part of the exergy destruction is produced by the other components. Contribution of each component to the total exergy destruction of the cycle based on (A) traditional and (B) advanced exergy analysis.

Figure 1. The organic Rankine cycle waste heat recovery system.
Figure 1. The organic Rankine cycle waste heat recovery system.

A Li-Ion Battery Thermal Management System Combining a Heat Pipe and Thermoelectric Cooler

  • Theoretical Analysis
  • Numerical Simulations
  • Experiment
  • Discussion and Conclusions 1. Discussion

As shown in Figure 8, the surface temperature of the battery continued to rise during the discharge period. As the discharge rate increased, the discharge time shortened and the surface temperature of the battery increased.

Table 1. TAFEL-LAE895 battery specifications.
Table 1. TAFEL-LAE895 battery specifications.

Heat Transport Capacity of an Axial-Rotating Single-Loop Oscillating Heat Pipe for

Abrasive-Milling Tools

Experimental Preparation and Data Processing 1. Description of Experimental Apparatus

The SLOHP is mounted on the holder 30 mm away from its axis of rotation, which is the same as the radius of the OHP tool. Temperatures of the evaporator and condenser are measured by Omega type-K thermocouples (error limits: 0.4%). In this case, to study the thermal performance of the axial-rotating SLOHP under the same conditions with the abrasive-milling process, the rotation speed in the experiment is and 1500 rpm, with a relative centrifugal acceleration of and 738 m/s2.

Thermal resistance is used as a measure of the thermal performance of the axially rotating SLOHP.

Figure 2. Experimental preparation of axial-rotating oscillating heat pipe: (a) illustration of axial-rotating OHP; and (b) experimental setup (aerogel insulation was removed for better illustration).
Figure 2. Experimental preparation of axial-rotating oscillating heat pipe: (a) illustration of axial-rotating OHP; and (b) experimental setup (aerogel insulation was removed for better illustration).

Flow Visualization and Modeling

At the moment the evaporator is heated, the liquid turns into vapor, which causes the expansion of the vapor volume. The left term is the momentum produced by the vapor due to the vapor volume expansion. The first term of the right-hand side is the pressure differences acting on the liquid plug and vapor plug, while the second term of the right-hand side is due to the surface tension and the last term due to the shear stress between the wall and liquid.

The pressure of vapor and liquid is p1=p0,v+π. where p0,vandp0,la is the pressure of the vapor and liquid phases in a static state, Ris is the distance between the OHP and the axis of rotation and ω is the angular velocity.

Figure 3. Cont.
Figure 3. Cont.

Results and Discussion

However, when the centrifugal acceleration is large (e.g., 738 m/s2), the thermal efficiency of the methanol-filled axially rotating SLOHP is better than that of DI water. The effects of centrifugal acceleration, heat flux, and working fluid on the thermal performance of an axially rotating SLOHP are investigated through visualization, theoretical analysis, and experiments. Nevertheless, the heat capacity of the axially rotating SLOHP filled with DI water first increases and then decreases as the centrifugal acceleration increases.

Experimental investigation of thermal performance of the oscillating heat pipe for the grinding wheel.Int.

Figure 6. Effects of centrifugal acceleration: (a) methanol; (b) acetone; and (c) DI water.
Figure 6. Effects of centrifugal acceleration: (a) methanol; (b) acetone; and (c) DI water.

Problem Statement

In fact, the proposed model, based on a Lagrangian approach [10], was validated considering the working fluid as water and a reduced heat transfer between the pipes and the surroundings due to the great insulation of the pipes. In this contribution, the considered working fluid is oil and the heat transfer is higher due to the thermal energy recovered from the Sun. Therefore, the model is extended to include solar heating systems, taking into account the thermal solar gain and the inertia of the pipe system.

Although this paper focuses on the experimental validation of a medium-sized solar thermal plant, it can be extended to the modeling of larger solar plants, while the behavior of the main element, namely a tube, is studied and validated.

