2021 IEEE Conference on Energy Conversion (CENCON)
IEEE Catalog Number: CFP21CEO-ART ISBN: 978-1-6654-0129-6
2021 IEEE Conference on Energy Conversion (CENCON) | 978-1-6654-0129-6/21/$31.00 ©2021 IEEE | DOI: 10.1109/CENCON51869.2021.9627300
Message from General Chairs
On behalf of the CENCON 2021 organizing committee, we welcome you to the 5th IEEE Conference on Energy Conversion (CENCON 2021). This conference is organized and sponsored by the IEEE Power Electronics (PELS) Malaysia Chapter, co-organized by Power Electronics and Drives Research Group (PEDG), Universiti Teknologi Malaysia (UTM), and technical co-sponsor by The Korean Institute of Power Electronics (KIPE).
Every one of us has been affected by the Covid-19 pandemic since it started a couple of years ago.
We must not let the pandemic weaken us; in fact, we must move forward and do our best to control the spread of the virus. Because of this, we have decided to hold CENCON 2021 virtually. To ensure the best experience for the participants, the conference is conducted on a user-friendly platform that offers almost the same features as a physical conference. Our virtual conference this year will have 3 parallel sessions held in one day. Registered participants can join and move between any session they wish by joining any virtual breakout rooms. They can choose to watch the recorded presentation of the technical papers and keynote speeches at their convenient time. The contents will be available to the participants up to 2 weeks after the conference ends.
CENCON 2021 is our 5th conference, which is held bi-annually. The last CENCON was held physically in Jog Jakarta, Indonesia, in 2019. CENCON provides an excellent opportunity for researchers and academicians to discuss and present their findings. This year we are lucky to have two distinguished professors deliver the keynote speeches. They are Prof. Dr. Zainal Salam from UTM and Prof. Taufik from Calpoly, USA. CENCON 2021 has received 79 paper submissions. And out of this, 39 have been accepted for presentations. Papers accepted and presented at the conference will be submitted to the IEEE and included in the IEEE Xplore digital library. We notice that the number of submissions is relatively lower than the past CENCON; however, the submissions came from all over the world, including India, the USA, South Korea, Taiwan, Germany, South Africa and a few more.
We hope that you will enjoy this virtual conference from the comfort of your home, and hopefully, we will see you again in 2023 for our next CENCON. Thank you.
Nik Rumzi Nik Idris Rahimi Baharom
CENCON 2021 General Chairs
2021 IEEE Conference on Energy Conversion (CENCON) | 978-1-6654-0129-6/21/$31.00 ©2021 IEEE | DOI: 10.1109/CENCON51869.2021.9627243
Table of Contents
Message from General Chairs i
Table of Contents ii
Copyright Page vii
Author Index viii
Author Papers
Session 1A: Photovoltaic System
Session chairs: Tan Chee Wei & Razman Ayop
1A1 A Single-Phase Multilevel Inverter With Reduced Switch Count for Solar PV Application
1
Ali Bughneda (Universiti Sains Malaysia, Malaysia); Mohamed Salem (Universiti Sains Malaysia (USM), Malaysia); Dahaman Ishak (Universiti Sains Malaysia, Malaysia);
Salah Alatai (Universiti Sains Malaysia, Malaysia & Bani Waleed University, Libya);
Mohamad Kamarol Mohd Jamil (Universiti Sains Malaysia, Malaysia); Khlid Ben Hamad (Cape Peninsula University of Technology, South Africa)
1A2 Increasing the Efficiency of Photovoltaic Generation Using Parabolic Reflector 7 Udaya Santha Rahubadde (Kotelawala Defence Univerisity, Sri Lanka); Akmeemanage
Don Dinul Manjitha (General Sir John Kotelawala Defence University, Sri Lanka)
1A3 Performance of the Hybrid Photovoltaic-Thermoelectric Generator (PV-TEG) System Under Malaysian Weather Conditions
11
Umar Abubakar Saleh (University Tun Hussein Onn Malaysia & Centre for Atmospheric Research, NARSDA, Prince Audu Abubakar University Anyigba, Kogi, Malaysia); Siti Amely Jumaat (Universiti Tun Hussein Onn Malaysia, Malaysia);
Muhammad Akmal Johar (Universiti Tun Hussein Onn Malaysia & Smart Structure and System Research Group, Malaysia); Wan Akasha Wan Jamaluddin (University Tun Hussein Onn Malaysia, Malaysia)
1A4 Photovoltaic Emulator Using Particle Swarm Optimization 17 Razman Ayop, Chee Wei Tan, Mohd Zaki Daud, Shahrin Md. Ayob, Awang Jusoh and
Mohd Rodhi Sahid (Universiti Teknologi Malaysia, Malaysia)
1A5 Sizing of Photovoltaic Wind Battery System Integrated With Vehicle-To-Grid Using Cuckoo Search Algorithm
22
Abdulgader H Alsharif, Chee Wei Tan, Razman Ayop and Kwan Yiew Lau (School of Electrical Engineering Universiti Teknologi Malaysia, UTM Johor Bahru, Malaysia);
Chuen Ling Toh (Department of Electrical and Electronic Engineering Universiti Tenaga National Kajang, Malaysia)
1A6 Design and Integration of Valves Controller for Drone Monitored Solar Irrigation System
28
Firas Basim Ismail Alnaimi, Muhammad Luqman Syakir Rosli, Mohamed Najah Mahdi (Universiti Tenaga Nasional, Malaysia), Ranjani Vasu (GSPARX Tenaga Nasional Berhad)
2021 IEEE Conference on Energy Conversion (CENCON) | 978-1-6654-0129-6/21/$31.00 ©2021 IEEE | DOI: 10.1109/CENCON51869.2021.9627278
Session 1B: Power Converters
Session chairs: Naziha Ahmad Azli & Mohd Zaki Daud
1B1 Comparison of Efficiency of Double Conversion UPS With LC, LCL and LCL With Damping Resistor Filters
34
Robinson Kong and Mohd Zaki Daud (Universiti Teknologi Malaysia, Malaysia); Lee Kar Kuan (Universiti Teknlogi Malaysia, Malaysia)
1B2 Design of a Half-Bridge Converter for Self-Adapting Capacitive Wireless Power Transfer
40 Norbert Seliger (Technische Hochschule Rosenheim, Germany)
1B3 Multiple Input Single Output Converter With Uneven Load Sharing Control for Improved Efficiency
46
Kristen Chan, Taufik (Cal Poly State University, USA), Rini Nur Hasanah (Universitas Brawijaya Malang, Indonesia), Suprapto, Mentari Putri Jati, Aris Nasuha (Universitas Negeri Yogyakarta Yogyakarta, Indonesia)
1B4 Lithium-Ion Cell Balancing Using Auxiliary Battery and DC/DC Unidirectional Converter
52
Mohd Junaidi Abd Aziz (Universiti Teknologi Malaysia, Malaysia), Muhammad Hazwan Hashim, Mohd Saiful Jamaluddin, Mohd Hafidzuddin Sam Hun (Kolej Kemahiran Tinggi Mara Pasir Mas Kelantan, Malaysia)
