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光伏基础原理
光的特性

各个区间波长的分布见下图,可见光,又可分为紫光(390-450)蓝光(450--490nm),绿光(490-570nm),红光(620-780nm).


光子的能量跟波长成反比,h为普朗克常数,C为光速,都为常量。下面公式1是基于把光当成电磁波来看。


大气质量:太阳光穿过大气层的路径,AM1.5为1.5倍垂直入射穿过大气层的距离,也就是θ=48度。AM0条件下,太阳能垂直入射到地球最大的光强为1366W/㎡。


二极管以及光伏发电原理


价带:共价键束缚载流子自由移动,不能参与导电。

导带:电子可以自由移动。

禁带:介于价带和导带之间。

禁带宽度:一个电子从价带运动到能参与导电的自由状态所需要吸收的最低能量值,硅材料禁带宽度1.12ev,对应110nm波段。

载流子:电子和空穴都能参与导电并都称为。

电子移向导带的运动导致了电子本身的移动。

电子移动过程还产生了空穴在价带中的移动。

本征载流子:没有注入能改变载流子浓度的杂质的半导体材料叫做本征材料,浓度跟材料本身以及温度有关系,且电子空穴数目相等。

N型半导体:掺杂后多子带负电,例如掺磷。

P型半导体:掺杂后多子带正电,例如掺硼,掺镓。

晶体硅的原子结构,最外层电子由四对共用电子对组成。

太阳能电池片最重要的参数

禁带宽度:电子从从价带到导带跃迁需要的最小能量;

导带自由载流子数量;

光照条件下产生和复合的自由载流子数量。


平衡载流子浓度

本征载流子浓度由材料以及温度所决定,温度越高,载流子浓度越高。

平衡载流子浓度:在没有偏置情况下,导带和价带的载流子数量称为平衡载流子浓度。多子数量等于本征自由载流子数量加上参杂的自由载流子数量,一般情况下,参杂的载流子数量大于本征载流子数量的几个数量级,也就是约等于参杂浓度。

Ni: 本征载流子数量, n0p0分别代表电子和空穴载流子数量。


光的吸收:

1.Eph

2.Eph=Eg 光子的能量刚刚好足够激发出一个电子-空穴对,能量被完全吸收。

3.Eph>Eg 光子能量大于禁带宽度并被强烈吸收。

吸收深度:


400nm以下紫外波段,在硅片厚度0.1um处被完全吸收。

400—800nm可见光波段,在硅片厚度10um处被完全吸收。

800-1000nm近红外波段,在硅片厚度100um处被完全吸收。

1100nm近红外处波段,能穿透硅片厚度超过1000um。

载流子的产生率:


不同波段光在电池片厚度的产生率: 蓝光在0.1um处被完全吸收;红光在50um处几乎被完全吸收; 近红外光在100um处还能激发表面90%的载流子,吸收很慢。

全波段总的生成率:在电池片表面,因短波段基本集中在表面,故激发的载流子数量最多,然后随着硅片厚度增加光的吸收逐步递减,导致载流子数量逐步减少。


三种复合:

• 辐射复合:电子空穴的复合,激发出近似禁带宽度的1100nm的光,也是EL/PL发光的原理。

• 俄歇复合:涉及两个电子,一个空穴。电子跟空穴复合,传递能量给另外一个电子做运动,没有光激发。主要体现在重掺杂或者加热高温材料。

• 肖克莱-雷德-霍尔复合:也叫复合中心的复合或者缺陷复合,直接吸收电子或者空穴,辐射出能量非常弱的光。

扩散长度/少子寿命

少子扩散长度:在复合之前一个载流子从产生处开始运动的平均路程。

少子寿命:在复合之前一个载流子从产生到复合的平均时间。

表面复合

半导体表面的缺陷是由于晶格排列在表面处的中断照成的,即在表面处产生挂键,所以电池表面是一个复合率非常高的区域。减少挂键的数目可以通过在半导体表面处生长一层薄膜以连接这些挂键,这种方法也叫做表面钝化。


载流子的运动:在大多数情况下,电子是电场相反的方向运动。

扩散:

