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Transcript
Solar Cell Parameters
EELE408 Photovoltaics
Lecture 11: Solar Cell Parameters
# of EHP Collected
# of Photons
Electrical Current Out
SR 
Optical Power In
• Quantum Efficiency
Dr. Todd J. Kaiser
[email protected]
QE 
• Spectral Response
Department of Electrical and Computer Engineering
Montana State University - Bozeman
• Open Circuit Voltage
Output Voltage with no current flow
• Short Circuit Current
Output Current with no load
Plot of the Current versus Voltage for varying loads
• I-V Curve
• Fill Factor
Ratio of operating current and voltage product to the product of short circuit current and open circuit voltage

• Efficiency
Electrical Power Out
Optical Power In
2
I-V Curve
Short Circuit Current Point
Light
Current
Current
  qV  
I  I 0 exp
  1  I L
  nkT  
The short circuit current is the current
through the cell when the voltage across
the cell is zero (the solar cell is short
circuited)
I
IL
V
I sc
Voltage
The IV curve shifts as
the cell begins to
generate power
Voltage
Illluminating the cell adds to the “dark”
current of the diode
Since the cell is generating power
the convention is to invert the
current axis
The greater the intensity the greater the
shift
3
Short Circuit Current Dependence:
4
Approximated Current
• Area of Solar Cell
• Comparing solar cells of the same material the most critical
material parameters are the surface passivation and diffusion
lengths
• Ignoring passivation effects the short circuit current density
can be approximated as:
– To remove the dependence on solar cell area, it is common to use the
Short Circuit Current Density (Jsc in mA/cm2)
• Intensity of Light
– Isc is directly dependent on the number of photons entering the cell
• Spectrum of Light
– For
o most
os measurements
easu e e s the
e spec
spectrum
u is
s sstandardized
a da d ed to
o AM1.5
5
• G: generation rate
rate, L diffusion lengths
• Optical Properties of the Cell
– Reflection and absorption
J sc  qG Ln  L p 
• Collection Probability
– Chiefly depends on surface passivation and minority carrier lifetime
5
6
1
Possible Current Density
Open Circuit Voltage Point
• Silicon solar cells under illumination at AM1.5 spectrum
Current
– Maximum possible current density of 46 mA/cm2
– Laboratory devices have reached 42 mA/cm2
– Commercial silicon solar cells 28-35 mA/cm2
The open circuit voltage is the maximum
voltage available from the solar cell. It
occurs at the zero current point
I sc
Voc
Voltage
7
Open Circuit Voltage
8
Open Circuit Voltage Dependence:
• Corresponds to the amount of forward bias on the cell due to
the bias generated by the illumination of the cell
• Solve for the Voltage when the net current is set to zero
• Light Generated Current
– Function of the illumination (typically fixed at AM1.5)
• Saturation Current
– I0 can vary orders of magnitude
– Depends on the amount of recombination in the solar cell
  qV  
0  I 0 exp oc   1  I L
  nkT  
Voc 
• Temperature
nkT  I L 
ln  1
q
 I0

9
Possible Voltages
10
Power & IV Curve
• Silicon solar cells under illumination at one sun and AM1.5
spectrum
• Power (Watts) is the rate at which energy (Joules) is
supplied by a source or consumed by a load… It is a
rate not a quantity
• The power output by a source is the product of the
current supplied and the voltage at which the current was
supplied
• Power output = Source voltage x Source current
– P=V x I (Watts = Joules/second) = (Volts)x(Amperes)
• By changing the resistance of the load different currents
and corresponding voltages can be measured and
plotted
– Laboratory devices have reached 720 mV
– Commercial silicon solar cells 500-600 mV
11
12
2
Fill Factor
IV Plot
Short
Circuit
Current
Maximum
Power
• A measure of the “Squareness” of the IV curve
• The largest area rectangle that can fit with in the IV curve
divide by the rectangle formed by the product of the maximum
current (Isc) and maximum voltage (Voc)
• Maximum FF can be calculated by:
Imp
FF 
Operating
Point
I mpVmp
Current
I scVoc
Power
Vmp
Voltage (V)
Open Circuit
Voltage
Volt (V)
0
0.1
0.3
0.5
0.54
0.57
Current (A)
1.3
1.3
1.3
1.2
0.75
0
Power (W)
0
0.13
0.39
0.6
0.4
0


d IV 
nkT  Vmp

 0  Vmp  Voc 
ln 
 1
dV
q
 nkT


 q
Not useful: not closed form
and still need Imp
13
Fill Factor 2
14
Ideality Factor: “n” Factor
• More commonly used empirical expression
FF 
• Measure of the junction quality and types of recombination in
the junction
• Small and Simple recombination n=1
• Large and complex n=2
• A high n values degrades the fill factor
• Also high n values means significant recombination and
l
lowers
the
h open circuit
i i voltage
l
voc  lnvoc  0.72
voc  1
normali ed Voc : voc 
normalized
q
Voc
nkT
15
Efficiency
16
Efficiency Testing
• Most commonly used parameter to compare the performance
of one solar cell to another
• Defined as the ratio of energy output by the solar cell to input
energy from the sun
• Efficiency depends on:
• Conditions are carefully controlled to compare devices
• Terrestrial Solar Cells
– AM1.5
– 25⁰C
• Space orbiting Earth
– AM0
– Spectrum
– Intensity
– Temperature

Pmax Voc I sc FF

Pin
Pin
17
18
3
Characteristic Resistance
Measuring Short Circuit Current
• The characteristic resistance is the output resistance of the
solar cell at its maximum power point
I sc
I mp
Rch 
Current
Vmp
I mp

Voc
I sc
Inverse of the slope is the
characteristic resistance
Voltage
Vmp Voc
19
Measuring Open Circuit Voltage
20
Generating the IV Curve
21
22
Experimental Setup for IV Curve
Generation
IV Curve
• Measure Current and Voltage as the load connected to the
solar cell is changed
R=0
R=1
I sc
R=10
Current
R=100
R=1000
R=∞
Voltage
Voc
23
24
4