1B5 Model Predictive Control for DC-DC Boost Converters 58 Ashish Choubey (PDPM, IIITDM, India); Sachin Kumar Jain (PDPM IIITDM Jabalpur, India); Prabin Padhy (PDPM, IIITDM Jabalpur (M. P.) India, India)
1B6 Phase-Shifted LLC Resonant DC-DC Converter for Battery Charging Application 64 Salah Alatai (Universiti Sains Malaysia, Malaysia & Bani Waleed University, Libya);
Mohamed Salem (Universiti Sains Malaysia (USM), Malaysia); Dahaman Ishak, Ali Bughneda and Mohamad Kamarol Mohd Jamil (Universiti Sains Malaysia, Malaysia);
Doudou N. Luta (University of Technology Cape Town, South Africa)
1B7 IMC-PID Control for Bidirectional Three Phase Active Front End Rectifier for Reference Tracking and Disturbance Rejection Capabilities
69
Azizah Abdul Razak, Norjulia Mohamad Nordin and Naziha Ahmad Azli (Universiti Teknologi Malaysia, Malaysia)
Session 1C: Inverters
Session chairs: Shahrin Md Ayob & Nik Din Mohamed
1C1 Open Circuit Fault Diagnosis for Multi-Level Inverters Using an Improved Current Distortion Method
75
Laith M. Halabi (Ajou University); Ibrahim M Alsofyani and Kyo-Beum Lee (Ajou University, Korea (South))
1C2 Open Fault Tolerant Method Using DPWM for Reducing Switching Loss in Three- Level Hybrid ANPC Inverter
80 Ha-Rang Jo (Ajou University, Korea (South)); Youngjong Ko (Pukyong National University, Korea (South)); Kyo-Beum Lee (Ajou University, Korea (South))
1C3 Performance Analysis of FCS-MPC Using the Generalized Formulation and Euler Method on Switched-Battery Boost Multilevel Inverter
85
Ahmad Takiyuddin Abdullah (Universiti Teknologi Malaysia & Universiti Kuala Lumpur Malaysia France Institute, Malaysia); Sevia Mahdaliza Idrus (Faculty Of Electrical Engineering & Universiti Teknologi Malaysia, Malaysia); Shahrin Md. Ayob (Universiti Teknologi Malaysia, Malaysia)
1C4 Quasi-Z-Source Four-Switch Three-Phase Inverter With Split Capacitor DC-Link Voltage Input
91
Izni Mustafar (Universiti Teknologi Malaysia, Malaysia & Universiti Sains Islam Malaysia, Malaysia); Naziha Ahmad Azli and Norjulia Mohamad Nordin (Universiti Teknologi Malaysia, Malaysia)
1C5 Single Phase Nine-Level Symmetrical Inverter Topology With Reduced Switch Count and Total Standing Voltage
97
Farogh Alam (Aligarh Muslim University, India); M Saad Bin Arif, Shahrin Md. Ayob and Razman Ayop (Universiti Teknologi Malaysia, Malaysia)
1C6 Zero-Sequence Circulating Current Suppression in Multi-Paralleled Three-Level NPC Inverters Under Unbalanced Operating Conditions
103 Kyo-Beum Lee and Jun-Hyeok Park (Ajou University, Korea (South))
Session 2A: Energy Conversion 1
Session Chairs: Toh Chuen Ling & NorJulia Mohamad Nordin
2A1 Characterization and Optimization of Lattice-Matched InGaAs TPV Cell for Waste Heat Harvesting
108
Mansur Gamel (Universiti Tenaga Nasional & Institute of Electrical Engineering, Malaysia); Pin Jern Ker (University Tenaga Nasional, Malaysia); Hui Jing Lee and M A Hannan (Universiti Tenaga Nasional, Malaysia)
2A2 Evaluation of Triboelectric Energy Generators Based on Military Textiles 114 Joseph Olanrewaju Adegite, Aaron McCutcheon, Nancy Nguyen, Eric Scholz, Rebecca
Serven, Spencer Tess, Gregory Noetscher and Pratap Rao (Worcester Polytechnic Institute, USA)
2A3 Experimental Investigations of FOV for Conventional and Hybrid Cylindrical Spacers in Compressed N2: SF6 Gas Mixture Under AC Voltages
120 Aman Ulla (Visvesvaraya Technological University, India)
2A4 Novel Method for Estimating State of Health for Lead-Acid Batteries 125 Ali Asger Khattab (IIT Bombay, India)
2A5 Optimization of InGaAsSb Thermophotovoltaic Cell for Waste Heat Harvesting Application
130
Rafiqi Rosli, Hui Jing Lee and Md Zaini Jamaludin (Universiti Tenaga Nasional, Malaysia); Mansur Gamel (Universiti Tenaga Nasional & Institute of Electrical Engineering, Malaysia); Pin Jern Ker (University Tenaga Nasional, Malaysia)
2A6 Simulation and Visualization of Occupancy-Based Energy Consumption in Campus Building Using SCADA Software
136
Aryuanto Soetedjo and Sotyohadi Sotyohadi (National Institute of Technology (ITN) Malang, Indonesia)
Session 2B: Energy Conversion 2
Session chairs: Mohd Junaidi Abd Aziz & Awang Jusoh
2B1 A Refined Predictive Torque Control for Two-Level Voltage Source Inverter of Induction Motor
142
Rozana Alik, Norjulia Mohamad Nordin and Nik Rumzi Nik Idris (Universiti Teknologi Malaysia, Malaysia)
2B2 Coal Fuel Efficiency With Mixed Palm Shell Biomass for Steam Power Plant 148 Hamzah Eteruddin, Muhammad Ridwan, Monice Monice and Zulfahri Zulfahri
(Universitas Lancang Kuning, Indonesia); Yanuar Arief (UNIMAS, Malaysia);
Fathimah Hasanti (Universiti Teknologi Malaysia, Malaysia)
2B3 Continuous-Time Sigma-Delta Modulator With Oscillator for Phase Locked Loop Wireless Controlled Power Applications
154 Wen Cheng Lai (National Taiwan University of Science and Technology, Taiwan)
2B4 Fuzzy Gain Scheduling for Cascaded PI-Control for DC Motor 158 Deany Putri Aulia, Alfiyah Yustin and Amien Hilman (Pertamina University, Indonesia); Aulia Annisa and Wahyu Kunto Wibowo (Universitas Pertamina, Indonesia)
2B5 Point Absorber With Direct-Drive Power Take-Off System for Low Wave Application
163
Jariyati Burhanudin and Asnor Mazuan Ishak (Universiti Pertahanan Nasional Malaysia, Malaysia); Taib Ibrahim (Universiti Teknologi Petronas, Malaysia); Ahmad Shukri Abu Hasim, Syed Mohd Fairuz Syed Mohd Dardin and Jariyani Burhanudin (Universiti Pertahanan Nasional Malaysia, Malaysia)
2B6 Reducing Power Loss Considering Massive Charging Station Using Metaheuristic Technique
169
Syed Norazizul Syed Nasir (Universiti Teknologi Malaysia, Malaysia); Wan Yusrizal Wan Yusoff (Tenaga Nasional Berhad, Malaysia); Jasrul Jamani Jamian and Razman Ayop (Universiti Teknologi Malaysia, Malaysia)
2B7 Modelling and Analysis of 18-Pulse Rectification System for DC Traction Power Substation
174 Chuen Ling Toh and Azrul Ikhwan Muhamad Shukran (Universiti Tenaga Nasional,
Malaysia); Chee Wei Tan (Universiti Teknologi Malaysia, Malaysia)
Session 2C: Power Quality and Power System Session chairs: Lau Kwan Liew & Mohd Rodhi Sahid
2C1 Active Power Filtering Solution for Improving Power Quality in Cold Ironed Electric Ships
180
Rahman Syed and Roberto Cervantes (Texas A&M University, USA); Irfan A Khan (Texas A&M University USA, USA); Atif Iqbal (Qatar University, Qatar); Shahrin Md.