Modelling

In blue, the glass envelope; in grey, the metal tube; and in white, the vacuum between the two. It is assumed that temperatures, heat transfer coefficients and thermodynamic properties are considered uniform around the perimeter of the heat collector. Furthermore, thermal losses through the support fittings are neglected, and solar absorption in the tube and glass jacket is treated as a linear phenomenon [21].

Experimental Apparatus

The mass flow rate is derived from a data calibration study performed on the pump to evaluate it as a function of operating conditions. In Table 1, the working conditions of the main variables and the parameters of the external environment during the experimental campaign are reported. Mass Oil Flow Variation Experiment (MFE): a step change is imposed on the ETC inlet oil mass flow rate by varying the pump speed up or down, starting from a steady state.

Attempt to change the inlet oil temperature (TE): The oil temperature at the inlet to the ETC is varied by turning off the air cooler, starting from a steady state.

Figure 2. Process flow diagram of the Parabolic Trough Test Loop (PTTL) facilities with the relative sensors and devices position [21].
Figure 2. Process flow diagram of the Parabolic Trough Test Loop (PTTL) facilities with the relative sensors and devices position [21].

Results and Discussion

Again, the evolution of the predicted outlet temperature follows the experimental trends for several mass flow steps, inlet temperature steps, and solar energy steps or a combination thereof (Figure 4). Again, there is good agreement between plug flow modeling and experimental data for wide variations in mass flow rate, inlet pipe temperature, and solar irradiance. As shown in a previous modeling study of a district heating network, the thermal inertia of the system and the operating mass flow have a significant impact on the outlet temperature response.

Indeed, the mass flow rate influences how the fluid propagates in the pipe, while the influence of thermal inertia can be observed when the SBE conditions are set and can lead to a significant additional delay (more than 200 s) to get an outlet temperature with a value similar to the inlet temperature (considering the heat transfer to the ambient constant).

Figure 4. Experimental results performing different days versus plug flow and finite volume methods for several inlet temperature, mass flow rate and solar beam conditions
Figure 4. Experimental results performing different days versus plug flow and finite volume methods for several inlet temperature, mass flow rate and solar beam conditions

Conclusions

Indeed, in large networks with several intersections between pipes, the hydraulic part of the problem can become complex to solve due to the quadratic law relationship between pressure losses and mass flow rate. All results show a good agreement between experimental data and simulation results for a wide range of power plant operating conditions. In Proceedings of the 2nd International Conference on Computer Modeling and Simulation, Brno, Czech Republic, 5–7 September 2011; page

In Proceedings of the 14th International Society of Building Performance Simulation BS2015, Rome, Italy, 2–4 September 2019; pp.

Design Evaluation for a Finned-Tube CO 2 Gas Cooler in Residential Applications

Materials and Methods

The simulation model calculated the overall heat transfer coefficient of the gas cooler based on the mass flows, inlet and outlet temperatures, and pressures of the medium. The model used the average temperature and pressure of the mediums to calculate the heat transfer coefficients. The calculations were used to evaluate the overall performance of the gas cooler in different conditions.

Based on the off-design data, the overall heat transfer coefficient was calculated using Equations (3)-(17).

Figure 1. Scheme of the considered CO 2 air conditioning system.
Figure 1. Scheme of the considered CO 2 air conditioning system.

Results and Discussion 1. Validation of the Model

The increase in the water inlet temperature had a similar effect on the overall heat transfer coefficient of the heat exchanger Figure 5b. The absolute deviations between the model and the experiments were extracted and demonstrate the reliability of the selected heat transfer correlations. Increasing the fan frequency, water mass flow rate, and water inlet temperature resulted in an improvement in the overall heat transfer coefficient of the heat exchanger.

This procedure enables a reliable validation of the applied air-side heat transfer correlation.

Figure 4. Deviations between the model and experimental overall heat transfer coefficient for 45 ◦ C water inlet temperature at (a) 50 Hz; and (b) 80 Hz fan frequency.
Figure 4. Deviations between the model and experimental overall heat transfer coefficient for 45 ◦ C water inlet temperature at (a) 50 Hz; and (b) 80 Hz fan frequency.

