- #36
The Electrician
Gold Member
- 1,402
- 210
DODGEVIPER13 said:Ok so I am going to put it on here and I am going to upload it later tonight. Ib1=V1-V2/Rb+rpi1, Ib2=V5-V4/Rb+rpi2, Ie1 = V2-V3/ro1, Ie1+Ie2=Ic3, Ie2 = V4-V3/ro2, gm6Vbe6 = V7-V6/ro6
You need to be very careful with your equations. When you type them in text form as you have done here, you need to use parentheses where there could be ambiguity. For example, you have typed:
Ib1=V1-V2/Rb+rpi1, which is the same as:
[tex]Ib1 =V1 - \frac{V2}{Rb}+ rpi1[/tex]
which is not what you really want. What you really want is:
[tex]Ib1 =\frac{V1-V2}{Rb+ rpi1}[/tex]
In plain text form you would need to use some parentheses to get a correct representation, like this:
Ib1=(V1-V2)/(Rb+rpi1)
Don't use this for equation 1; I'm going to change the nodes below.
You can use LaTeX on this forum to get the pretty expressions as I've done above. Here's an FAQ that explains how to do it:
https://www.physicsforums.com/showpost.php?p=3977517&postcount=3
DODGEVIPER13 said:Yes I guess so man I don't think my buddies really get this problem either they are just pulling formulas from the book I think I would be better off letting this part go and just going with what Jony and you provided. That being said how would I start on part d ultimatley that was where I was trying to get the total gain?
Parts b and d can both be answered by using the model you have so far. You only need to set up the 7 nodal equations and solve them. Sounds easy, right?
Please use lower case v for the node designators; for small signal analysis, lower case letters are conventionally used for variables.
We will get easier results if two of the nodes are changed slightly. Let's use these node designators:
v1. Top of rpi1
v2. Top of ro1
v3. Top of 80k resistor
v4. Top of ro2
v5. Top of rpi2
v6. Emitter of Q6
v7. Collector of Q6 (your output node)
This will change your equation 1. Here's how we derive it.
The voltage at each node is given by the relevant designator; at node 2, the voltage is v2. Currents leaving a node are considered positive and those entering a node are negative.
There are two paths for current at node 1: the input current in RB1 and the current in rpi1.
1. The current in RB1 is just the voltage across RB1, which is (v1-V1), divided by the resistance RB1: (v1-V1)/RB1. (Here's why you need to use lower case v for the node voltages. v1 is the voltage at the top of rpi1 and V1 is the input voltage). This current is leaving node 1 because we chose to define the voltage as (v1-V1), not (V1-v1); see the explanation at the end of this post for more info about this.
2. The current in rpi1 is the voltage across rpi1, which is (v1-v3), divided by the value of rpi1: (v1-v3)/rpi1
Equation 1 simply sets the sum of these two currents equal to zero:
Eq1: (v1-V1)/RB1 + (v1-v3)/rpi1 = 0
Let's derive equation 2.
We have 3 currents leaving node 2 (If any are actually entering, the algebra will give a negative sign for them; that is taken care of by the order of the subtraction of voltages in the numerator expression for each current).
1. The current in the collector resistor of Q1 (which you should have labeled Rc1, not just Rc) is equal to the voltage across it, which is (v2-0), (remember that V+ is signal ground) divided by the resistance itself: (v2-0)/Rc1 which is just v2/Rc1. That is a current leaving node 2.
2. The current in the resistor ro1 is the voltage across ro1, which is (v2-v3), divided by the resistance of ro1: (v2-v3)/ro1
3. The current supplied by the gm1 source; that current is gm1*vbe1. But, notice that Vbe1 is just (v1-v3), so this current is given by gm1*(v1-v3)
Equation 2 is just the sum of these 3 currents set equal to zero:
Eq2. v2/Rc1 + (v2-v3)/ro1 + gm1*(v1-v3) = 0
You should be able to see how this works. You identify all the paths for current to leave or enter a node; those paths are often just some impedance, although they are sometimes sources such as the gm sources. If the path is an impedance, write an expression for the numerator of a fraction, that expression being the voltage across the impedance in a form like this (va-vb). The va is the voltage at the node being worked on, and vb is the voltage at the other end of the impedance; by ordering the voltages like this: (va-vb) instead of (vb-va) the current is calculated as if leaving the node and is therefore a positive current. The denominator is just the impedance under consideration.
If the path is a controlled source such as your gm sources, write an expression for the current supplied by the source, involving the voltage(s) at some other nodes, where those nodes are the ones whose voltages control the source.
Each current is in the form of a fraction (except possibly for the currents from controlled sources) and all the currents are summed to zero to give you an equation.
Derive the next 5 equations and post them, each on a separate line, not all on one line separated by commas!
You will need to solve 7 simultaneous equations; how will you do that? Do you have access to Matlab, MathCad, or some similar software?
Last edited: