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Efficiency of Dual Junction Photovoltaic Solar Cell

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Focusing on the bandgap of the double junction solar cell, it has been shown to be more efficient compared to the single junction solar cell. This demonstrates that a significant amount of efficiency can be achieved with a multi-junction III-V solar cell.

INTRODUCTION

HISTORY

8 The entire PV technology is based on the photoelectronic effect invented by Albert Einstein in 1905. In 1954, the world was introduced to the first photovoltaic module that was just a solar battery. The two most recognized power plants are the Solar Star PV plant which produces 550 megawatts.

Figure 1.1 Photoelectric effect
Figure 1.1 Photoelectric effect

WORKING PRINCIPLEOF PHOTOVOLATIC CELL

The modules can therefore be connected in series or parallel, which is very beneficial for the system. 11 But typically in the case of other formation of solar cells, such as crystalline silicon, solar cells are not 100% efficient in diagram.

Figure 1.3 (a) Layers of photo voltaic cell (b) Energy absorption of photo voltaic  cell[1]
Figure 1.3 (a) Layers of photo voltaic cell (b) Energy absorption of photo voltaic cell[1]

TYPES OF PHOTOVOLATIC TECHNOLOGY

Thin Film PV

The general procedure is to follow the sunlight from east to west during the day. The importance of this type is that it can deliver 30% to 40% more energy, which is more than a fixed array.

Concentrated PV (CPV)

13 The basis of this technology is the use of inexpensive materials such as mirrors or plastic lenses to track the sun's energy and focus it on solar PV cells. The main reason for using CPV is to reduce the number of solar cell material.

Figure 1.6 Concentrated-film PV
Figure 1.6 Concentrated-film PV

MATERIALS DEVELOPMENT

THE NEXT GENERATION PHOTO VOLTAICS CELL

And this is the maximum current capacity of the solar cell at any illumination level. In addition, the band gaps of adjacent layers should differ as little as possible, since the amount of excess energy from light converted into heat is equal to the difference between the photon energy and the gap of the absorbing material [39]. the semiconductor material determines how the solar cell reacts to light.

RECENT IMPROVEMENTS ON PHOTO VOLTAIC CELL

Improved Efficiency

Their technology was based on an intermediate process that occurs between sunlight and the solar cell, where the photoluminescent material used absorbs radiation from the sun, which converts the heat and light from the sun into an "ideal". As a consequence, a higher conversion efficiency was ensured and the device efficiency was increased from 30% to 50%[6].

Solar Fabrication Using Maximum Voltage from CdTe

Introducing Hot Solar Cell

The conversion efficiency of a solar cell is the ratio of the maximum output power generated to the input or accidental power that can be generalized by η. The amount and intensity of solar insolation (solar radiation) controls the amount of output current ( I ), and the operating temperature of the solar cells affects the output voltage ( V ) of the PV array.

Developing Home Systems in Bangladesh

Installation and Plans by BPDB

Bangladesh Power Development Board (BPDB) has also installed solar power plants in various parts of the country. In addition, IDCOL has financed nine biogas-based power plants, with a total capacity of 618 kW, and two rice husk-based power plants with a total capacity of 650 kW in the country.

New Solar Panel in Market 2017

To solve this problem, the innovative manufacturer is making inverters that can be easily attached to the back of the panel. The modules are planned to be manufactured with small inverters already located on the back of the panel.

CONCLUSION

The simple claim is that double-sided panels can capture light as it reflects from the roof or ground surface below the panel. Due to the fact that the majority of roofs in the residential market are black, in order to maximize light reflection, the installers will typically paint a white border around the solar system before installation.

INTRODUCTION

THEORATICAL APPROACH

  • Equivalent Circuit
  • Short Circuit Current
  • Open Circuit Voltage
  • Maximum Power
  • Fill Factor

This is the current that flows through the external circuit when the electrodes of a solar cell are short-circuited. These three important parameters (𝑉𝑜𝑐, 𝐼𝑠𝑐and FF) as described above are the main factors that determine how efficient a solar cell is and are optimized for efficient solar cell design.

Figure 2.1 Incident light on a typical PN Solar Cell [2]
Figure 2.1 Incident light on a typical PN Solar Cell [2]

PRACTICAL APPROACH

  • Solar Area Mounting and Tracking
  • Improving Solar Efficiency Using Simple Mirrors and
  • Improved Perovskite Solar Cell
  • High Efficient Ga-As-P Solar Cell
  • A Micro-scale Photo Voltaic Cell “Solar Glitter”

Therefore, the improvement of solar cells is very important so that a smaller number of arrays can produce more electricity. Step 3: A rose petal-like film was placed as the top layer of the solar panel to capture even more light.