在两个不同浓度的区域之间将会出现载流子梯度。载流子将从高浓度区域流向低浓度区域。

漂移:

由外加电场所引起的载流子运动叫“漂移运动”。

PN结:

n型半导体区域的电子浓度很高,而p型区域的空穴浓度很高,所以电子从n型区扩散到p型区,同理,空穴从P型区扩散到n型区。当电子和空穴运动到pn结的另一边时,也在杂质原子区域留下了与之相反的电荷,这种电荷被固定在晶格当中不能移动。在n型区,被留下的便是带正电的原子核,相反,在p型区,留下的是带负电的原子核。于是,一个从n型区的正离子区域指向p型区的负离子区域的电场E就建立起来了。这个电场区域叫做“耗尽区”,因为此电场能迅速把自由载流子移走,因此,这个区域的自由载流子是被耗尽的。

正向偏压下的二极管(核心知识点)

正向偏压(也叫正向偏置)指的是在器件两边施加电压,以使得pn结的内建电场减小。电场的减小将破坏pn结的平衡,即减小了对载流子从pn结的一边到另一边的扩散运动的阻碍,增大扩散电流。

从pn结的一端到另一端的扩散运动的增加导致了少数载流子(少子)往耗散区边缘的注入。这些少数载流子由于扩散而渐渐远离pn结并最终与多数载流子(多子)复合。在正向偏置下的扩散电流也是复合电流。复合的速度越高,通过pn结的扩散电流就越大。“暗饱和电流”(I0)是区别两种不同二极管的非常重要的参数。I0是衡量一个器件复合特点的标准,二极管的复合速率越大,I0也越大。

反向偏压

反向偏置电压是指在器件两端加电场,以使pn结增大。在pn结中的内建电场越大,载流子能从pn结一段扩散至另一端的概率就越小,即扩散电流就越小。

理想二极管方程:


I为通过二极管的净电流;

I0为暗饱和电流(在没有光照情况下输出的电流),I0随着T的升高而增大。在温度为300k时,KT/q=25.85mV。

V是施加在二极管两端的电压;

q和k分别代表电荷的绝对值和玻耳兹曼常数;

T则表示绝对温度(K)。

收集概率:(可结合载流子产生率对比)

“收集概率”描述了光照射到电池的某个区域产生的载流子被pn结收集并参与到电流流动的概率,它的大小取决于光生载流子需要运动的距离和电池的表面特性。在耗散区的所有光生载流子的收集概率都是相同的,因为在这个区域的电子空穴对会被电场迅速地分开。当载流子在与电场的距离大于扩散长度的区域产生时,那么它的收集概率是相当低的。相似的,如果载流子是在靠近电池表面这样的高复合区的区域产生,那么它将会被复合。下面的图描述了表面钝化和扩散长度对收集概率的影响。


量子效率:

所谓“量子效率”,即太阳能电池所收集的载流子的数量与入射光子的数量的比例。量子效率即可以与波长相对应又可以与光子能量相对应。如果某个特定波长的所有光子都被吸收,并且其所产生的少数载流子都能被收集,则这个特定波长的所有光子的量子效率都是相同的。而能量低于禁带宽度的光子的量子效率为零。下图将描述理想太阳能电池的量子效率曲线。


光伏 效应(核心知识点)

电池开路的情况下,pn结的正向偏压处在新的一点,此时,光生电流大小等于扩散电流大小,且方向相反,即总的电流为零。

电池短路的情况下,将不会出现电荷的聚集,因为载流子都参与了光生电流的流动,短路电流等于光生电流(同样等于开压状态下内部扩散电流)。

工作状态下,其电流等于光生电流减去太阳能电池内部扩散电流。

短路电流等于光生电流,且等于内建电场作用下的漂移电流,也是电池片能提供的最大的电流。

开路电压下,光生载流子导致正向偏压从而消弱内建电场,增加扩散电流,光生电流等于扩散电流且方向相反。


工作状态下,流出电池的电流大小就等于光生电流与扩散电流的差。

内建电场代表着对前置扩散电流的障碍,所以电场减小的同时也增大扩散电流。


复合机制对开路电压的影响(核心难点)

