Комментарии:
Can the resistor 'Re' be equal to zero in this circuit?
ОтветитьThank you for this explanation, how do we define Beta here?
ОтветитьAs I was hovering looking for a perfect solution .. I just saw your the cover photo and I knew my problem is solved.... And guess what am just 4mins I to the video and I have understood everything... Thanks man .... 🔥🤗
ОтветитьIf i use exact method even if bre>>10r2 then is it right
ОтветитьThank you
ОтветитьJust awesome explanation sir, thank you so much for that video. I have one doubt about beta, how can we take the beta value as constant because in any transistor data sheet the beta value have a range. For example BC548 has a beta range from 110 to 500. So which value should i take while using this transistor for amplification (for a perfect active region). Please explain sir, if possible.
Ответитьbless you sir. Great video
ОтветитьThanks for a very clear and helpful explanation. I now have a much better understanding of how to set up a bias circuit for a BJT, and why a certain amount of "slop" necessarily occurs when calculating actual voltage, current, and resistance values.
ОтветитьHow are those resistors in parallel? Having a little trouble getting my head around that
ОтветитьWhat is the use of RE in the circuit?how it provide stability?
ОтветитьThis video helped me understand the biasing of BJT. Thanks a lot sir!
ОтветитьFinally someone that made me understand this theory. Thanks a lot.
ОтветитьThanks for the good video. How would you solve the question if there is also a resistor between base of transistor and opposite node? Thanks
ОтветитьThe "short-cut" method calculates the quiescent collector current and dc bias points of a transistor that has infinite β. The stability of the dc bias against changes in β depends purely on the relative size of the emitter resistor Re. That resistor provides negative feedback that stabilises the operating points as well as reducing the distortion of the stage. It comes at the cost of lowering the voltage gain of the stage, which is 3 in this case. It also "absorbs" around 2.5V of the potential output swing.
You can improve the performance of a common emitter by removing some of the negative feedback from the emitter resistance by lowering it, while providing a feedback path from the collector to the base. In other words, derive your base voltage bias (the positive end of R1) from the collector rather than the positive supply rail. Since the emitter resistor only needs to be more than 10 times the dynamic emitter resistance of the transistor (25mV/Ic) to provide reasonable linearity, the emitter can be usefully biased to as little as 250mV above ground, putting the base at about 900mV above ground. If you assume that the collector bias point is around half the supply voltage, you can quickly calculate the ratio of R1 to R2. Knowing the β will allow you to make R1 || R2 less than 1/10 of β.Re for any value of Re. That shows you that the input impedance of the stage is inversely proportional to the collector current, and (all else being equal) you should choose Ic to obtain whatever Zin is required. Somewhere between 1mA and 2mA with a β > 250 or so will result in an input impedance around 5K to 10K.
That solution will allow reasonable gains of around 20 to 30 with good stability and linearity, while maintaining independence of transistor parameters. I recommend it to you.
Thanks so much . Your video has clarified all my doubt. Thanks once more
ОтветитьGreat BUT why you say voltage divider R1 and R2 and immediately căLculate Rth as parralel ?/
ОтветитьThe best video i've seen so far, thank you.
ОтветитьExcellent explanation. Infinitely more helpful than a university professor
ОтветитьWhere did you get Re from?
ОтветитьCould you please explain how you calculate R(th) as being 8.33 KΩ ?
ОтветитьVery useful methode
Ответитьthx a lot bro
ОтветитьI find I'm more of a spice warrior then a scientific calculator nerd 😁
ОтветитьWhat is the equation to solve for ro? Anyone
ОтветитьGreat explanation sir! Now I understand what's going on there
ОтветитьSublime!
ОтветитьThank you for such a crystal clear explanation of a VDB-BJT.
ОтветитьThanks for making this very CLEAR plain English video. I can definitely understand your Canadian English.
ОтветитьOnly complaint is there is not a download link for a pdf document of this lecture. The information is so good there should be a link.
ОтветитьSir how to get answer uA please tell me i don't uderstands
ОтветитьThank you so much
ОтветитьThanks for the video. I've gained a headache.
Ответитьhow to solve for IC if the beta is unknown? plss help
ОтветитьVery clear explanation!
ОтветитьExcellent presentation, and delivery of material content. Thoroughly explained in detailed information describing the devices characteristics and biasing approaches.
ОтветитьThanks a lot
From iraq 🇮🇶
Wow!! Thanks..
ОтветитьMore than 3 years after graduating, I am now understanding this. Thank you so much.
Ответитьhow do you get (beta+1) ? great video though! my professor cant explain shit!
ОтветитьAlso is (Vth) the same as (Vb) the voltage looking into the base of the transistor?
ОтветитьSo (Rth) is the same as the resistance at the base of the transistor so (Ib) times (Rth) will give me the voltage at the base of the transistor and therefore will give me the voltage at the resistor going to the ground (Rb2) does that sound right?
ОтветитьI think you are one of the best teachers ever! Please make more videos related to EE courses. Thanks. GOD BLESS YOU!
ОтветитьWhats the value of i1 and i2?
ОтветитьWhat if Current Gain is not given?
Ответить