Ayob (Universiti Teknologi Malaysia, Malaysia)
2C2 Analysis of Droop Control for Emulating Grid Synchronization Mechanism 185 Ronald Jackson and Shamsul Zulkifli (Universiti Tun Hussein Onn Malaysia, Malaysia); Mohamed Benbouzid (University of Brest, France); Suriana Salimin, Mubashir Khan and Garba Elhassan (Universiti Tun Hussein Onn Malaysia, Malaysia)
2C3 Energy Management Strategy and Capacity Planning of an Autonomous Microgrid: A Comparative Study of Metaheuristic Optimization Searching Techniques
190
Abba Lawan Bukar, Chee Wei Tan and Kwan Yiew Lau (Universiti Teknologi Malaysia, Malaysia); Chuen Ling Toh (Universiti Tenaga Nasional, Malaysia); Razman Ayop (Universiti Teknologi Malaysia, Malaysia); Ahmed Tijjani Dahiru (School of Electrical Engineering, Universiti Teknologi Malaysia, Malaysia)
2C4 Investigation of Single-Band and Multi-Band Power System Stabilizers Towards Transient Stability Improvement in Electrical Networks
196
Ahmad Adel Alsakati and Chockalingam Aravind Vaithilingam (Taylor's University, Malaysia); Jamal Alnasseir (Damascus University, Syria); Arthanari Jagadeeshwaran (Sona College of Technology, India)
2C5 Review of Market Clearing Method for Blockchain-Based P2P Energy Trading for Microgrid System
202
Nor Ashbahani Mohamad Kajaan, (Universiti Malaysia Perlis, Malaysia), Zainal Salam, Raja Zahilah Raja Mohd Radzi (Universiti Teknologi Malaysia, Malaysia)
2C6 Blockchain Applications and Challenges in Smart Grid 208 Ibrahim Alhamrouni (British Malaysian Institute, Universiti Kuala Lumpur); Younes
Zahraoui (British Malaysian Institute, Universiti Kuala Lumpur, Malaysia)
2C7 Stability Analysis in a Grid-Interactive Residential Nanogrid Using Markov Chains
214
Ahmed Tijjani Dahiru (School of Electrical Engineering, Universiti Teknologi Malaysia, Malaysia); Chee Wei Tan and Kwan Yiew Lau (Universiti Teknologi Malaysia, Malaysia); Chuen Ling Toh (Universiti Tenaga Nasional, Malaysia); Abba Lawan Bukar and Sani Salisu (Universiti Teknologi Malaysia, Malaysia)
IEEE Copyright
2021 IEEE Conference on Energy Conversion (CENCON)
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IEEE CATALOG NUMBER: CFP21CEO-ART
ISBN : 978-1-6654-0129-6
2021 IEEE Conference on Energy Conversion (CENCON) | 978-1-6654-0129-6/21/$31.00 ©2021 IEEE | DOI: 10.1109/CENCON51869.2021.9627266
Author Index
Aaron McCutcheon (Worcester Polytechnic Institute, USA) 2A2
Abba Lawan Bukar (Universiti Teknologi Malaysia, Malaysia) 2C3, 2C7 Abdulgader H Alsharif (Universiti Teknologi Malaysia, Malaysia) 1A5
Ahmad Adel Alsakati (Taylor's University, Malaysia) 2C4
Ahmad Shukri Abu Hasim (Universiti Pertahanan Nasional Malaysia, Malaysia) 2B5 Ahmad Takiyuddin Abdullah (Universiti Teknologi Malaysia Malaysia) 1C3 Ahmed Tijjani Dahiru (Universiti Teknologi Malaysia, Malaysia) 2C3, 2C7 Akmeemanage Don Dinul Manjitha (General Sir John Kotelawala Defence University, Sri Lanka) 1A2
Alfiyah Yustin (Universitas Pertamina, Indonesia) 2B4
Ali Asger Khattab (IIT Bombay, India) 2A4
Ali Bughneda (Universiti Sains Malaysia, Malaysia) 1A1, 1B6
Ali Bughneda (Universiti Sains Malaysia, Malaysia)
Aman Ulla (Visvesvaraya Technological University, India) 2A3
Amien Hilman (Universitas Pertamina, Indonesia) 2B4
Aris Nasuha (Universitas Negeri Yogyakarta Yogyakarta, Indonesia) 1B3 Arthanari Jagadeeshwaran (Sona College of Technology, India) 2C4 Aryuanto Soetedjo (National Institute of Technology (ITN) Malang, Indonesia) 2A6
Ashish Choubey (PDPM, IIITDM, India) 1B5
Asnor Mazuan Ishak (Universiti Pertahanan Nasional Malaysia, Malaysia) 2B5
Atif Iqbal (Qatar University, Qatar) 2C1
Aulia Annisa (Universitas Pertamina, Indonesia) 2B4
Awang Jusoh (Universiti Teknologi Malaysia, Malaysia) 1A4
Azizah Abdul Razak (Universiti Teknologi Malaysia, Malaysia) 1B7 Azrul Ikhwan Muhamad Shukran (Universiti Tenaga Nasional, Malaysia) 2B7
Chee Wei Tan (Universiti Teknologi Malaysia, Malaysia) 1A4, 1A5, 2B7,
2C3, 2C7 Chockalingam Aravind Vaithilingam (Taylor's University, Malaysia) 2C4
Chuen Ling Toh (Universiti Tenaga Nasional, Malaysia) 1A5, 2B7, 2C3
2C7
Dahaman Ishak (Universiti Sains Malaysia, Malaysia) 1A1, 1B6
Deany Putri Aulia (Universitas Pertamina, Indonesia) 2B4
Doudou N. Luta (University of Technology Cape Town, South Africa) 1B6
Eric Scholz (Worcester Polytechnic Institute, USA) 2A2
Farogh Alam (Aligarh Muslim University, India) 1C5
Fathimah Hasanti (Universiti Teknologi Malaysia, Malaysia) 2B2
Firas Basim Ismail Alnaimi (Universiti Tenaga Nasional, Malaysia) 1A6 Garba Elhassan (Universiti Tun Hussein Onn Malaysia, Malaysia) 2C2
Gregory Noetscher (Worcester Polytechnic Institute, USA) 2A2
Hamzah Eteruddin (Universitas Lancang Kuning, Indonesia) 2B2
Ha-Rang Jo (Ajou University, South Korea) 1C2
2021 IEEE Conference on Energy Conversion (CENCON) | 978-1-6654-0129-6/21/$31.00 ©2021 IEEE | DOI: 10.1109/CENCON51869.2021.9627259