PN结边缘的少子数量,越少,耗尽区越宽,则需要增加掺杂浓度。

扩散长度。 掺杂浓度越高,扩散长度越低(扩散电流越大),则需要降低掺杂浓度。

二者需要达到平衡。


ECV曲线解读


体电阻(硅片电阻率):电阻是纵向的,电子垂直移动然后到达表面。故移动的距离为电池片厚度,横截面为电池片面积,即R=ρW/A

方块电阻:电阻是横向的,不是垂直纵向,即横截面积等于距离L乘以厚度T,所以电阻R=ρ L / (L*T),只要L是正方形边长,则方块电阻只跟电阻率以及N区厚度有关系。

方块电阻的测量非常容易,通过四探针测试方法,外面两根探针提供电流,中间两根探针处产生压降,N区和P区之间的PN结做为结缘体。注意测试必须在暗室。


太能能电池等效电路图(核心知识点)


引起串联电阻的因素有三种:

第一,穿过电池发射区和基区的电流流动;

第二,金属电极与硅之间的接触电阻;

第三便是顶部和背部的金属电阻。串联电阻对电池的主要影响是减小填充因子,此外,当阻值过大时还会减小短路电流。串联电阻并不会影响到电池的开路电压,因为此时电池的总电流为零,所以串联电阻也为零。

并联电阻RSH造成的显著的功率损失通常是由于制造缺陷引起的。

温度效应

本征载流子随着温度高,浓度高,导致暗电流增加,复合增加,从而导致开路电压下降。

Characteristics of light



See the following figure for the wavelength distribution in each section. Visible light can be divided into purple light (390-450), blue light (450--490nm), green light (490-570nm) and red light (620-780nm)





The energy of a photon is inversely proportional to the wavelength. H is the Planck constant and C is the speed of light, both of which are constants. The following formula 1 is based on treating light as an electromagnetic wave.





Atmospheric quality: the path of sunlight through the atmosphere. AM1.5 is 1.5 times the distance of vertical incidence through the atmosphere, i.e θ= 48 degrees. Under the condition of AM0, the maximum intensity of solar energy vertically incident on the earth is 1366w/ ㎡.





Diode and photovoltaic power generation principle



Valence band: covalent bonds bind carriers to move freely and cannot participate in conduction.



Conduction band: electrons can move freely.



Forbidden band: between valence band and conduction band.



Band gap width: the lowest energy value that an electron needs to absorb from the valence band to the free state that can participate in conduction. The band gap width of silicon material is 1.12eV, corresponding to the 110Nm band.



Carrier: both electrons and holes can participate in conducting electricity and are called.



The movement of the electron towards the conduction band results in the movement of the electron itself.



The electron movement process also produces the movement of holes in the valence band.



Intrinsic carriers: semiconductor materials without impurities that can change the carrier concentration are called intrinsic materials. The concentration is related to the material itself and temperature, and the number of electron holes is equal.



N-type semiconductor: after doping, many subbands are negatively charged, such as phosphorus doping.



P-type semiconductor: multi subband positive charge after doping, such as boron and gallium.



The atomic structure of crystalline silicon in which the outermost electrons are composed of four common electron pairs.



The most important parameters of solar cells



Band gap width: the minimum energy required for electron transition from valence band to conduction band;



Number of free carriers in conduction band;



The number of free carriers produced and combined under illumination.





Equilibrium carrier concentration



The intrinsic carrier concentration is determined by the material and temperature. The higher the temperature, the higher the carrier concentration.



Equilibrium carrier concentration: the number of carriers in the conduction and valence bands without bias is called the equilibrium carrier concentration. The number of multi carriers is equal to the number of intrinsic free carriers plus the number of heterozygous free carriers. Generally, the number of heterozygous carriers is greater than several orders of magnitude of the number of intrinsic carriers, that is, it is about equal to the heterozygous concentration.



Ni: number of intrinsic carriers, n0p0 represents the number of electron and hole carriers respectively.





Light absorption:



1. Eph


2. The energy of eph=eg photon is just enough to excite an electron hole pair, and the energy is completely absorbed.



3. The photon energy of eph>eg is larger than the band gap and is strongly absorbed.



Absorption depth:





The ultraviolet band below 400nm is completely absorbed at the thickness of 0.1um.



