Figure 1.
Home PV installation under investigation.
Heat performance and internal pressure loss are important reference standards in solar air heaters (SAH). In order to solve the problem of too large a pressure loss in SAH, an innovative SAH with sinusoidal baffles was proposed on the basis of folded baffle and semi-circular baffle air heaters. A computational fluid dynamics (CFD) simulation calculation was performed for the SAH with sinusoidal baffles, and the relevant parameters, such as the heat collection efficiency and the pressure loss, were analyzed. The results showed that the sinusoidal baffle had a better heat collection performance and a smaller pressure loss compared to the folded baffle and the semi-circular baffle. A sinusoidal baffle can further improve the thermal performance of SAH. The simulation calculation of wave lengths for sinusoidal baffles revealed that when the wavelength value was 200 mm, the SAH had the best heat collection effect, and the heat collection efficiency was 64.49%. On the basis of determining the wavelength, the wave height of the sinusoidal baffle was studied. When the wave height was 30 mm, the minimum pressure loss of the SAH was 17.51 Pa, and the maximum heat collection efficiency was 64.91%. Analyses and research on the Reynolds number of the air inlet showed that as the Reynolds number increased, the collection efficiency and internal pressure loss gradually increased, while the outlet temperature decreased. The curve fitting of the imported Reynolds number and the pressure loss showed that the accuracy of pressure loss fitting curve is 0.997. Research on a double-layer SAH showed that the cross different inlet (CDI) had the best collector performance. This research has a high practicality and can provide a theoretical basis for winter air heating.
Citation: Xiaolong Wang, Lingning Zhang, Yuan Chang, Yang Song, Liang Wang. Numerical simulation study on heat performance and pressure loss of solar air heater with sinusoidal baffles[J]. AIMS Energy, 2024, 12(3): 617-638. doi: 10.3934/energy.2024029
| [1] | Amer Braik, Asaad Makhalfih, Ag Sufiyan Abd Hamid, Kamaruzzaman Sopian, Adnan Ibrahim . Impact of photovoltaic grid-tied systems on national grid power factor in Palestine. AIMS Energy, 2022, 10(2): 236-253. doi: 10.3934/energy.2022013 |
| [2] | Arben Gjukaj, Rexhep Shaqiri, Qamil Kabashi, Vezir Rexhepi . Renewable energy integration and distributed generation in Kosovo: Challenges and solutions for enhanced energy quality. AIMS Energy, 2024, 12(3): 686-705. doi: 10.3934/energy.2024032 |
| [3] | Paul K. Olulope, Oyinlolu A. Odetoye, Matthew O. Olanrewaju . A review of emerging design concepts in applied microgrid technology. AIMS Energy, 2022, 10(4): 776-800. doi: 10.3934/energy.2022035 |
| [4] | Jin H. Jo, Zachary Rose, Jamie Cross, Evan Daebel, Andrew Verderber, John C. Kostelnick . Application of Airborne LiDAR Data and Geographic Information Systems (GIS) to Develop a Distributed Generation System for the Town of Normal, IL. AIMS Energy, 2015, 3(2): 173-183. doi: 10.3934/energy.2015.2.173 |
| [5] | Virendra Sharma, Lata Gidwani . Recognition of disturbances in hybrid power system interfaced with battery energy storage system using combined features of Stockwell transform and Hilbert transform. AIMS Energy, 2019, 7(5): 671-687. doi: 10.3934/energy.2019.5.671 |
| [6] | Yannick Fanchette, Harry Ramenah, Camel Tanougast, Michel Benne . Applying Johansen VECM cointegration approach to propose a forecast model of photovoltaic power output plant in Reunion Island. AIMS Energy, 2020, 8(2): 179-213. doi: 10.3934/energy.2020.2.179 |
| [7] | Lasanthika Dissawa, Nirmana Perera, Kapila Bandara, Prabath Binduhewa, Janaka Ekanayake . Thirteen-level inverter for photovoltaic applications. AIMS Energy, 2016, 4(2): 397-413. doi: 10.3934/energy.2016.2.397 |
| [8] | Otto Andersen, Geoffrey Gilpin, Anders S.G. Andrae . Cradle-to-gate life cycle assessment of the dry etching step in the manufacturing of photovoltaic cells. AIMS Energy, 2014, 2(4): 410-423. doi: 10.3934/energy.2014.4.410 |
| [9] | Kharisma Bani Adam, Jangkung Raharjo, Desri Kristina Silalahi, Bandiyah Sri Aprilia, IGPO Indra Wijaya . Integrative analysis of diverse hybrid power systems for sustainable energy in underdeveloped regions: A case study in Indonesia. AIMS Energy, 2024, 12(1): 304-320. doi: 10.3934/energy.2024015 |