Hui Jing Lee (Universiti Tenaga Nasional, Malaysia) 2A1, 2A5
Ibrahim Alhamrouni (Universiti Kuala Lumpur, Malaysia) 2C6
Ibrahim M Alsofyani (Ajou University, South Korea) 1C1
Irfan A Khan (Texas A&M University USA, USA) 2C1
Izni Mustafar (Universiti Sains Islam Malaysia, Malaysia) 1C4
Jamal Alnasseir (Damascus University, Syria) 2C4
Jariyani Burhanudin (Universiti Pertahanan Nasional Malaysia, Malaysia) 2B5 Jariyati Burhanudin (Universiti Pertahanan Nasional Malaysia, Malaysia) 2B5 Jasrul Jamani Jamian (Universiti Teknologi Malaysia, Malaysia) 2B6 Joseph Olanrewaju Adegite (Worcester Polytechnic Institute, USA) 2A2
Jun-Hyeok Park (Ajou University, South Korea) 1C6
Khlid Ben Hamad (Cape Peninsula University of Technology, South Africa) 1A1
Kristen Chan (Cal Poly State University, USA) 1B3
Kwan Yiew Lau (Universiti Teknologi Malaysia, Malaysia) 1A5, 2C3, 2C7
Kyo-Beum Lee (Ajou University, South Korea) 1C1, 1C2, 1C6
Laith M. Halabi (Ajou University, South Korea) 1C1
Lee Kar Kuan (Universiti Teknlogi Malaysia, Malaysia) 1B1
M A Hannan (Universiti Tenaga Nasional, Malaysia) 2A1
M Saad Bin Arif (Universiti Teknologi Malaysia, Malaysia) 1C5
Mansur Gamel (Universiti Tenaga Nasional, Malaysia) 2A1, 2A5
Md Zaini Jamaludin (Universiti Tenaga Nasional, Malaysia) 2A5
Mohamad Kamarol Mohd Jamil (Universiti Sains Malaysia, Malaysia) 1A1, 1B6
Mohamed Benbouzid (University of Brest, France) 2C2
Mohamed Najah Mahdi (Universiti Tenaga Nasional, Malaysia) 1A6
Mohamed Salem (Universiti Sains Malaysia, Malaysia) 1A1, 1B6
Mohd Hafidzuddin Sam Hun (Kolej Kemahiran Tinggi Mara Pasir Mas Kelantan, Malaysia) 1B4 Mohd Junaidi Abd Aziz (Universiti Teknologi Malaysia, Malaysia) 1B4
Mohd Rodhi Sahid (Universiti Teknologi Malaysia, Malaysia) 1A4
Mohd Saiful Jamaluddin (Kolej Kemahiran Tinggi Mara Pasir Mas Kelantan, Malaysia) 1B4
Mohd Zaki Daud (Universiti Teknologi Malaysia, Malaysia) 1A4, 1B1
Monice Monice (Universitas Lancang Kuning, Indonesia) 2B2
Mubashir Khan (Universiti Tun Hussein Onn Malaysia, Malaysia) 2C2 Muhammad Akmal Johar (Universiti Tun Hussein Onn Malaysia, Malaysia) 1A3 Muhammad Hazwan Hashim (Kolej Kemahiran Tinggi Mara Pasir Mas Kelantan, Malaysia) 1B4 Muhammad Luqman Syakir Rosli (Universiti Tenaga Nasional, Malaysia) 1A6
Muhammad Ridwan (Universitas Lancang Kuning, Indonesia) 2B2
Nancy Nguyen (Worcester Polytechnic Institute, USA) 2A2
Naziha Ahmad Azli (Universiti Teknologi Malaysia, Malaysia) 1B7, 1C4 Nik Rumzi Nik Idris (Universiti Teknologi Malaysia, Malaysia) 2B1 Nor Ashbahani Mohamad Kajaan (Universiti Malaysia Perlis, Malaysia) 2C5
Norbert Seliger (Technische Hochschule Rosenheim, Germany) 1B2
Norjulia Mohamad Nordin (Universiti Teknologi Malaysia, Malaysia) 1B7, 1C4, 2B1
Pin Jern Ker (University Tenaga Nasional, Malaysia) 2A1, 2A5
Prabin Padhy (PDPM, IIITDM Jabalpur (M. P.) India, India) 1B5
Pratap Rao (Worcester Polytechnic Institute, USA) 2A2
Rafiqi Rosli (University Tenaga Nasional, Malaysia) 2A5
Rahman Syed (Texas A&M University, USA) 2C1
Raja Zahilah Raja Mohd Radzi (Universiti Teknologi Malaysia, Malaysia) 2C5
Ranjani Vasu (GSPARX Tenaga Nasional Berhad, Malaysia) 1A6
Razman Ayop (Universiti Teknologi Malaysia, Malaysia) 1A4, 1A5, 1C5,
2B6, 2C3
Rebecca Serven (Worcester Polytechnic Institute, USA) 2A2
Rini Nur Hasanah (Universitas Brawijaya Malang, Indonesia) 1B3
Roberto Cervantes (Texas A&M University, USA) 2C1
Robinson Kong (Universiti Teknologi Malaysia, Malaysia) 1B1
Ronald Jackson (Universiti Tun Hussein Onn Malaysia, Malaysia) 2C2
Rozana Alik (Universiti Teknologi Malaysia, Malaysia) 2B1
Sachin Kumar Jain (PDPM IIITDM Jabalpur, India) 1B5
Salah Alatai (Bani Waleed University, Libya) 1A1, 1B6
Sani Salisu (Universiti Teknologi Malaysia, Malaysia) 2C7
Sevia Mahdaliza Idrus (Universiti Teknologi Malaysia, Malaysia) 1C3
Shahrin Md. Ayob (Universiti Teknologi Malaysia, Malaysia) 1A4, 1C3, 1C5, 2C1
Shamsul Zulkifli (Universiti Tun Hussein Onn Malaysia, Malaysia) 2C2 Siti Amely Jumaat (Universiti Tun Hussein Onn Malaysia, Malaysia) 1A3 Sotyohadi Sotyohadi (National Institute of Technology (ITN) Malang, Indonesia) 2A6
Spencer Tess (Worcester Polytechnic Institute, USA) 2A2
Suprapto, Mentari Putri Jati (Universitas Negeri Yogyakarta Yogyakarta, Indonesia) 1B3 Suriana Salimin (Universiti Tun Hussein Onn Malaysia, Malaysia) 2C2 Syed Mohd Fairuz Syed Mohd Dardin (Universiti Pertahanan Nasional Malaysia, Malaysia) 2B5 Syed Norazizul Syed Nasir (Universiti Teknologi Malaysia, Malaysia) 2B6
Taib Ibrahim (Universiti Teknologi Petronas, Malaysia) 2B5
Taufik (Cal Poly State University, USA) 1B3
Udaya Santha Rahubadde (Kotelawala Defence Univerisity, Sri Lanka) 1A2 Umar Abubakar Saleh (Prince Audu Abubakar University Anyigba, Kogi, ) 1A3
Wahyu Kunto Wibowo (Universitas Pertamina, Indonesia) 2B4
Wan Akasha Wan Jamaluddin (University Tun Hussein Onn Malaysia, Malaysia) 1A3
