推荐回答(2个)
晶体管工作的条件
1.集电极电阻Rc:
在共发射极电压放大器中,为了取出晶体管输出端的被放大信号电压Use(动态信号),需要在集电极串接一只电阻Rc。这样一来,当集电极电流Ic通过时,在Re上产生一电压降IcRc,输出电压由晶体管c-e之间取出,即Usc=Uce=Ec-IcRc,所以Use也和IcRc —样随输入电压Ui的发生而相应地变化。
2.集电极电源Ec(或Vcc):
Ec保证晶体管的集电结处于反向偏置,使管子工作在放大状态,使弱信号变为强信号。能量的来源是靠Ec的维持,而不是晶体管自身。
3.基极电源Eb:
为了使晶体管产生电流放大作用,除了保证集电结处于反向偏置外,还须使发射结处于正向偏置,Eb的作用就是向发射结提供正向偏置电压,并配合适当的基级电阻Rb,以建立起一定的静态基极电流Ib。当Vbe很小时,Ib=O,只有当Vbe超过某一值时(硅管约0.5V,锗管约0.2V,称为门槛电压),管子开始导通,出现Ib。随后,Ib将随Vbe增大而增大,但是,Vbe和Ib的关系不是线性关系:当Vbe大于0.7V后,Vbe再增加一点点,Ib就会增加很多。晶体管充分导通的Vbe近似等于一常数(硅管约0.5V,锗管约 0.5V)。
4.基极偏流电阻Rb:
在电源Eb的大小已经确定的条件下,改变Rb的阻值就可以改变晶体管的静态电流Ib,从而也改变了集电极静态电流Ic和管压降Vce,使放大器建立起合适的直流工作状态。
二、晶体管工作状态的判断
晶体三极管工作在放大区时,其发射结(b、e极之间)为正偏,集电结(b、c极之间)为反偏。对于小功率的NPN型硅,呈现为Vbe≈0.7V,Vbc<0V(具体数值视电源电压Ec与有关元件的数值而定):对于NPN型锗管,Vbe≈0.2V,Vbc<0V;对于PNP型的晶体三极管,上述电压值的符号相反,即小功率PNP型硅管Vbe≈-0.7V,Vbc>0V,对于小功率 PNP型锗管,Vbe≈-0.2V,Vbc>0V。如果我们在检测电路中发现晶体三极管极间电压为上述数值,即可判断该三极管工作在放大区,由该三极管组成的这部分电路为放大电路。
另外,在由晶体管组成的振荡电路中,其三极管也是工作在放大区,但由于三极管的输出经选频谐振回路并同相反馈到其b、C极之间,使电路起振,那么b、e极之间的电压Ube,对于硅管来说就小于0.7V 了(一般为0.2V左右)。如果我们检测出Vbe<0.7V,且用导线短接选频谐振电路中的电感使电路停振时Vbe0.7V,则可判断该电路为振荡电路。
2.工作在截止区的判断:
三极管工作在截止区时,发射结与集电结均为反偏,而在实际的电路中,发射结也可以是零偏置。这样对于小功率NPN型三极管,呈现为Vbe≤0,Vbc<0V(具体数值主要决定于电源电压Ec);对于小功率NPN型三极管,呈现为Vbe≥OV,Vbc≥0V,此时的 Vce≈Ec,如果我们检测出电路中晶体三极管间电压为上述情况,则可判断该三极管工作在截止区。
3.工作在饱和区的判断:
三极管工作在饱和区时,其发射结与集电结均为正偏。对于小功率NPN型硅管,呈现为Vbe多0.7V(略大于工作在放大区时的数值),Vbc>0V (不大于Vbe的值);对于小功率NPN型锗管,类似地有Vbe≥0.2V(略大于工作在放大区时的值),Vbc>OV (不大于Vbe的值)。对于PNP型的晶体管,上述电压值的符号相反,即小功率的PNP型硅管,Vbe≥-0.7V,Vb<0V(不小于Vbe的值;小功率PNP型锗管,Vbe≤-2V,Vbc<0V(不小于Vbe的值)。一般情况下,此时的Vce≈0.3V(硅管)或 Vce≈0.1V(锗管),如果我们检测出电路中的晶体三极管极间电压符合上述情况,则可判断该三极管工作在饱和区。
需要指出一点的是:在有些电子电路中,如开关电路、数字电路等,三极管工作在截止区与饱和区之间相互转换,如附图所示。当A点为0V时,EB通过R1、R2分压使基极处于负电压,发射结反偏;同时集电结也是反偏的,那么三极管T截止;当A点输入为6V时,R1、R2分压使三极管发射结正偏,产生足够大的基极电流使三极管饱和导通,输出端L约为0.3V,此时集电结也为正偏。我们检测电路是否正常时,可以分别使A端输人0V与6V的电压,并分别测量两种情况下的三极管极间电压,看是否符合上述截止与饱和的情况,从而就可以判断该电路工作是否正常。
A和B中的三极管工作在饱和导通状态,C为截止状态。
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