In the visible light band of 400-800nm, it is completely absorbed at the silicon wafer thickness of 10um.



800-1000nm near-infrared band, fully absorbed at 100um silicon wafer thickness.



At 1100nm near-infrared wave band, it can penetrate the thickness of silicon wafer more than 1000um.



Carrier generation rate:





The generation rate of light at different wavelengths in the thickness of the cell: blue light is completely absorbed at 0.1um; Red light is almost completely absorbed at 50um; Near infrared light can also excite 90% of the surface carriers at 100um, and the absorption is very slow.



Total generation rate of full band: on the surface of the cell, the number of excited carriers is the largest because the short band is basically concentrated on the surface, and then the absorption of light decreases gradually with the increase of the thickness of the silicon wafer, resulting in the gradual reduction of the number of carriers.





Three combinations:



• radiation recombination: the recombination of electron holes excites 1100nm light with approximate band gap width, which is also the principle of el/pl luminescence.



• Auger recombination: two electrons and one hole are involved. Electrons combine with holes to transfer energy to another electron for movement. There is no light excitation. Mainly reflected in heavily doped or heated high-temperature materials.



• Shockley Reid hall recombination: also known as recombination of recombination centers or defect recombination, it directly absorbs electrons or holes and radiates very weak light.



Diffusion length / minority carrier lifetime



Minority carrier diffusion length: the average path of a carrier from the point of origin before recombination.



Minority carrier lifetime: the average time from generation to recombination of a carrier before recombination.



Surface compounding



The defects on the semiconductor surface are caused by the interruption of lattice arrangement at the surface, that is, the hanging bond is generated at the surface, so the battery surface is a region with very high recombination rate. To reduce the number of hanging keys, a thin film can be grown on the semiconductor surface to connect these hanging keys. This method is also called surface passivation.





Carrier motion: in most cases, electrons move in the opposite direction of the electric field.



Diffusion:



There will be a carrier gradient between two regions with different concentrations. The carrier will flow from the high concentration region to the low concentration region.



Drift:



The carrier motion caused by the applied electric field is called "drift motion".



PN junction:



The electron concentration in the n-type semiconductor region is very high, while the hole concentration in the p-type region is very high, so electrons diffuse from the n-type region to the p-type region. Similarly, holes diffuse from the p-type region to the n-type region. When electrons and holes move to the other side of the PN junction, they also leave opposite charges in the impurity atom region, which are fixed in the lattice and cannot move. In the n-type region, the positively charged nuclei are left behind. On the contrary, in the p-type region, the negatively charged nuclei are left behind. Thus, an electric field E from the positive ion region of the n-type region to the negative ion region of the p-type region is established. This electric field region is called "depletion region", because this electric field can quickly remove the free carriers, so the free carriers in this region are exhausted.



Diode under forward bias voltage (core knowledge points)



Forward bias (also known as forward bias) refers to the application of voltage on both sides of the device to reduce the built-in electric field of the PN junction. The decrease of the electric field will destroy the balance of the PN junction, that is, it will reduce the obstacle to the diffusion movement of carriers from one side of the PN junction to the other, and increase the diffusion current.



The increase of the diffusion motion from one end of the PN junction to the other leads to the injection of minority carriers into the edge of the dissipation region. These minority carriers gradually move away from the PN junction due to diffusion and eventually compound with the majority carriers (multipons). The diffusion current under forward bias is also a composite current. The higher the recombination speed, the greater the diffusion current through the PN junction. "Dark saturation current" (I0) is a very important parameter to distinguish two different diodes. I0 is a standard to measure the composite characteristics of a device. The greater the composite rate of the diode, the greater the I0.



Reverse bias



The reverse bias voltage means that an electric field is applied at both ends of the device to increase the PN junction. The larger the built-in electric field in the PN junction, the smaller the probability of carrier diffusion from one section of the PN junction to the other, that is, the smaller the diffusion current.



Ideal diode equation:





I is the net current through the diode;



I0 is the dark saturation current (the current output without illumination), and I0 increases with the increase of T. When the temperature is 300K, kt/q=25.85mv.