Table 2.1 Azimuth Angle by heading [13]
Table 2.1 Azimuth Angle by heading [13]

LATEST INNOVATIONS

  • Cool Earth Inflatable Solar Balloons
  • Moth Eyes Biomimicry for Solar Cell
  • Printed Solar Panel “Nanosolar”
  • Convertion of Infrared Light to Electricity
  • CdTe Solar Panel

Because of this, such solar panels have a theoretical absorption limit of 63%, which compares to around 40% for ordinary solar cells. The US National Renewable Energy Laboratory (NREL) has created thin-film solar panels that come very close to competing with their more traditional silicon-based cousins.

Figure 2.9 A forest of GaAs nano wires growing on a silicon substrate.
Figure 2.9 A forest of GaAs nano wires growing on a silicon substrate.

CONCLUSION

However, the efficiency of CdTe is less susceptible to cell temperature increases, enabling CdTe solar modules to generate relatively more electricity under high ambient (and thus high cell) temperatures. As a result, under real-world conditions, CdTe will generally produce more electricity than a conventional solar module with similar power ratings [15].

INTRODUCTION

OPERATING PRINCIPLE OF SOLAR CELL

44 energy conversion, but in practice almost all photovoltaic energy conversion uses semiconductor materials in the form of a p-n junction.

RESEARCH WORK RELATED TO SOLAR DEVICES

Analytical Method

  • Solar cell parameters
  • Effect of Rs and Rsh Parameters

As a result, the voltage-controlled portion of the I-V curve begins to fall far from the origin, causing a significant reduction in the terminal current I and a slight reduction in VOC. As a result, the current-controlled portion of the I-V curve begins to slope toward the origin, causing a significant decrease in the junction voltage V and a slight decrease in Isc, the short-circuit current.

Fig 3.3 General view of solar cell idealized curve
Fig 3.3 General view of solar cell idealized curve

Effect of Temperature

D = given minority carrier diffusivity for silicon as a function of doping in the silicon material. The equation above shows that the temperature sensitivity of a solar cell depends on the open circuit voltage of the solar cell, with higher voltage solar cells being less affected by temperature.

SIMULATION ANALYSIS

Why We Need the Simulation

Based on the TCAD device design, the physical parameters that contribute to the resistances between the connections can be extracted and a system-level model developed. From the system cell level model, checks can be made to determine the effect of different cell widths on module performance.

TCAD (Technology Computer Aided Design)

  • TCAD Tools
  • TCAD simulation process
  • TCAD work flow

It takes a spice file as input and produces output describing the requested simulation of the circuit. Manufacturing manufacturing modeling is called Process TCAD, while device operation modeling is called Device TCAD.

Parameters That Can be changed

EXPERIMENTAL ANALYSIS

  • For The Measurement of External Characteristics
  • Measurement in Different Wavelengths
  • For the Measurement of Internal Characteristics
  • Measurement of Electro-luminiscence

Here we are observing various changes in the solar cell due to the effects of less and less light and different wavelengths of light on the PV cell and the temperature of the cell. When sunlight falls on the solar cell, the curve begins to move downward. a) (b) (c) Figure 3.15 Change of I-V characteristic curve with increasing incident light.

Figure 3.11 Schematic diagram for external characteristics of solar panel
Figure 3.11 Schematic diagram for external characteristics of solar panel

RESULT FOUND FROM THESE METHODS

CONCLUSION

INTRODUCTION

VIRTUAL WAFER WEB

We used double junction solar cell as a reference model for multi junction solar cell. For silicon single junction solar cell, we used three different materials (boron, arsenic, silicon) as the n-layer.

Fig 4.3 Flow of simulation
Fig 4.3 Flow of simulation

SIMULATION for ELECTRICAL CHARACTERISTICS

Functions of The Simulator

Inputs and Outputs

MODEL EXTRACTOR

DEVICE EDITOR

VISUALIZATION TOOL

SIMULATION PROCEDURE OVERVIEW

Modes of Operation

Solar Junction's multi-junction solar cell consists of several individual solar cells grown on top of each other. We noticed that the efficiency is much higher than the single junction solar cell.

Starting with Model Extractor

Syntex

Structure Specification

POSITION -defines the location of the region in terms of (1) actual position and (2) grid nodes. Atlas also provides a standard list of parameters for the properties of the material used in the simulation.

Result Analysis

Here we analyze two specific solar cells: a single-junction solar cell and a multi-junction solar cell. Secondly, in the case of single junction solar cells, the phosphorus doped silicon solar cell is better (both in terms of efficiency and fill factor) than all other single junction cells.

Extract Description

CONCLUSION

Thus, TCAD tools provide researchers with the electrical properties of solar cells under illumination in two- and three-dimensional domains. Two simulation inputs consisting of a text file and a simulation file are made using Deckbuild and Devedit.