Wan Yusrizal Wan Yusoff (Tenaga Nasional Berhad, Malaysia) 2B6
Wen Cheng Lai (National Taiwan University of Science and Technology, Taiwan) 2B3
Yanuar Arief (UNIMAS, Malaysia) 2B2
Younes Zahraoui (Universiti Kuala Lumpur, Malaysia) 2C6
Youngjong Ko (Pukyong National University, South Korea) 1C2
Zainal Salam (Universiti Teknologi Malaysia, Malaysia) 2C5
Zulfahri Zulfahri (Universitas Lancang Kuning, Indonesia) 2B2
Biomass for Steam Power Plant
Hamzah Eteruddin Dept. of Electrical Engineering,
Faculty of Engineering Universitas Lancang Kuning
(UNILAK),
Jl. Yos Sudarso, km 8 Rumbai, 28265 Rumbai, Riau, Indonesia
[email protected] Zulfahri
Dept. of Electrical Engineering, Faculty of Engineering Universitas Lancang Kuning
(UNILAK),
Jl. Yos Sudarso, km 8 Rumbai, 28265 Rumbai, Riau, Indonesia
Muhammad Ridwan Dept. of Electrical Engineering,
Faculty of Engineering Universitas Lancang Kuning
(UNILAK),
Jl. Yos Sudarso, km 8 Rumbai, 28265 Rumbai, Riau, Indonesia
[email protected] Yanuar Z. Arief
Dept. of Electrical and Electronic Eng., Faculty of Engineering Universiti Malaysia Sarawak
(UNIMAS)
Kota Samarahan, Sarawak, Malaysia [email protected]
Monice
Dept. of Electrical Engineering, Faculty of Engineering Universitas Lancang Kuning
(UNILAK),
Jl. Yos Sudarso, km 8 Rumbai, 28265 Rumbai, Riau, Indonesia
[email protected] Fathimah Hasanti Dept. of Computer Network &
Security, Faculty of Engineering Universiti Teknologi Malaysia (UTM)
Skudai, Johor Bahru, Malaysia [email protected]
Abstract—The accumulation of coal-based fuels is depleting and to obtain coal fuel requires a great amount of money, as a corollary, measures must be taken to reduce the usage of this fuel. PT. Pembangkit Jawa Bali (PJB) is currently investigating the co-firing technique by using oil palm shell biomass waste as a combination coal fuel with a proportion of 95% coal and 5%
palm shell, the efficiency results will be compared to 100% of coal fuel. In this research, the Mathcad program and the Professional Simulator 8 were employed, the specific fuel consumption (SFC) technique is used to determine the efficiency of production expenses, as well as the direct and indirect methods to calculate the boiler efficiency. The results reveal that 4.09 IDR/kWh reduction in primary energy expenses could be achieved (0.65%). Co-firing fuel will undoubtedly have a significant impact on the boiler's performance, therefore when using 100% of coal as a fuel, the boiler efficiency value is 63.38%
(Direct Method), while using the Indirect Method will produce up to 82.24%, respectively. However, when using co-firing fuel with 95% of coal and 5% of palm shell (Direct Method), the boiler efficiency value is 63.92%, and 83.71% when using the Indirect Method.
Keywords— Co-firing method, production cost efficiency, palm shell, biomass, boiler efficiency, direct method, indirect method
I. INTRODUCTION
Electric power generation, both new renewable energy and fossil energy generation, has been widely investigated [1]–[6].
A boiler in a Steam Power Plant (SPP) is a facility that transforms liquid water to steam. Boilers use Circulating Fluidized Bed Combustion (CFBC) as one of its technologies [7–10]. The system has several advantages of working principles such as a compact boiler design, fuel flexibility, high combustion efficiency and low emission of harmful pollutants such as Sulfur Oxide (SOx) and Nitrogen Oxide (NOx) [7]. Coal is the primary fuel, however biomass such as palm shells, sawdust, or other agricultural waste can also be used in boilers only if it mixed. [11–13].
The SPP Tenayan power station in Riau province, Indonesia has a capacity of 2×110 MW and it is one of the PLN power plants run by PT. PJB that utilizes low calories or Low Rank Coal (LRC) with a heating value of 3,800 – 4,700
kCal/kWh as a fuel [14], [15]. LRC has a high sulfur concentration, which is bad for equipment, particularly the tube Boiler. SPP Tenayan uses a Circulating Fluidized Bed (CFB) boiler, which has a wide range of fuel options, high combustion efficiency, effective sulfur absorption, low NOx emissions, and a lower furnace cross section. [16], [17].
Riau Province is home to a palm oil plant with a capacity of 12,170 tons per hour [18]. The potential for Palm Kernel Shell (PKS) or biomass waste is very substantial in terms of shifting away from reliance on fossil fuels and toward green power plants. Increasing the Medium-Rank Coal (MRC) ratio, contributed to higher furnace bed and intake cyclone temperatures [15], [19]. Meanwhile, the implementation of CFB at the SPP Tenayan supports co-firing experiments using palm shell biomass. This study discusses the comparison of the fuel efficiency of pure coal and coal with a mixture of PKS biomass in Boiler Unit 2 at PT. PJB Tenayan Raya using specific fuel consumption technique (SFC).