| [10] | Jin H. Jo, Jamie Cross, Zachary Rose, Evan Daebel, Andrew Verderber, David G. Loomis . Financing options and economic impact: distributed generation using solar photovoltaic systems in Normal, Illinois. AIMS Energy, 2016, 4(3): 504-516. doi: 10.3934/energy.2016.3.504 |
Heat performance and internal pressure loss are important reference standards in solar air heaters (SAH). In order to solve the problem of too large a pressure loss in SAH, an innovative SAH with sinusoidal baffles was proposed on the basis of folded baffle and semi-circular baffle air heaters. A computational fluid dynamics (CFD) simulation calculation was performed for the SAH with sinusoidal baffles, and the relevant parameters, such as the heat collection efficiency and the pressure loss, were analyzed. The results showed that the sinusoidal baffle had a better heat collection performance and a smaller pressure loss compared to the folded baffle and the semi-circular baffle. A sinusoidal baffle can further improve the thermal performance of SAH. The simulation calculation of wave lengths for sinusoidal baffles revealed that when the wavelength value was 200 mm, the SAH had the best heat collection effect, and the heat collection efficiency was 64.49%. On the basis of determining the wavelength, the wave height of the sinusoidal baffle was studied. When the wave height was 30 mm, the minimum pressure loss of the SAH was 17.51 Pa, and the maximum heat collection efficiency was 64.91%. Analyses and research on the Reynolds number of the air inlet showed that as the Reynolds number increased, the collection efficiency and internal pressure loss gradually increased, while the outlet temperature decreased. The curve fitting of the imported Reynolds number and the pressure loss showed that the accuracy of pressure loss fitting curve is 0.997. Research on a double-layer SAH showed that the cross different inlet (CDI) had the best collector performance. This research has a high practicality and can provide a theoretical basis for winter air heating.
Electrical power quality has been one of the major issues under investigation in the past decades. Electrical power quality is reflected on the electrical current and voltage waveforms. Ideal waveforms have a pure sinusoidal form with a standard frequency, depending on the country. For example, in Greece, the electrical current and voltage waveforms should present sinusoidal form with a frequency of 50 Hz. These waveforms deviate from the pure sinusoidal form due to many factors associated especially with power electronics. For this reason, quality indices have been introduced in order to characterize the purity of these waveforms. For the current and the voltage respectively, the Total Harmonic Distortion of the Current, THDi, and the Total Harmonic Distortion of the Voltage, THDv, are widely used. The massive penetration of PV generators, charging stations for electric vehicles and other similar electronic devices with high power content, resulted in an increment of the harmonic distortion and especially in the frequency band between 2 and 150 kHz. The term "supraharmonics" has been introduced from the scientific and engineering communities to characterize this particular frequency band.
Recent research work has proven that the existence of supraharmonics can have a negative impact on the operation of the electricity network [1,2]. For example, supraharmonics have been associated with acoustic noise. Coils, transformers and capacitors included in household devices constitute sources of mechanical oscillations which are transmitted on the surfaces of devices and detected as noise. Characteristic examples of devices that have been associated with acoustic noise resulting from supraharmonics are battery chargers for electronic equipment such as personal computers and smart phones [3].
Research on supraharmonics has recently intensified due to the increasing reports of disturbances attributed to them. Data from various sites in Europe and North America reveals that supraharmonic emission is affecting networks worldwide [4]. In North America, the problem of supraharmonic emission is stronger than in Europe, possibly because of a differentiation on the design of the two grids or due to the connection of more supraharmonic injecting devices to the North American electrical grid. Furthermore, according to [4], important problems for the correct measurement of supraharmonics are measuring instrument restrictions and the lack of standardization regarding measuring techniques.
