power generation from renewable energy sources

Power Generation from Renewable Energy Sources

Fall 2013Instructor: Xiaodong Chu

Email ： [email protected] Tel.: 81696127

mailto:[email protected]

Flashbacks of Last Lecture

• There are two conditions for the actual PV and for its equivalent circuit: – The current that flows when the terminals are shorted together (the

short-circuit current, ISC)

– The voltage across the terminals when the terminals are left open (the open-circuit voltage, VOC)


• The PV equivalent circuit includes both series and parallel resistances as

P

SSSC R

RIV

kT

RIVqIII 1

)(exp0


• The basic building block for PV applications is a module consisting of a number of pre-wired cells in series, all encased in tough, weather-resistant packages

• Multiple modules can be wired in series to increase voltage and in parallel to increase current, the product of which is power referred to as an array


• Example 8.3 of the textbook

Photovoltaic Materials and Electrical Characteristics–Shading impacts on I–

V curves• The output of a PV module can be reduced dramatically when

even a small portion of it is shaded• External diodes can help preserve the performance of PV

modules– The main purpose for such diodes is to mitigate the impacts of

shading on PV I –V curves– Such diodes are usually added in parallel with modules or blocks of

cells within a module


V curves • Consider an n-cell module with current I and output voltage V

shows one cell separated from the others• In the sun, the same current I flows through each of the cells• In the shade, the current source of the shaded cell ISC is

reduced to zero; the voltage drop across RP as current flows through it causes the diode to be reverse biased, so the diode current is also zero


V curves• Consider the case when the bottom n − 1 cells still have full

sun and still carry their original current I so they will still produce their original voltage Vn−1

• The output voltage of the entire module VSH with one cell shaded will drop to

• The voltage of the bottom n − 1 cells will be

• Then

1 ( )SH n P SV V I R R

1

1n

nV V

n

1( )SH P S

nV V I R R

n


V curves• The drop in voltage ΔV at any given current I , caused by the

shaded cell, is given by

• Since the parallel resistance RP is much greater than the series resistance RS

11 ( )SH P SV V V V V I R Rn

( )P S

VV I R R

n

P

VV IR

n


V curves• At any given current, the I –V curve for the module with one

shaded cell drops by ΔV


V curves• Example 8.6 of the textbook


V curves• The voltage drop problem in shaded cells could be to corrected

by adding a bypass diode across each cell• When a solar cell is in the sun, there is a voltage rise across the

cell so the bypass diode is cut off and no current flows through it—it is as if the diode is not even there

• When the solar cell is shaded, the drop that would occur if the cell conducted any current would turn on the bypass diode, diverting the current flow through that diode

• Since the bypass diode, when it conducts, drops about 0.6 V, the bypass diode controls the voltage drop across the shaded cell, limiting it to a relatively modest 0.6 V instead of the rather large drop that may occur without it


V curves• In real modules, it would be impractical to add bypass diodes

across every solar cell, but manufacturers often provide at least one bypass diode around a module to help protect arrays, and sometimes several such diodes around groups of cells within a module

• These diodes do not have much impact on shading problems of a single module, but they can be very important when a number of modules are connected in series

• Just as a single cell can drag down the current within a module, a few shaded cells in a single module can drag down the current delivered by the entire string in an array


V curves


V curves• When any of the cells are shaded, they cease to produce

voltage and instead begin to act like that cause voltage to drop as the other modules continue to try to push current through the string

• Without a bypass diode to divert the current, the shaded module loses voltage and the other modules try to compensate by increasing voltage, but the net effect is that current in the whole string drops

• If bypass diodes are provided, current will go around the shaded module and the charging current bounces back to nearly the same level that it was before shading occurred


V curves• Bypass diodes help current go around a shaded or

malfunctioning module within a string• This not only improves the string performance, but also

prevents hot spots from developing in individual shaded cells• When strings of modules are wired in parallel, a similar

problem may arise when one of the strings is not performing well

• Instead of supplying current to the array, a malfunctioning or shaded string can withdraw current from the rest of the array

• By placing blocking diodes, the reverse current drawn by a shaded string can be prevented


V curves

Photovoltaic Materials and Electrical Characteristics–Crystalline Silicon

Technologies• There are a number of ways to categorize photovoltaics

– Thickness of the semiconductor– Extent to which atoms bond with each other– Heterogeneity of p and n material

Photovoltaic Materials and Electrical

Characteristics–Crystalline Silicon Technologies

• On the thickness of the semiconductor– Conventional crystalline silicon solar cells are relatively thick—on the

order of 200–500 μm– An alternative approach to PV fabrication is based on thin films of

semiconductor—on the order of 1–10 μm



• On the extent to which atoms bond with each other in individual crystals– Single crystal, the currently dominant silicon technology– Multicrystalline, in which the cell is made up of a number of relatively

large areas of single crystal grains, each on the order of 1 mm to 10 cm in size

– Polycrystalline, with many grains having dimensions on the order of 1 μm to 1 mm

– Microcrystalline, with grain sizes less than 1 μm– Amorphous, in which there are no single-crystal regions



• On whether the p and n regions of the semiconductor are made of the same material– With the same material, they are called homojunction PVs– When the p–n junction is formed between two different

semiconductors, they are called heterojunction PVs



• Multiple junction solar cells are made up of a stack of p–n junctions with each junction designed to capture a different portion of the solar spectrum– The shortest-wavelength, highest-energy photons are captured in the

top layer while most of the rest pass through to the next layer– Subsequent layers have lower and lower band gaps, so they each pick

off the most energetic photons that they see, while passing the rest down to the next layer

• Very high efficiencies are possible using this approach– Lab examples of multi-junction cells have demonstrated performance

over 42%



• Concentrated photovoltaic (CPV) technology uses optics such as lenses to concentrate a large amount of sunlight onto a small area of solar photovoltaic materials to generate electricity

• Unlike traditional, more conventional flat panel systems, CPV systems are often much less expensive to produce, because the concentration allows for the production of a much smaller area of solar cells



• Today, the vast majority of PV modules (85% to 90% of the global annual market) are based on wafer-based crystalline silicon

• Crystalline silicon PV modules are expected to remain a dominant PV technology until at least 2020, with a forecasted market share of about 50% by that time


Characteristics–Thin-Film Photovoltaics

• Conventional crystalline silicon technologies require considerable amounts of expensive material with additional complexity and costs needed to wire individual cells together

• Competing technologies are based on depositing extremely thin films of photovoltaic materials onto glass or metal substrates

• Thin-film devices use relatively little material, do not require the complexity of cell interconnections, and are particularly well suited to mass-production techniques



• Their thinness allows photons that aren’t absorbed to pass completely through the photovoltaic material, which offers two special opportunities– Their semitransparency means that they can be deposited onto

windows, making building glass a provider of both light and electricity– They also lend themselves to multiple-junction, tandem cells in which

photons of different wavelengths are absorbed in different layers of the device



• Currently, thin-film cells are not as efficient as crystalline silicon —especially when they are not used in tandem devices

• While the likelihood of significant reductions in module costs are modest for conventional crystalline silicon, many opportunities remain to increase efficiency and dramatically reduce costs using thin-film technologies



• Thin films currently account for 10% to 15% of global PV module sales

• They are subdivided into three main families– Amorphous (a-Si) and micromorph silicon (a-Si/μc-Si)– Cadmium-Telluride (CdTe)– Copper-Indium-Diselenide (CIS) and Copper-Indium-Gallium-

Diselenide (CIGS)

power generation from renewable energy sources

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