Feasibility Study of a Centralised Electrically Driven Air Source Heat Pump Water Heater to Face Energy

Results

Figure 6 shows iso-lines of heating capacity as a function of rotation speed and ambient wet bulb temperature. A comparison with an actual machine was performed to validate the results of the heat pump model. A literature search was conducted to find an existing device that fits the characteristics of the modeled one.

On the other hand, the ratio between the thermal demand and the minimum heat capacity is on.

Figure 6. Iso-lines of heating capacity of the ASHPWH.
Figure 6. Iso-lines of heating capacity of the ASHPWH.

Discussion

In Figure 13, the average EPI obtained for residential blocks in Spain was represented through such a fitting curve, obtaining their heated area to maintain the same levelized costs as in the base case. Speed ​​regulation in the compressor gives the heat pump the ability to meet almost all heating needs (96% in the base case) with good efficiency. In addition, total energy from renewable sources is obtained to meet the heating demand, taking into account both the energy supplied by the air and the share of renewable sources in the electricity mix (used for heat pump electricity consumption).

Accordingly, in the same example, the levelized heating costs decrease by €500 for a house of 100 m2 (with a base cost of €848).

Figure 13. Required heated area (A) for each energy performance index (EPI) to maintain the same LCOH DB than in the baseline case (92.22 €/MWh) and LCOH AB obtained
Figure 13. Required heated area (A) for each energy performance index (EPI) to maintain the same LCOH DB than in the baseline case (92.22 €/MWh) and LCOH AB obtained

Conclusions

Disponible en línea: https://www.miteco.gob.es/es/ministerio/planes-estrategias/estrategia-pobreza-energetica/actuali zaciondeindicadorespobrezaenergetica2019_tcm30-502983.pdf (consultado el 15 de abril de 2020). Disponible en línea: https://www.codigotecnico.org/images/stories/pdf/ahorroEnergia/CTE datosMET_20140418.zip (consultado el 9 de abril de 2020). Disponible en línea: https://www.certificadosenergeticos.com/wp-content/uploads/2018/12/informe-seguimiento-certi ficacion-energetica.pdf (consultado el 26 de mayo de 2020).

Dostopno na spletu: https://www.miteco.gob.es/es/ministerio/servicios/info rmacion/informacion-y-atencion-al-ciudadano/default.aspx (dostopano 14. maja 2020).

Applicability of Swaging as an Alternative for the Fabrication of Accident-Tolerant Fuel Cladding

Experimental 1. Swaging Method

The PST was synthesized by applying a pressure of 4 t/cm2 in the direction of the central axis of the double tube. Figure 1 shows a schematic of the swing method for the double tube and the type of stress applied to the tube during the process. Figure 2 shows that the inner surface of the outer tube and the outer surface of the inner tube adhere closely to each other.

It is imperative to note that gaps in the interface can degrade the mechanical and chemical properties of the pipe.

Figure 2. Mechanism of swaging.
Figure 2. Mechanism of swaging.

LUFDOR\

To confirm the diffusion behavior of the PST, an EDS analysis was performed, as shown in Figure 10. TEM analysis was performed to confirm the interfacial stability of the PST after exposure to high temperatures. Figure 11 is a cross-sectional TEM image showing the Zircaloy-4/SUS 316 interfacial structure of the PST when quenched to room temperature after being held at 900°C for 1 hour.

Transmission electron microscopy (TEM) cross-sectional image showing the boundary structure of Zircaloy-4/SUS 316 PST quenched to room temperature after being held at 900 °C for 1 h.

Table 1 shows various physical properties of Zircaloy-4 and SUS 316. The total strain generated by swaging consists of a combination of elastic strain and plastic strain
Table 1 shows various physical properties of Zircaloy-4 and SUS 316. The total strain generated by swaging consists of a combination of elastic strain and plastic strain

Application of the 2-D Trefftz Method for Identification of Flow Boiling Heat Transfer

Experimental Facility

Two pressure sensors (Kobold 0–2.5 bar) were placed at the inlet and outlet of the channel. Photographs of the observed two-phase flow structures were taken with a high-speed video camera with a recording speed of 7000 fps. Lab is the void fraction for a single elongated bubble, Llb is the bubble length, composed of the length of an ellipsoidal cylinder and two half-ellipsoids.