II. METHOD
The Specific Fuel Consumption (SFC) can be used to determine an-engine's economic value [20], [21]. SPLN No.
80 (1989) says, this parameter can be used to compute the amount of fuel required to create a specified amount of power in a given time interval. The following are some of the formulas that are used to calculate the particular fuel consumption [22]:
a) Specific Fuel Consumption Brutto (SFCB)
6 3
3.6 10 10 g/kWh (h LHV)
f eff
SFC m P
= × = (1)
Where mf is the fuel consumption in kg/s, Peff is power (brake) effective machine, the efficiency (η) of the engine, and LHV which is the lower calorific value fuel in kWh/kg, SFC gross = Qf/(kWh(gross)).
b) Specific Fuel Consumption Netto (SFCN) SFC netto = Qf/(kWh(netto))
2021 IEEE Conference on Energy Conversion (CENCON) | 978-1-6654-0129-6/21/$31.00 ©2021 IEEE | DOI: 10.1109/CENCON51869.2021.9627271
rate:
a). Heat Rate brutto (HRB) = (Mf ×LHV)/(kWhB) b). Heat Rate netto (HRN) = (Mf ×LHV)/(kWhB-kWhPS) Where:
Qf : Quantity of coal used (kg)
LHV : Lower calorific value of the utilized fuel (kCal/kg) HHV : Higher calorific value of the utilized fuel (kCal/kg) kWhB : Number of kWh generated by generator (kWh) kWhps : Number of kWh required for personal use (kWh) Mf : Fuel weight during test (kg)
Heat Rate Brutto (HRB) is the amount of fuel heat computed to produce each gross kWh based on the calorific value (LHV). The following is the formula for estimating the cost of producing energy per kWh. Electricity production cost is SFCnett (kg/kWh) x Coal price (IDR/kg).
Boiler Efficiency
The percentage of fuel heat energy (heat input) that is effectively used in the steam produced is referred to as a boiler's thermal efficiency. Alternatively, boiler efficiency is referred to as the work performance or level of boiler performance determined from the comparison of the energy transmitted to the working fluid or absorbed by the working fluid in the boiler with the heat energy input of the fuel.
According to the USA Standard ASME PTC 4-1 Power Test Code for Steam Generating Units, there are two methods for evaluating boiler efficiency are Direct Method, where energy is transferred to the working fluid (water and steam) rather than the heat energy of the fuel boilers, and the Indirect Method, where efficiency is the difference between the percentage of heat entering and the percentage of loss that occurs [23].
A. Direct Method
An engine's efficiency is a measurement of its performance. The value of the level of boiler performance capability resulting from a comparison of energy output (output) and energy input (input) is defined as the efficiency of the boiler engine. The direct / input – output technology is mainly referred as because the efficiency value is calculated by dividing the output or output (steam) with the heat input or input (fuel). As a result, the boiler efficiency (ƞBoiler) equation is (heat output)/(heat input)×100%, or as follows [24], [25]:
ƞBoiler = 𝑄𝑄 (ℎ𝑔𝑔−ℎ𝑓𝑓)
𝑞𝑞 ×𝐺𝐺𝐺𝐺𝐺𝐺 × 100%
Where:
Q = Total steam yield (kg/hour).
q = Total fuel consumption (kg/hour).
hg = Saturated steam enthalpy (kkal/kg).
hf = Feed water enthalpy (kkal/kg).
GCV = Fuel gross heat value (kkal/kg).
B. Indirect Method
The indirect method utilizes the difference between the input energy and the losses. This technique is often referred to as the heat loss technique. A coal-fired boiler and a fuel analysis provide the necessary information for the indirect technique. There are several things in the Coal fired boiler data, such as: the amount of fuel that enters every hour, the
the steam output, the temperature of the feed water, the content of CO2 and CO levels, the temperature of the exhaust gases, the ambient temperature, the humidity of the ambient air, the surface temperature of the boiler, wind speed around the boiler, the total surface area of the boiler, the GCV value of bottom ash and fly ash. The fuel analysis data includes information on coal's ash content, carbon, hydrogen, nitrogen, oxygen, sulfur, and HHV values. The boiler has eight heat losses, as shown in the calculation below, according to the ASME PTC 4-1 standard.
a). Estimate the total heat loss (%).
Heat loss due to dry flue gas (L1) L1 = (m×cp×(Tf-Ta))/GCV ×100 Where:
m = Mass of dry exhaust gas (kg/fuel)
Cp = Specific heat of dry exhaust gas (kCal/kg) GCV= Calorific coal value (kCal/kg)
Tf = Exhaust gas temperature (°C) Ta = Temperature ambient (°C) b). Heat loss due to H2 in fuel (L2)
L2 = (9×H2×(584×Cp(Tp-Cp)))/GCV 100 Where:
H2 = The number of hydrogen atoms in the fuel (kg/kg fuel)
Cp = Specific heat of superheated steam (kCal/kg) 584 = The latent heat associated with the partial pressure
of water vapor (kCal/kg) GCV= Calorific coal value (kCal/kg) Tf = Exhaust gas temperature (°C) Ta = Temperature ambient (°C) c). Heat loss due to moisture in fuel (L3)
L3 = (M×(584×CP(Tf-Ta)))/GCV 100 Where:
M = Moisture in fuel (kg/kg fuel)
Cp = Specific heat of superheated steam (kCal/kg 0C) 584 = The latent heat associated with the partial pressure
of water vapor (kCal/kg) GCV= Calorific coal value (kCal/kg) Tf = Exhaust gas temperature (°C) Ta = Temperature ambient (°C) d). Heat loss due to moisture in air (L4)
L4 = (AAS×humidity factor×Cp(Tf-Ta))/GCV 100 Where:
AAS = Actual mass of air (kg/kg fuel) Humidity factor = 0,023
Cp = Specific heat of superheated steam (kCal/kg) GCV = Calorific coal value (kCal/kg)
Tf = Exhaust gas temperature (°C) Ta = Temperature ambient (°C)
e). Heat loss due to incomplete combustion (L5) L5 =(%CO×C×5744)/((%CO+%CO2)×GCV)×100
CO = Volume of CO in exhaust gas (%) CO2 = Actual volume of CO2 in exhaust gas (%) C = Carbon content (kg/kg fuel)
GCV = Calorific coal value (kCal/kg) f). Heat loss due to radiation and convection (L6)
4 4
6 0.548 1.25
1
1 9
.957 ( )
55.5 9
5 5
6.85 68
.55 .