Scientific research conducted on the electricity network in Germany [2] has revealed supraharmonic pollution in the electrical current and voltage waveforms associated with renewable energy sources. The existence of supraharmonics was the result of the utilization of frequency power converters. Additionally, according to this research, the supraharmonics can be transferred from the High Voltage network to the Medium Voltage and Low Voltage networks. In [5], an investigation on the supraharmonic interaction between an electrical vehicle and a photovoltaic inverter was conducted. The intermodulation distortion due to the interaction of different switching frequencies was highlighted. A typical domestic customer was also considered in this study to reveal the effect of intermodulation distortion on household equipment. Supraharmonic emissions from electric trains used in public transportation were investigated in [6]. The static frequency converters used in these railway systems seem to have an extra negative impact on suprahatmonic emissions. It was shown that the increase of frequency power converters in such railway systems lead to the increase of emissions in the 1–10 kHz band. A system built to measure supraharmonics in the range of 2 up to 300 kHz revealed the supraharmonic emission of Light Emitting Diodes (LEDs) and CFL lighting devices [7,8]. This system considers the measurement of the voltage as well as current spectra. The operation of Compact Fluorescent Lamps (CFL) was also investigated in [9]. Simulation results showed that the ballast circuit used in CFLs can be responsible for supraharmonic emissions. However, since the distribution system impedance is basically resistive, it was concluded that it is unlikely for the supraharmonic emission from CFLs to spread through the electricity network. On the other hand, as it was proved in [10], supraharmonics can, in fact, propagate through a Medium Voltage electrical network over several kilometers. Practical methods for the determination of the sources of supraharmonics were also introduced.
Apart from supraharmonic emission propagation toward the electrical grid, there is also the case of emission propagating toward a neighboring customer's installation. In fact, the latter seems to be more likely than the former. Moreover, supraharmonic emissions propagation seems to be strongly associated with the number and constellation of devices emitting supraharmonics, as well as the source impedance characteristics [11]. Furthermore, the flow of a large number of harmonics and supraharmonics may result in high frequency resonances in the grid. The change in the resonance characteristics of the power grid cannot be addressed with classical passive filters. For this reason, the use of active filters can significantly improve the performance of passive filters [12].
Regardless of the power rating of the devices, grid-connected inverters used for the conversion of DC current and voltage to AC are a common component. Even though the application of pulse width modulation techniques can significantly mitigate low order harmonic distortion, (<2 kHz), the high switching frequency required in modulation techniques results in suprahamonic emission. For this reason, both harmonic and supraharmonic distortion have to be taken into consideration from the early design stage of power inverters [13,14].
Emission levels seem to depend on many factors. For example, in photovoltaic systems such factors are the DC input voltage, AC voltage level and fluctuation and power output of the inverter. It is observed that different inverter models, with different designs and control schemes, present supraharmonic emission to the grid [15]. However, due to the wide range of operating conditions of PV systems, their behavior has to be more rigorously studied. The acquisition of as much data as possible on the factors affecting this behavior can provide helpful guidance on the selection of suitable equipment or installation location. In [16], the supraharmonic emissions of a small-scale grid-connected PV system were studied by means of a dedicated simulation tool. The impact of specific PV system parameters, such as filter component values and the location of the system on the utility distribution feeder, was investigated. In this study, field measurements of the supraharmonic emissions of a grid-connected PV system are examined and important conclusions regarding the influence of environmental parameters on their levels are derived. A custom measuring procedure was designed in the frame of the paper. The existence of supraharmonics was confirmed with the supraharmonic distortion due to the inverter be worst at low solar irradiance and therefore at low output power. The supraharmonics seem to be straight correlated with the switching frequency of the inverter and its integer multiples. The above-mentioned important observations can open new horizons in the design of power inverters aiming to the limitation of the supraharmonics. Additionally, this paper can essentially contribute to the shaping of future legislation about the supraharmonics into the modern electrical networks.
Our aim of this article is to investigate the suprahamonics produced by the inverter of a typical small residential photovoltaic (PV) system. Furthermore, the association of supraharmonic emissions with environmental parameters is investigated aiming to identify potential relation between them. The PV system used in this work is installed in Athens, Greece, with a nominal power of 8 kWp, with a 3-phase inverter and no other PV in the same connection line up to the transformer. The PV is directly connected to the low voltage electrical grid, in a distance of 300 m from the distribution transformer. The installed inverter is an SMA Sunny Tripower. Figure 1 presents the wiring of the PV scheme.
