Modeling and Simulation of Photovoltaic Components of a Solar Power - - PowerPoint PPT Presentation

modeling and simulation of photovoltaic components of a
SMART_READER_LITE
LIVE PREVIEW

Modeling and Simulation of Photovoltaic Components of a Solar Power - - PowerPoint PPT Presentation

Modeling and Simulation of Photovoltaic Components of a Solar Power System Ajith Gopi Parsons Brinckerhoff Parson Brinckerhoff >14,000 people 150 offices six continents PB Power Asia 500 people Most major


slide-1
SLIDE 1

Modeling and Simulation of Photovoltaic Components of a Solar Power System

Ajith Gopi

slide-2
SLIDE 2

Parsons Brinckerhoff

  • Parson Brinckerhoff

– >14,000 people – 150 offices – six continents

  • PB Power Asia

– 500 people – Most major Asian cities – Asia-Pacific region since early 1990s – Engineering Support for solar and wind power development

slide-3
SLIDE 3

Recent Solar PV Modeling Experiences

  • LE’s Technical Advisor for

Multiple Solar PV Projects in China (25.5MW)

  • Technical Due Diligence
  • f PV Projects (20MW) in

Portugal for a client in Korea

  • LE for 25 MW Solar PV

project in Gujarat in India

slide-4
SLIDE 4

Contents

slide-5
SLIDE 5

PV Cell Model

The output current from the PV cell can be found using the equation: I=Isc-Id

(Where Isc is the short-circuit current that is equal to the photon generated current, and Id is the current shunted through the diode)

The diode current is given by the Schottky diode equation: Id= I0* (eq*Vd/(k*T) -1)

(Where Isc is the reverse saturation current of the diode (A), q is the electron charge (1.602 x 10-19C), Vd is the voltage across the diode (V), k is the Boltzmann’s constant (1.381x10-23 J/K) and T is the junction temperature in Kelvin (K))

slide-6
SLIDE 6

PV Cell Model (…continued)

Combining the diode current equation with the equation for the output current of the PV cell creates: I= Isc- I0* (eq*V/(k*T) -1) (Where V is the voltage across the PV cell, and I is the output current) We can solve for the reverse saturation current (I0) by setting I=0 (no

  • utput current).

I0= Isc (eq*Vd/(k*T) -1)

slide-7
SLIDE 7

More accurate model of a PV Cell

Taking into account the series Resistance, Shunt Resistance and Recombinations, the equation becomes: I= Isc – I01 * (eq*V+I*Rs /(k*T) -1) – I02* (eq*V+I*Rs /(2*k*T) -1)- (V+I*Rs)/Rp The two diodes can be combined to simplify the equation to: I= Isc – I0 * (eq*V+I*Rs /(n* k*T) -1) - (V+I*Rs)/Rp (Where n is known as the “ideality factor” and takes a value between one and two)

slide-8
SLIDE 8

Model of a PV Cell

The effect of the shunt resistance is minimal for a small number of modules. Therefore, we can assume Rp=∞ ∞ ∞ ∞, simplifying the photon-generated current equation to: I= Isc – I0 * (eq*(V+I*Rs /(n*k*T)-1)

slide-9
SLIDE 9

Simulink - PV Cell Model

slide-10
SLIDE 10

PV Cell Model I-V and Power Characteristics

slide-11
SLIDE 11

Simulink Implementation of PV Module

PV Modules are implemented as Masked Subsystems in Simulink in two Input modes

  • Current Input PV

Module

  • Voltage Input PV

Module

slide-12
SLIDE 12

Model parameters for the Simulink Model

Model parameters, in both cases, are the standard PV module data-sheet parameters:

  • Short-circuit current Isc
  • Open-circuit voltage Voc
  • Rated current Ir at maximum power

point (MPP)

  • Rated voltage Vr at MPP

(Under standard test conditions of 1kW/m2, 1.5 AM, 25oC).

slide-13
SLIDE 13

Simulink Implementation of a Current Input PV Module

Inputs:

  • PV current Ipv [A]
  • Insolation [W/m2]

Outputs:

  • PV voltage Vpv [V]
  • PV output power Ppv [W]

This model is well suited for the case when modules are connected in series and share the same current

slide-14
SLIDE 14

Simulink PV Module Model

slide-15
SLIDE 15

Simulink PV Module Model Sub System with Current Input (Ipv)

slide-16
SLIDE 16

Simulink Implementation of a Current Input PV Module

Inputs:

  • PV voltage Vpv [V]
  • Insolation [W/m2]

Outputs:

  • PV current Ipv [A]
  • PV output power Ppv [W]

This model is well suited for the case when modules are connected in parallel and share the same voltage

slide-17
SLIDE 17

PV Module Sub System with Voltage Input (Vpv) (Suitable for Parallel Connections)

slide-18
SLIDE 18

Simulink PV Module Model as a Software Tool for Performance Analysis

slide-19
SLIDE 19

PV Module Model – I-V and Power Characteristics

slide-20
SLIDE 20

Performance Comparison two PV Modules

Data Sheet Parameters of Module A Isc 2.5 A Voc 21.8 V Imp 2.3 A Vmp 17.3 V Power at S.T.C 40 W Data Sheet Parameters of Module B Isc 2.5 A Voc 21 V Imp 2.18 A Vmp 17 V Power at S.T.C 40 W

slide-21
SLIDE 21

I V Characteristics comparison and validating with PV Syst values

Fill Factor is more for Module A since the squareness of the curves is more for Module A. Hence Module A is more efficient than Module B

slide-22
SLIDE 22

Power Characteristics Comparison odf Module A & B

Fill Factor is directly proportional to the Power output of the PV Module Hence it is evident that

  • utput power of Module

A more compared to Module B

slide-23
SLIDE 23

Simulink – PV Array Model

(WITH SOLAR MODULE MODEL SUBSYSTEM BLOCK WITH CURRENT (Ipv) INPUT)

slide-24
SLIDE 24

Conclusions

  • Photovoltaic components of a Solar Power System are

mathematically modelled and then simulated in Matlab/Simulink.

  • Simulink models are implemented for:

Solar Cell, PV Module (Current Input Model and Voltage Input Model) & a typical Solar Array

  • Development of a Software tool for the PV Module Performance

Evaluation from the Module Data Sheet Parameters.

slide-25
SLIDE 25

Any Questions?

Thank you for your attention!

Further information please contact: Ajith Gopi Principal Engineer gopi.ajith@pbworld.com