L Ts 5Ta Ts a
Vm
T
+ −
= × − ×
× ×
+ Where:
Vm = Wind velocity (m/s) Ts = Surface temperature (K) Ta = Temperature ambient (K) g). Heat loss due unburnt in fly ash (L7)
(Total Ash Collected/kg of Fuel Burn) GCV of Fly 0 l
Ash 10 7 t
of Fue
L GVC
×
= ×
h). Heat loss due unburnt in bottom ash (L8) GCV of Fly Ash 100
8
of Fuel Total botom colected fuel
L GVC
×
= ×
Boiler efficiency is obtained by subtracting 100 with all losses
η𝑏𝑏𝑏𝑏𝑏𝑏𝑏𝑏𝑏𝑏𝑏𝑏 = 100 – (𝐿𝐿1 + 𝐿𝐿2 + 𝐿𝐿3 + 𝐿𝐿4 + 𝐿𝐿5 + 𝐿𝐿6 + 𝐿𝐿7 + 𝐿𝐿8)
III. RESULT AND DISCUSSION
The SFC comparison was calculated at a load of 89 MW Gross in two fuel trials, namely circumstances utilizing 100%
coal and co-firing conditions using 5% Palm Shells, as shown in Table 1.
TABLE I. SFCCALCULATIONS FOR OPERATING CONDITIONS
Parameter Co-Firing Test
0 % PKS 5 % PKS
Gross Load Setting, MW 89.00 89.00
Gross Electrical Energy, kWh 350,276 346,680 Net Electrical Energy, kWh 306,081 302,749 2A CF Fuel Consumption, kg 50,219 54,594 2B CF Fuel Consumption, kg 100,000 102,000 2C CF Fuel Consumption, kg 103,000 92,000 2D CF Fuel Consumption, kg 52,000 48,000 Total Fuel Consumption, kg 305,219 296,594 Specific Fuel Consumption, kg/kWh 0.871 0.856
Table 1 shows the results of SFC calculations for operating conditions involving 100% coal and 5% palm shell co-firing.
Figure 1 shows a comparison of Specific Fuel Consumption (SFC) for 100% coal and co-firing 95% coal 5
% palm shells.
Fig. 1. Comparisson graph of SFC values of 100% Coal and 5% Palm Oil.
Specific fuel consumption Rp. 0.871 kg/kWh with 100%
coal and Rp. 0.856 kg/kWh for (95% BB + 5%PKS).
a) Production cost of 100% coal:
Production price
= Coal Price× SFC 100% BB
= 720 IDR/kg × 0.871 kg/kWh
= 627.38 IDR/kWh
Production cost of co-firing 5%:
Production price
= Cost (5% PKS+95%BB)×SFC co-firing 5%
= {(0.05 × Rp. 900 + 0.95 × Rp.720)}×0.855/kWh
= Rp. 623.29 /kWh
As a result, when 5% palm shells are co-fired with 100%
coal, the difference in production costs is:
= 627.38 IDR/kWh – 623.29 IDR/kWh
= 4.09 IDR/ kWh
The following calculations are performed to obtain the percentage of production cost efficiency:
= (4.09 IDR/kWh)/(627.38 IDR/kWh) × 100 %
= 0.00651 × 100 % = 0.65%
Based on the aforementioned calculations, the efficiency value of the production cost comparison between 100% coal fuel and co-firing fuel, 95% coal and 5% palm shell, is 4.09 IDR/kWh or 0.65% more efficient co-firing fuel than pure coal fuel.
Boiler Efficiency Comparison
As demonstrated in Table 2, the co-firing fuel 95% coal 5% PKS has a higher boiler efficiency estimate than 100%
coal.
TABLE II. BOILER EFFICIENCY COMPARISON
Fuel Boiler Efficiency Application Results (%) 100 %
Coal
Direct Method MathCad 63.38
Simulator Profesional 8 63.38
Indirect Method MathCad 81.60
Simulator Profesional 8 80.29 95% Coal
&
5% PKS
Direct Method MathCad 63.92
Simulator Profesional 8 63.92
Indirect Method MathCad 83.14
Simulator Profesional 8 83.71 87,10%
85,60%
0%
20%
40%
60%
80%
100%
95% Coal 5% PKS 100% Coal
95% Coal 5% PKS 100% Coal
Efficiency (%)
The results of the boiler efficiency comparison can be seen in the graph shown in figure 2 below.
Fig. 2. Boiler Efficiency Comparison
According to the results of the boiler efficiency calculations shown in the previous graph, co-firing fuel can increase boiler efficiency by 0.12% using the Direct Method with Mathcad calculations and simulations, while using the Indirect Method calculation can increase boiler efficiency by 1.54% using (Mathcad) and 3.42% using (Simulation).
Palm Shell Demand Co-firing
To enhance the percentage of palm shell biomass in the co- firing test, the required fuel requirements must be predicted, as well as the fuel required to increase the percentage of the co-firing test, as indicated in Table 3.
TABLE III. PREDICTION OF CO-FIRING FUEL DEMAND
Co-firing 24 Hours 30 Days
5 % PKS 95 % Coal 3,648 Tons 109,440 Tons 5 % PKS 192 Tons 5,760 Tons 10 % PKS 90 % Coal 3,456 Tons 103,680 Tons 10 % PKS 384 Tons 11,520 Tons 15 % PKS 85 % Coal 3,264 Tons 97,920 Tons 15 % PKS 576 Tons 17,280 Tons
Based on the results of the survey on palm shell production in Table 3 and the availability of palm shells at PT. ATM and PT. EPE, the percentage of palm shells co-firing experiments should be increased to 10% - 15%. Both companies are still able to help with the current percentage of palm shells available. However, in the long run, the demand for palm shells supplies will grow year after year, so collaboration with other companies that can give palm shells supplies is encouraged to cover the expenses.
Operation Data Parameters During Co-Firing Test Observations were made on several elements that need to be monitored during the co-firing test, which were sourced from the co-firing test report data at PT. PJB SPP Tenayan Raya, to find out the comparison findings achieved in the 100% coal test results and the co-firing test results. When working with 95% coal and 5% palm shells, several factors must be taken into consideration [14].
a) Load – FEGT Temperature
Table 4 shows the results of observing Co-firing operation data on the Furnace Exit Gas Temperature parameter.
Time Load (MW) FEGT (°C)
0% PKS 5% PKS 0% PKS 5% PKS
11:00 88.499 87.455 868.905 843.014
11:30 89.722 86.622 873.548 845.159
12:00 89.145 87.691 859.611 849.094
12:30 87.854 88.045 853.266 852.434
13:00 88.795 87.736 858.735 852.955
13:30 88.559 87.455 860.146 853.092
14:00 88.395 88.499 855.442 855.356
14:30 89.322 88.549 863.058 853.586
15:00 88.982 88.549 860.911 855.898
Fig. 3. Comparison Graph of Furnace Exit Gas Temperature 0% Palm Shell and 5% Palm Shell
When testing co-firing 5% of palm shells with a similar load (89 MW), it is shown that the FEGT value with 5% of palm shells is lower than when using 100% BB. This is due to the fact that PKS has a lower density than coal and a higher Volatile Matter (VM), making PKS more combustible in the bed furnace region while decreasing FEGT values are still safe for operation.
b) Load – Bed Temperature
Table 5 shows the findings of the Bed Temperature parameter observation of the Co-firing operation data.