Table 1 presents the AC output characteristics of the inverter. It is worth noting that the THDi value, which is ≤3%, requires the THDv to be < 2% and the AC output power to be > 50% of nominal power. The THDi and THDv indices given for the inverter have been calculated without taking into consideration the supraharmonics band, due to the fact that supraharmonics are not addressed by international standards.
| Parameter | Value |
| Nominal value at 230 V and 50 Hz | 10 kW |
| Apparent Power with cosφ = 1 | 10 kVA |
| Nominal Grid Voltage | ~3/N/PE, 230 V/400 V |
| Nominal Current @ 220 V | 14.5 A |
| Nominal Current @ 230 V | 14.5 A |
| Nominal Current @ 240 V | 13.9 A |
| THDi when THDv < 2% and AC Power > 50% of nominal value | ≤3% |
DownLoad:
CSV
Figure 2 illustrates the measuring topology used in this paper. Temperature measurements are conducted on the frame and protected glass of the photovoltaic (no. 1 in Figure 2) using a laser thermometer. Ambient temperature and humidity are measured (no. 2) by means of a hand measuring device and solar irradiance is measured by means of a pyranometer (no. 3). Furthermore, a personal computer is used to obtain power measurements (no. 4) and three current probes in combination with a digital oscilloscope are used for the measurement of the three phase currents at the AC side of the inverter.
As mentioned, a laser thermometer was used for the temperature measurement on the glass of the photovoltaic panels and for the temperature on the corresponding frame of the photovoltaic panels. This laser thermometer (Type UNI-T UT303B IR) has a temperature range of –32 ~ 850 ℃. The response is 250 msec and the accuracy is ±1.8%.
The solar irradiance was measured by means of the solar irradiance sensor (pyranometer) DeltaOHM LP471PYRA.03 and a digital measuring device of type HD2102.2. The data sheet of the two measuring devices employed in the measurement of solar irradiance can be found in reference [17].
Three current transformers were used for the detection of the three phases of the current at the AC side of the inverter (Type ELDITEST CP6220 [18]). Their basic technical specifications are presented in Table 2. In addition, a four-channel digital oscilloscope (Type SDS2304X [19]) was used for the capture and measurement of the three electric currents. The current probe measuring bandwidth is DC up to 300 kHz. This range covers the supraharmonics located in the range of 2–150 kHz. The sampling rate of the oscilloscope is 2 Gsa/sec. This speed is adequate for the accurate detection and measurement of supraharmonics.
| Parameter | Value |
| Measurement ranges | 100–10 mV/A |
| Current (DC + peak AC) | 10–100 A |
| Bandwidth | DC–300 kHz |
| Rise and fall time | 1.2 µs (typ.) |
| Max. working voltage | 600 VAC RMS CAT Ⅱ / 300 VAC RMS CAT Ⅲ |
| Max. floating voltage | 600 VAC RMS CAT Ⅱ / 300 VAC RMS CAT Ⅲ |
| Operating Temp. | 0 to 50 ℃ (32 to 122 °F) |
| Max. operating humidity | 0 to 95% (0 to 40 ℃; 32 to 104 °F) 0 to 45% (40 to 50 ℃; 104 to 122 °F) |
DownLoad:
CSV
Our aim is to investigate the possible relation and potential correlation of specific environmental parameters with the supraharmonics produced at the inverter output of a small-scale residential PV installation. For this reason, two different sets of measurements are taken into consideration. The two sets were conducted on different days and hours of the year. The first measurement set was conducted on the 4th of September and in the time slot of 12.30 to 14.00. The second measurement set was conducted on the 17th of August and in the time slot of 16.00 to 18.15. The measured parameters were the solar irradiance in [W/m2], the PV glass temperature and PV panel frame temperature in [℃], the ambient temperature and humidity in [℃] and [%], respectively, the inverter AC output in [kW], and the three electric currents for the three phases at the inverter output in [A].
The electric current measurements for the three phases were conducted by means of the digital oscilloscope in combination with the current probes mentioned in the previous section. Their analysis for the existence of supraharmonics was done using Fourier transform with MATLAB code written by the authors.
Figure 3 presents the 3-phase electric currents at one measurement instance. The waveform is not a pure sinusoidal wave. The existence of harmonics is proven in Figure 3a. Additionally, Figure 3b shows the Fourier Transform analysis which was conducted in the band area from 10 up to 40 kHz. The Fourier analysis confirms the existence of supraharmonics.
During the measurement procedure six different parameters were measured, namely the three phase currents, the ambient temperature and humidity, the glass and frame temperature of the photovoltaic panels and the solar irradiance. Two measurement sets were obtained, corresponding to the two different days and time slots. Figure 4 presents the correlation of the THDi versus the inverter power output and the solar irradiance for the measurements of the first day. This figure presents the resulting THDi at 16 kHz (Figure 4a,b) and the resulting THDi at 32 kHz (Figure 4c,d). Quite expectedly, as the solar irradiance increases, so does the power output. However, it can also be deduced that as the solar irradiance increases, the THDi decreases. This is also evident from the results obtained on the second day, which are presented in Figure 5.