V is the voltage applied to both ends of the diode;



Q and K represent the absolute value of charge and Boltzmann constant respectively;



T is the absolute temperature (k).



Collection probability: (can be compared in combination with carrier generation rate)



"Collection probability" describes the probability that the carriers generated by the light irradiating a certain area of the battery will be collected by the PN junction and participate in the current flow. Its size depends on the distance that the photogenerated carriers need to move and the surface characteristics of the battery. The collection probability of all photogenerated carriers in the dissipative region is the same, because the electron hole pairs in this region will be rapidly separated by the electric field. When the carrier is generated in the region where the distance from the electric field is greater than the diffusion length, its collection probability is quite low. Similarly, if the carrier is generated in a region close to a high recombination region such as the battery surface, it will be recombined. The following figure describes the effect of surface passivation and diffusion length on the collection probability.





Quantum efficiency:



The so-called "quantum efficiency" refers to the ratio of the number of carriers collected by the solar cell to the number of incident photons. Quantum efficiency can correspond to both wavelength and photon energy. If all photons at a particular wavelength are absorbed and the minority carriers produced by them can be collected, the quantum efficiency of all photons at that particular wavelength is the same. The quantum efficiency of photons whose energy is lower than the band gap is zero. The following figure will describe the quantum efficiency curve of an ideal solar cell.





Photovoltaic effect (core knowledge points)



When the battery is open, the forward bias voltage of PN junction is at a new point. At this time, the magnitude of photogenerated current is equal to the magnitude of diffusion current, and the direction is opposite, that is, the total current is zero.



When the battery is short circuited, there will be no charge accumulation, because the carriers participate in the flow of the photo generated current, and the short-circuit current is equal to the photo generated current (also equal to the internal diffusion current under the open voltage state).



In the working state, the current is equal to the photogenerated current minus the internal diffusion current of the solar cell.



The short-circuit current is equal to the photo generated current and the drift current under the action of the built-in electric field, which is also the maximum current that the battery can provide.



Under the open circuit voltage, the photogenerated carriers cause a positive bias voltage, which weakens the built-in electric field and increases the diffusion current. The photogenerated current is equal to the diffusion current and the direction is opposite.





In the working state, the current flowing out of the battery is equal to the difference between the photogenerated current and the diffusion current.



The built-in electric field represents an obstacle to the pre diffusion current, so the reduction of the electric field also increases the diffusion current.





Influence of composite mechanism on open circuit voltage (core difficulty)



The smaller the number of electrons at the edge of the PN junction, the wider the depletion region is, and the doping concentration needs to be increased.



Diffusion length. The higher the doping concentration, the lower the diffusion length (the greater the diffusion current), so it is necessary to reduce the doping concentration.



The two need to be balanced.





Interpretation of ECV curve





Bulk resistance (silicon wafer resistivity): the resistance is vertical, and the electrons move vertically and then reach the surface. Therefore, the moving distance is the thickness of the battery, and the cross section is the area of the battery, i.e. R= ρ W/A



Block resistance: the resistance is horizontal, not vertical, that is, the cross-sectional area is equal to the distance L multiplied by the thickness T, so the resistance R= ρ L / (l*t). As long as l is the square side length, the block resistance is only related to the resistivity and the thickness of N zone.



It is very easy to measure the block resistance. Through the four probe test method, the two probes outside provide current, the two probes in the middle generate voltage drop, and the PN junction between N and P regions is used as the bonding body. Note that the test must be in a dark room.





Equivalent circuit diagram of solar cell (core knowledge points)





There are three factors causing series resistance:



First, the current flow through the emission region and the base region of the battery;



Second, contact resistance between metal electrode and silicon;



The third is the metal resistance at the top and back. The main effect of series resistance on the battery is to reduce the filling factor. In addition, when the resistance is too large, it will also reduce the short-circuit current. The series resistance does not affect the open circuit voltage of the battery, because the total current of the battery is zero, so the series resistance is zero.



The significant power loss caused by parallel resistance RSH is usually caused by manufacturing defects.



temperature effect



With the increase of temperature and concentration of intrinsic carriers, the dark current and recombination increase, resulting in the decrease of open circuit voltage.

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