INTRODUCTION

SILICON SOLAR CELL

WORKING PRINCIPLE

The electricity was produced by a series of solar cells converting solar energy into a usable amount of direct current (DC).

DUAL JUNCTION SOLAR CELL

PARAMETERS TO BE CONSIDERED

Lattice Match

94 Further InxGa1-xAs at X can be alloyed with InP to obtain a quaternary alloy InxGa1- xAsyP1-y, whose properties lie on the line connecting X and InP and thus all have the same lattice parameter as InP, but different bandgap- layers of InxGa1- xAsyP1-y with composition between X and InP can be grown exponentially on InP substrate by various techniques such as liquid phase epitaxy or molecular beam epitaxy.

Bandgap

  • Structure
  • Metal contacts
  • Window layer and back surface layer
  • Anti reflective (AR) coating
  • Tunnel junction

The back surface field, or BSF, consists of a higher doped region on the back surface of the solar cell. To avoid reducing the performance of the MJ solar cells, the tunnel junctions must be transparent to the wavelengths absorbed by the following photovoltaic cell.

Figure 5.5 Irradiance on different bandgap cell
Figure 5.5 Irradiance on different bandgap cell

CONCLUSION

INTRODUCTION

Throughout our analysis, we have approached versatile techniques that we look right now. So we have always tried to achieve the highest efficiency and fill factor by applying various measures.

Figure 6.1 Summary of the analysis
Figure 6.1 Summary of the analysis

SINGLE JUNCTION SOLAR CELL

Boron doped silicon solar cell

From the I-V curve, P-V curve and the Voc, Isc parameters we obtain further curves to study the filling factor and efficiency of the cells. But we could not find any significant change of fill factor with concentration as the curve appeared random.

Figure 6.2  I-V Characteristics Curve Boron Doped  Silicon Solar Cell
Figure 6.2 I-V Characteristics Curve Boron Doped Silicon Solar Cell

Arsenic doped silicon solar cell

Initially, the efficiency increased, but later, with increasing concentration, the efficiency decreased. The curve is random and maintains a sequence of increasing and decreasing fill factor with increasing.

Figure 6.8 P-V characteristics of Arsenic doped Si solar cell
Figure 6.8 P-V characteristics of Arsenic doped Si solar cell

Phosphorus doped silicon solar cell

We obtained the highest efficiency for phosphorus-doped silicon solar cell (18.55%) and the lowest for boron-doping (18.2%). We obtained almost the same fill factor (84.347%) for arsenic-doped solar cell and finally the lowest for boron-doping (83.53%).

Table 6.3 Important parameters for phosphorus doped silicon solar cell  Concentration  Open-circuit
Table 6.3 Important parameters for phosphorus doped silicon solar cell Concentration Open-circuit

DUAL JUNCTION SOLAR CELL

InGaP-GaAs Dual Junction Solar Cell

AlGaAs-GaAs Dual Junction Solar Cell…

There is a small difference in filling factor between InGaP-GaAs and AlGaAs-GaAs solar cells. In our next section we tried to improve the InGaP-GaAs solar cell by changing the concentration or replacing the back material.

Figure 6.21 I-V characteristics of AlGaAs-GaAs dual junction solar cell  From figure 6.21 after analyzing we get Voc=1.75V, Isc=7.55×10-11A and  Pmax=6.11×10 -9 W
Figure 6.21 I-V characteristics of AlGaAs-GaAs dual junction solar cell From figure 6.21 after analyzing we get Voc=1.75V, Isc=7.55×10-11A and Pmax=6.11×10 -9 W

InGaP-GaAs DUAL JUNCTION SOLAR CELL

  • Concentration Increasing
  • Concentration Decreasing
  • Changing Back Surface
  • Increasing Concentration for New BSF
  • Concentration Change for Wider Bandgap for New BSF
  • Concentration Change for Wider Bandgap for New BSF

From the above discussion, we can form a table in which we can summarize and show the change in efficiency for increasing concentration of InGaP and GaAs. In this case we get a higher efficiency as we reduce the concentration of the intersections.

Figure 6.26 P-V curve for high concentration  From figure 6.26 after analyzing we get, FF=91.24%  and  η=36.96%
Figure 6.26 P-V curve for high concentration From figure 6.26 after analyzing we get, FF=91.24% and η=36.96%

CONCLUSION

CONCLUSION

RECOMMENDATION FOR FUTURE WORK

Gambar

Figure 1.8 Black carbon nano tubes sit on top of the absorber-emitter layer,  collecting energy across the solar spectrum and converting it to heat
Figure 2.4 A 2-Axis Tracking system (It can move up to 270degree in the horizontal  and 75 degree vertical)
Figure 2.9 A forest of GaAs nano wires growing on a silicon substrate.
Figure 2.12 Cadmium Telluride Solar Panels
+7

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