Figure 6 presents the correlation of THDi for the supraharmonic components of 16 and 32 kHz with the PV glass temperature and the solar irradiance. The increase of the solar irradiance results to an increase of the power output from the inverter. Moreover, the increase of the solar irradiance is associated with the increase of the PV glass temperature. On the other hand, the THDi for the supraharmonics seems to decrease.
Supraharmonics distortion is a power quality disturbance that has only been under study for the past few years. The results of the presented research confirm the presence of supraharmonics at the output of the power inverter of a small grid-connected PV system. The mean THDi value turned out to be quite significant and cannot be ignored. The correlation of the THDi with environmental parameters such as PV glass temperature and solar irradiance had not been examined up to this point. Most of the existing studies are based on the correlation of the AC power output quality with the THDi. From the presented measurements it can be deduced that the solar irradiance, which affects the AC power output, has an impact on the THDi. The decrease of the solar irradiance leads to an increase of the supraharmonics.
Even though many parameters have been taken into consideration in the current study, the investigation of additional operation conditions is of high priority. All the measurements presented in this study were taken during three different summer days with constantly high ambient temperatures. It is proposed that multiple sets of measurements are obtained, under different environmental conditions and seasons of the year. Moreover, in addition to the supraharmonic emissions of small-scale 3-phase PV inverters examined in this study, an extensive investigation of the supraharmonic emissions of power inverters included in large-scale PV installations should also be conducted. Additionally, standards on supraharmonics must be introduced as soon as possible, since PV inverters are only a portion of the supraharmonic emitting devices. Other well-established applications of inverter technology include motor control drives in industrial installations, wind farms and quick chargers for electrical vehicles.
We examined the correlation between the supraharmonic current emission of a residential PV inverter and environmental conditions. Two supraharmonic areas centered around 16 and 32 kHz were considered, since these areas demonstrated the greatest impact during the measurement procedure. The presented graphs separately displayed the THDi at 16 and 32 kHz. The total supraharmonic-related THDi is the sum of the corresponding indices at 16 and 32 kHz. This results in THDi values ranging from 2.5% at low solar irradiance (about 150 W/m2) to 0.8% at maximum solar irradiance (about 800 W/m2). The presented THDi is a mean value of the THDi of the three phases. It should be noted that in some cases with low solar irradiance the THDi of one phase was exceeding the value of 10%. There seems to be no correlation between the PV glass temperature and the THDi of the supraharmonics. It is our opinion that the investigation of the correlation of solar irradiance with the THDi must be extended to include the total harmonic range from fundamental to 150 kHz, and an overall THDi including the harmonic and supraharmonic bands should be calculated and regulated, because the supraharmonics do not have regulated limits. This will allow to identify the true THDi in the networks and will reduce the stress in the existing network equipment which is not designed to operate in such rich in harmonics environment. Additional measurements should be taken considering different locations, PV systems orientation, and different operational and weather conditions, allowing a better understanding of the magnitude of supraharmonics emitted to the networks from the PV operation. This will allow the proper regulation of the limits for supraharmonics emission to the grids.
The authors declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.
The publication of this article was financially supported by the Special Accounts for Research Grants, University of West Attica.
Constantinos S. Psomopoulos is an editorial board member for AIMS Energy and was not involved in the editorial review or the decision to publish this article. All authors declare that there are no competing interests.
Dimitrios Barkas: Investigation, Formal analysis, Data Curation, Writing—Original draft. Anthoula Menti: Writing—Review and Editing. Pavlos Pachos: Writing—Review and Editing, Funding acquisition. Constantinos Psomopoulos: Conceptualization, Writing—Review and Editing, Supervision.