Lab is the void for a single elongated bubble, Llb, ije length of the bubble, composed of the length of the ellipsoid cylinder and one semi-ellipsoid.

Figure 2. General view of the experimental stand; labels as in Figure 1.
Figure 2. General view of the experimental stand; labels as in Figure 1.

Mathematical Model and Numeric Solution

Next, by combining four T-complete functions for Equation (20) and specific solution of Equation (11), the field of the fluid temperature was found. Fluid flowing in the minichannel significantly reduces the temperature of the copper block over the contact area, Figure 12. Variation of the heat transfer coefficient for the flowing two-phase mixture is shown in Figure 13 as a function of the distance from the minichannel inlet.

Uncertainties of the experimental parameters determined in the study [2] were applied to calculate the mean relative error (MRE) of the heat transfer coefficient α(x).

Figure 11. Examples of recorded flow structures presented in (A1): q = 298.8 kW/m 2 , G = 8.6 kg/(m 2 s);
Figure 11. Examples of recorded flow structures presented in (A1): q = 298.8 kW/m 2 , G = 8.6 kg/(m 2 s);

A Study on the Application Possibility of the Vehicle Air Conditioning System Using Vortex Tube

Experimental Approach 1. Principle of Vortex Tube

The variation of temperature according to the pressure in the vortex tube device and the number of nozzles of the generator is investigated. In the case of Taoc (◦C), the temperature was measured by comparing the air flow rate at low temperature (yc) of the flow. The value of ΔTac (◦C) was also measured using the low temperature airflow ratio (yc), and the temperature difference was similar to Taoc (◦C).

Numerical investigations of compressible flow and energy dissipation in the Ranque–Hilsch vortex tube. Int.

Figure 1. Cross-section of the vortex tube in the “free” and “forced” vortex flow.
Figure 1. Cross-section of the vortex tube in the “free” and “forced” vortex flow.

MDPI

Gambar

Table 4. Thermodynamic properties, physical and chemical exergy of the trigeneration system.
Figure 7. Relative cost difference of the trigeneration system at different compressor inlet air temperatures, (a) Microturbine components, and (b) Absorption chiller components.
Figure 4. Advanced exergy analyses for each component in the ORC cycle, (a) HX 1, (b) P1, (c) turbine, (d) P2, (e) evaporator, and (f) condenser.
Figure 5. Contribution of each component to the overall exergy destruction of the cycle based on (A) traditional and (B) advanced exergy analysis.
+7

Referensi

Dokumen terkait

properties of dissimilar inner tube diameter of mild steel by MIG orbital welding. To develop and verify the empirical

Sedangkan untuk kondisi parameter pemotongan dengan suhu luaran vortex tube 14,67 o C, kepatan potong 88,39 m/min, diameter benda kerja 45 mm dan putaran poros 625 rpm

to ATEX declaration of conformity Design Hard tag, R30 Diameter 30 mm +/- 0.5 mm Features ■EEPROM, memory 128 byte ■Not for direct mounting on metal ■ATEX category II 1 G, Ex zone

The optical and thermal efficiencies are determined for a PTC system with aperture width 0.8 m, length 1.25 m, receiver tube diameter 12 mm and rim angle 90o for varying water inlet

Effect of the length to inner diameter ratio of vapor tube on the performance of a vacuum closed loop thermosyphon สราวุฒิ สิริเกษมสุข1, ธนาพล สุขชนะ1* Sarawut Sirikasemsuk1,

C; inner tube convective heat transfer correlation coefficient - Wilson plot Co annulus convective heat transfer correlation coefficient -Wilson plot D1 diameter of outer wall of

Results and Discussion In this analysis, the aim is to determine the effect of the cold mass fraction on various properties of vortex tube such as isentropic efficiency, COP, cold air

Nomenclature ΔP Pressure drop kPa add Additives - aq Aqueous phase - B.pt Boiling point ◦C C0 Initial concentration ppm dt Throat diameter of vortex diode mm Dev 1 Vortex-diode