TABLE V. OBSERVATION OF LOAD OPERATION DATA –BED
TEMPERATURE
Time Load (MW) Bed Temp (°C)
0% PKS 5% PKS 0% PKS 5% PKS
11:00 88.499 87.455 816.305 812.766
11:30 89.722 86.622 818.200 809.775
12:00 89.145 87.691 818.212 812.322
12:30 87.854 88.045 814.707 816.051
13:00 88.795 87.736 817.871 813.810
13:30 88.559 87.455 819.510 811.872
14:00 88.395 88.499 817.331 819.654
14:30 89.322 88.549 821.272 819.340
15:00 88.982 88.549 820.038 821.837
63,8
81,6
63,92
83,14 63,8
80,29
63,92
83,71
0 20 40 60 80 100
100% Coal Direct
method 100% Coal
Indirect Method 95% Coal 5% PKS
Direct Method 95% Coal 5% PKS Indirect Method
Efficiency (%)
Mathcad Simulator
Fig. 4. Comparison Graph of Bed Temperature 0% Palm Shell and 5%
Palm Shell
Co-firing 5% palm shells with a similar load (89MW) was put to the test. Due to lower density and greater VM than coal, the bed temperature trend tends to increase (up to a maximum of 3 oC) when employing 5% PKS, causing combustion to occur in the lower furnace. Meanwhile, the 5% PKS test trend of increasing bed temperature is still safe to operate.
c) Load – Coal Flow
Table 6 shows the findings of observations of Co-firing operation data on Coal Flow characteristics.
TABLE VI. OBSERVATION OF OPERATION DATA LOAD –COAL FLOW
Time Load (MW) Total coal flow (t/h)
0% PKS 5% PKS 0% PKS 5% PKS
11:00 88.499 87.455 76.134 74.139
11:30 89.722 86.622 77.155 74.225
12:00 89.145 87.691 76.478 75.282
12:30 87.854 88.045 76.476 75.923
13:00 88.795 87.736 77.420 74.296
13:30 88.559 87.455 76.012 73.993
14:00 88.395 88.499 78.038 73.890
14:30 89.322 88.549 77.102 75.262
15:00 88.982 88.549 78.790 73.889
Fig. 5. Comparison Graph of Coal Flow 0% Palm Shell and 5% Palm Shell
When testing co-firing 5% palm shells with a similar load (89MW), it shows that: Coal biomass flow is somewhat lower than when using 100% BB, which is related to PKS having a higher calorific value than the coal used in SPP Tenayan. This
cleaner (export standards).
d) Air Chamber Pressure
Table 7 summarizes the output of analyzing the Load – Air Chamber Pressure parameters after watching the Co-firing operation data.
TABLE VII. LOAD –AIR CHAMBER PRESSURE
Time Load (MW) Air Chamber Preasure (Kpa)
0% PKS 5% PKS 0% PKS 5% PKS
11:00 88.499 87.455 12.605 12.569
11:30 89.722 86.622 12.641 12.491
12:00 89.145 87.691 12.674 12.554
12:30 87.854 88.045 12.658 12.426
13:00 88.795 87.736 12.449 12.488
13:30 88.559 87.455 12.531 12.491
14:00 88.395 88.499 12.550 12.606
14:30 89.322 88.549 12.606 12.591
15:00 88.982 88.549 12.414 12.526
Fig. 6. Comparison Graph of Air Chamber Pressure 0% Oil Palm Shells and 5% Palm Shells
When testing co-firing 5% Palm shells with a similar load (89MW), it can be shown that: Air chamber pressure is relatively constant (stable) when examining 5% PKS compared to full coal data, indicating that there is no nozzle obstruction or agglomeration.
e) Load – Sealpot Temperature
Table 8 shows the results of observing the Co-firing operation data on the Load – Sealpot temperature parameters.
TABLE VIII. SEALPOT TEMPERATURE
Time Load (MW) Sealpot Temperature (°C)
0% PKS 5% PKS 0% PKS 5% PKS
11:00 88.499 87.455 932.789 924.835
11:30 89.722 86.622 938.529 921.069
12:00 89.145 87.691 932.593 923.015
12:30 87.854 88.045 928.585 928.503
13:00 88.795 87.736 931.166 927.022
13:30 88.559 87.455 931.476 924.523
14:00 88.395 88.499 931.011 928.580
14:30 89.322 88.549 935.952 928.745
15:00 88.982 88.549 935.738 929.592
Fig. 7. Comparison Graph of Sealpot Temperature 0% Palm Shell and 5%
Palm Shell
When testing co-firing 5% Palm Shells with a similar load (89 MW), it was discovered that: a). The sealpot temperature was decreased when testing 5% Palm Shells compared to pure coal data, indicating that there is no combustion delay. b).
Before it reaches the sealpot, coal biomass is already burned in the furnace.
IV. CONCLUSION
With SFC difference of 0.016 kg/kWh, a coal price of 720 IDR/kg, and a palm shell price of 900 IDR/kg, the operation at the SPP Tenayan utilizing the co-firing method of 5% palm shells at a load of 89 MW gross can minimize primary energy costs by 4.09 IDR/kWh (0.65%). From Fig. 2 for boiler efficiency, it can be seen that co-firing fuel can boost boiler efficiency by 0.12% (Direct Method), while using the Indirect Method by 1.54% (Mathcad), and 3.42% using Simulator Professional 8, respectively.
Observation of operating conditions on boiler unit 2 of SPP Tenayan with a similar load of 89 MW reveals changes in numerous parameters when the ratio is between 100% coal and 5% co-firing. For instance, FEGT drops by 10 °C, Bed Temperature drops by 4 °C, and coal flow drops by 5 °C, respectively. As a result, the value of SFC decreased to 0,016 kg/kWh.
It can be observed from the calculation results that using 5% of co-firing fuel can reduce production costs as well as enhancing biogas production, thus palm shell percentage must be added to reach a higher efficiency value. In context of Table 3 on palm shell availability for long-term use, it is required to assess the availability of oil palm shells in the Riau area in order to fulfill the long-term fuel demands.
ACKNOWLEDGMENT
We would like to thank to PT. Pembangkit Jawa Bali (PJB) and Universitas Lancang Kuning for providing us the financial and technical support to conduct this study.
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