| [1] |
Jia B, Liu F, Wang D (2019) Experimental study on the performance of spiral solar air heater. Sol Energy 182: 16–21. https://doi.org/10.1016/j.solener.2019.02.033 doi: 10.1016/j.solener.2019.02.033
|
| [2] |
Hao W, Zhang H, Liu S, et al. (2012) Design and prediction method of dual working medium solar energy drying system. Appl Therm Eng 195: 117153. https://doi.org/10.1016/j.applthermaleng.2021.117153 doi: 10.1016/j.applthermaleng.2021.117153
|
| [3] |
Zayed ME, Zhao J, Elsheikh AH, et al. (2019) Application of cascaded phase change materials in solar water collector storage tank:A review. Sol Energy Mater Sol Cells 199: 24–49. https://doi.org/10.1016/j.solmat.2019.04.018 doi: 10.1016/j.solmat.2019.04.018
|
| [4] |
Yin Y, Chen H, Zhao X, et al. (2022) Solar-absorbing energy storage materials demonstrating superior solar-thermal conversion and solar-persistent luminescence conversion towards building thermal management and passive illumination. Energy Convers Manage 266: 115804. https://doi.org/10.1016/j.enconman.2022.115804 doi: 10.1016/j.enconman.2022.115804
|
| [5] |
Muthukumaran J, Senthil R (2022) Experimental performance of a solar air heater using straight and spiral absorber tubes with thermal energy storage. J Energy Storage 45: 103796. https://doi.org/10.1016/j.est.2021.103796 doi: 10.1016/j.est.2021.103796
|
| [6] |
Stelian BA, Croitoru C, Bode F, et al. (2022) Experimental investigation of an enhanced transpired air solar collector with embodied phase changing materials. J Cleaner Prod 336: 130398. https://doi.org/10.1016/j.jclepro.2022.130398 doi: 10.1016/j.jclepro.2022.130398
|
| [7] |
Zayed ME, Zhao J, Li W, et al. (2020) Recent progress in phase change materials storage containers: Geometries, design considerations and heat transfer improvement methods. J Energy Storage 30: 101341. https://doi.org/10.1016/j.est.2020.101341 doi: 10.1016/j.est.2020.101341
|
| [8] |
El-Said EMS, Gohar MA, Ali A, et al. (2022) Performance enhancement of a double pass solar air heater by using curved reflector: Experimental investigation. Appl Therm Eng 202: 117867. https://doi.org/10.1016/j.applthermaleng.2021.117867 doi: 10.1016/j.applthermaleng.2021.117867
|
| [9] |
Heydari A, Mesgarpour M (2018) Experimental analysis and numerical modeling of solar air heater with helical flow path. Sol Energy 162: 278–288. https://doi.org/10.1016/j.solener.2018.01.030 doi: 10.1016/j.solener.2018.01.030
|
| [10] |
Gopi R, Ponnusamy P, Fantin AA, et al. (2021) Performance comparison of flat plate collectors in solar air heater by theoretical and computational method. Mater Today: Proc 39: 823–826. https://doi.org/10.1016/j.matpr.2020.09.809 doi: 10.1016/j.matpr.2020.09.809
|
| [11] |
Nain S, Ahlawat V, Kajal S, et al. (2021) Performance analysis of different U-shaped heat exchangers in parabolic trough solar collector for air heating applications. Case Stud Therm Eng 25: 100949. https://doi.org/10.1016/j.csite.2021.100949 doi: 10.1016/j.csite.2021.100949
|
| [12] |
Perwez A, Kumar R (2019) Thermal performance investigation of the flat and spherical dimple absorber plate solar air heaters. Sol Energy 193: 309–323. https://doi.org/10.1016/j.solener.2019.09.066 doi: 10.1016/j.solener.2019.09.066
|
| [13] |
Jiang Y, Zhang H, Wang Y, et al. (2021) A comparative study on the performance of a novel triangular solar air collector with tilted transparent cover plate. Sol Energy 227: 224–235. https://doi.org/10.1016/j.solener.2021.08.083 doi: 10.1016/j.solener.2021.08.083
|
| [14] |
Zhang H, Ma X, You S, et al. (2018) Mathematical modeling and performance analysis of a SAH with silt-perforated corrugated plate. Sol Energy 167: 147–157. https://doi.org/10.1016/j.solener.2018.04.003 doi: 10.1016/j.solener.2018.04.003
|
| [15] |
Saedodin S, Zaboli M, Ajarostaghi SSM (2021) Hydrothermal analysis of heat transfer and thermal performance characteristics in a parabolic trough solar collector with Turbulence-Inducing elements. Sustainable Energy Technol Assess 46: 101266. https://doi.org/10.1016/j.seta.2021.101266 doi: 10.1016/j.seta.2021.101266
|
| [16] |
Chand S, Chand P, Kumar GH (2022) Thermal performance enhancement of solar air heater using louvered fins collector. Sol Energy 239: 10–24. https://doi.org/10.1016/j.solener.2022.04.046 doi: 10.1016/j.solener.2022.04.046
|
| [17] |
Rehman T, Nguyen DD, Sajawal M (2024) Smart optimization and investigation of a PCMs-filled helical finned-tubes double-pass solar air heater: An experimental data-driven deep learning approach. Therm Sci Eng Prog 49: 102433. https://doi.org/10.1016/j.tsep.2024.102433 doi: 10.1016/j.tsep.2024.102433
|
| [18] |
Saravanakumar PT, Somasundaram D, Matheswaran MM (2020) Exergetic investigation and optimization of arc shaped rib roughened solar air heater integrated with fins and baffles. Appl Therm Eng 175: 115316. https://doi.org/10.1016/j.applthermaleng.2020.115316 doi: 10.1016/j.applthermaleng.2020.115316
|
| [19] |
Marwa A, Ameni M, Hatem M, et al. (2020) Numerical analysis of SAH provided with rows of rectangular fins. Energy Rep 6: 3412–3424. https://doi.org/10.1016/j.egyr.2020.11.252 doi: 10.1016/j.egyr.2020.11.252
|
| [20] |
Aref L, Fallahzadeh R, Shabanian SR, et al. (2021) A novel dual-diameter closed-loop pulsating heat pipe for a flat plate solar collector. Energy 230: 120751. https://doi.org/10.1016/j.energy.2021.120751 doi: 10.1016/j.energy.2021.120751
|
| [21] |
Saravanan A, Murugan M, Sreenivasa RM, et al. (2021) Thermo-hydraulic performance of a solar air heater with staggered C-shape finned absorber plate. Int J Therm Sci 2021,168: 107068. https://doi.org/10.1016/j.ijthermalsci.2021.107068 doi: 10.1016/j.ijthermalsci.2021.107068
|
| [22] |
Du J, Chen H, Li Q, et al. (2024) Turbulent flow-thermal-thermodynamic characteristics of a solar air heater with spiral fins. Int J Heat Mass Transfer 226: 125434. https://doi.org/10.1016/j.ijheatmasstransfer.2024.125434 doi: 10.1016/j.ijheatmasstransfer.2024.125434
|
| [23] |
Elumalai V, Arunkumar T, Thiruselvam K, et al. (2021) Thermal performance improvement in solar air heating: An absorber with continuous and discrete tubular and v-corrugated fins. Therm Sci Eng Prog 48: 102416. https://doi.org/10.1016/j.tsep.2024.102416 doi: 10.1016/j.tsep.2024.102416
|
| [24] |
Waheed S, Mahamed E, Ravishankar S, et al. (2023) Performance evaluation of a solar air heater with staggered/longitudinal finned absorber plate integrated with aluminium sponge porous medium. J Build Eng 73: 106841. https://doi.org/10.1016/j.jobe.2023.106841 doi: 10.1016/j.jobe.2023.106841
|
| [25] |
Wang L, Man Y (2018) Numerical simulation of SAH with folded baffles. Renewable Energy Resour 36: 997–1003. https://doi.org/10.13941/j.cnki.21-1469/tk.2018.07.008 doi: 10.13941/j.cnki.21-1469/tk.2018.07.008
|
| [26] |
Jia B, Yang L, Zhang L, et al. (2021) Optimizing structure of baffles on thermal performance of spiral solar air heaters. Sol Energy 224: 757–764. https://doi.org/10.1016/j.solener.2021.06.043 doi: 10.1016/j.solener.2021.06.043
|
| [27] |
Rani P, Tripathy PP (2022) Experimental investigation on heat transfer performance of solar collector with baffles and semicircular loops fins under varied air mass flow rates. Int J Therm Sci 178: 107597. https://doi.org/10.1016/j.ijthermalsci.2022.107597 doi: 10.1016/j.ijthermalsci.2022.107597
|
| [28] |
Jia B, Liu F, Li X, et al. (2021) Influence on thermal performance of spiral solar air heater with longitudinal baffles. Sol Energy 225: 969–977. https://doi.org/10.1016/j.solener.2021.08.004 doi: 10.1016/j.solener.2021.08.004
|
| [29] |
Zayed ME, Kabeel A, Bashar S, et al. (2023) Performance augmentation and machine learning-based modeling of wavy corrugated solar air collector embedded with thermal energy storage: Support vector machine combined with Monte Carlo simulation. J Energy Storage 74: 109533. https://doi.org/10.1016/j.est.2023.109533 doi: 10.1016/j.est.2023.109533
|
| [30] |
Magda K, Aly-Eldeen A, Abdelmaqsoud A, et al. (2024) Enhanced performance assessment of an integrated evacuated tube and flat plate collector solar air heater with thermal storage material. Appl Therm Eng 245: 122653. https://doi.org/10.1016/j.applthermaleng.2024.122653 doi: 10.1016/j.applthermaleng.2024.122653
|
| [31] |
Wang L (2022) Research on the collect heat performance of new type collector. Energy Sources, Part A: Recovery, Util, Environ Effects, 44: 9412–9427. https://doi.org/10.1080/15567036.2021.1954729 doi: 10.1080/15567036.2021.1954729
|
| [32] |
Song Z, Xue Y, Jia B, et al. (2022) Introduction of the rectangular hole plate in favor the performance of photovoltaic thermal solar air heaters with baffles. Appl Therm Eng 220: 119774. https://doi.org/10.1016/j.applthermaleng.2022.119774 doi: 10.1016/j.applthermaleng.2022.119774
|
| [33] |
Zhang D, Zhang J, Zhang Y, et al, (2019) Baffles optimization of a flat plate SAH with double channel. J Shanghai Jiao tong Univ 53: 1302–1307. https://doi.org/10.16183/j.cnki.jsjtu.2019.11.005 doi: 10.16183/j.cnki.jsjtu.2019.11.005
|
| 1. | Anthoula Menti, Pavlos Pachos, Constantinos S. Psomopoulos, Supraharmonic Distortion at the Grid Connection Point of a Network Comprising a Photovoltaic System, 2025, 18, 1996-1073, 564, 10.3390/en18030564 | |
| 2. | Chao Yan, Hongtao Shen, Jie Yu, Peng Tao, Hongxi Wang, Ting Yang, Supraharmonics monitoring based on VSSESP-DBP dynamic compressed sensing algorithm, 2025, 13, 2296-598X, 10.3389/fenrg.2025.1502652 | |
| 3. | Supraja Rajkumar, R. Balasubramanian, Parkavi Kathirvelu, N. Mohanraj, Analysis of supraharmonic emissions in hybrid power distribution systems, 2025, 0948-7921, 10.1007/s00202-025-03111-w |
Figures(12) / Tables(5)
Xiaolong Wang, Lingning Zhang, Yuan Chang, Yang Song, Liang Wang. Numerical simulation study on heat performance and pressure loss of solar air heater with sinusoidal baffles[J]. AIMS Energy, 2024, 12(3): 617-638. doi: 10.3934/energy.2024029
| Parameter | Value |
| Nominal value at 230 V and 50 Hz | 10 kW |
| Apparent Power with cosφ = 1 | 10 kVA |
| Nominal Grid Voltage | ~3/N/PE, 230 V/400 V |
| Nominal Current @ 220 V | 14.5 A |
| Nominal Current @ 230 V | 14.5 A |
| Nominal Current @ 240 V | 13.9 A |
| THDi when THDv < 2% and AC Power > 50% of nominal value | ≤3% |
DownLoad:
CSV
| Parameter | Value |
| Measurement ranges | 100–10 mV/A |
| Current (DC + peak AC) | 10–100 A |
| Bandwidth | DC–300 kHz |
| Rise and fall time | 1.2 µs (typ.) |
| Max. working voltage | 600 VAC RMS CAT Ⅱ / 300 VAC RMS CAT Ⅲ |
| Max. floating voltage | 600 VAC RMS CAT Ⅱ / 300 VAC RMS CAT Ⅲ |
| Operating Temp. | 0 to 50 ℃ (32 to 122 °F) |
| Max. operating humidity | 0 to 95% (0 to 40 ℃; 32 to 104 °F) 0 to 45% (40 to 50 ℃; 104 to 122 °F) |
DownLoad:
CSV
| Parameter | Value |
| Nominal value at 230 V and 50 Hz | 10 kW |
| Apparent Power with cosφ = 1 | 10 kVA |
| Nominal Grid Voltage | ~3/N/PE, 230 V/400 V |
| Nominal Current @ 220 V | 14.5 A |
| Nominal Current @ 230 V | 14.5 A |
| Nominal Current @ 240 V | 13.9 A |
| THDi when THDv < 2% and AC Power > 50% of nominal value | ≤3% |
| Parameter | Value |
| Measurement ranges | 100–10 mV/A |
| Current (DC + peak AC) | 10–100 A |
| Bandwidth | DC–300 kHz |
| Rise and fall time | 1.2 µs (typ.) |
| Max. working voltage | 600 VAC RMS CAT Ⅱ / 300 VAC RMS CAT Ⅲ |
| Max. floating voltage | 600 VAC RMS CAT Ⅱ / 300 VAC RMS CAT Ⅲ |
| Operating Temp. | 0 to 50 ℃ (32 to 122 °F) |
| Max. operating humidity | 0 to 95% (0 to 40 ℃; 32 to 104 °F) 0 to 45% (40 to 50 ℃; 104 to 122 °F) |
