diff --git a/subs/3NIegrCmA5k.srt.sjson b/subs/3NIegrCmA5k.srt.sjson
new file mode 100644
index 0000000000..bc505bb0d1
--- /dev/null
+++ b/subs/3NIegrCmA5k.srt.sjson
@@ -0,0 +1,5 @@
+{
+  "start": [], 
+  "end": [], 
+  "text": []
+}
\ No newline at end of file
diff --git a/subs/EG-fRTJln_E.srt.sjson b/subs/EG-fRTJln_E.srt.sjson
new file mode 100644
index 0000000000..bc505bb0d1
--- /dev/null
+++ b/subs/EG-fRTJln_E.srt.sjson
@@ -0,0 +1,5 @@
+{
+  "start": [], 
+  "end": [], 
+  "text": []
+}
\ No newline at end of file
diff --git a/subs/G_2F9wivspM.srt.sjson b/subs/G_2F9wivspM.srt.sjson
new file mode 100644
index 0000000000..34fc42d535
--- /dev/null
+++ b/subs/G_2F9wivspM.srt.sjson
@@ -0,0 +1,191 @@
+{
+  "start": [
+    0, 
+    1800, 
+    2440, 
+    7270, 
+    11690, 
+    13030, 
+    17060, 
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+  ], 
+  "text": [
+    "SPEAKER 1: So I want to show you a simple circuit that", 
+    "looks like this.", 
+    "And let's go ahead and measure some voltages and currents.", 
+    "In terms of terminology, remember", 
+    "this is called a loop.", 
+    "So if I start from the point C, and I travel through the", 
+    "voltage source, come to the node A, down through R1 and", 
+    "all the way down through R2 back to C, that's a loop.", 
+    "Similarly, this point A is a node where the register R1,", 
+    "the voltage source V0 and R4 are connected.", 
+    "Just make sure your terminology is correct.", 
+    "So what I'll do is let me make some quick measurements for", 
+    "you, and show you that these KVL and KCL are indeed true.", 
+    "So the circuit's up there.", 
+    "So let me take some measurements.", 
+    "And why don't you write down what I measure on the board.", 
+    "Let me borrow another piece of chalk here.", 
+    "What I'll do is focus on this loop here and focus on this", 
+    "node and make some measurements.", 
+    "So you see the circuit up there.", 
+    "[INAUDIBLE]", 
+    "So I get three volts for the voltage from C to A. So why", 
+    "don't you write down three volts.", 
+    "OK, so the next one is minus 1.6.", 
+    "And so that will be I'm doing AB, VAB.", 
+    "And then let me do the last one.", 
+    "And it is minus 1.37.", 
+    "Within the bonds of experimental error, notice", 
+    "that if I add up these three voltages, they", 
+    "nicely sum up to zero.", 
+    "OK, next let me focus on this node here.", 
+    "And at this node, let me go ahead and", 
+    "measure some currents.", 
+    "What I'll do now is change to an AC voltage so that I can go", 
+    "ahead and measure the current without breaking my circuit.", 
+    "This time around, you'll get to see the measurements that", 
+    "I'm taking as well.", 
+    "What I have here is three wires that I have pulled out", 
+    "from D. And this is the node D. So three wires coming into", 
+    "the node D just to make it a little bit easier for me to", 
+    "measure stuff.", 
+    "So everybody keep your fingers crossed so I don't", 
+    "look like a fool here.", 
+    "Hope this works out.", 
+    "So it's about 10 millivolts peak to peak out there.", 
+    "Let's say that if the wave form rises on the left hand", 
+    "side, it's positive.", 
+    "So it's positive 10 millivolts.", 
+    "And another positive 10 millivolts.", 
+    "So that's 20 millivolts.", 
+    "And this time it's a negative, roughly 20, I", 
+    "guess, negative 20.", 
+    "So I'm getting, in terms of currents, I have a positive", 
+    "10, a positive 10 and a negative 20 that adds up to 0.", 
+    "But more interestingly, I can show you the same thing by", 
+    "holding this current measuring probe", 
+    "directly across that node.", 
+    "And notice that the net current that is entering into", 
+    "this node here is zero.", 
+    "So that should just show you that KCL does indeed hold in", 
+    "practice, and it is not just a figment of our imaginations."
+  ]
+}
\ No newline at end of file
diff --git a/subs/SMVp8kv_rlg.srt.sjson b/subs/SMVp8kv_rlg.srt.sjson
new file mode 100644
index 0000000000..b0d89f501d
--- /dev/null
+++ b/subs/SMVp8kv_rlg.srt.sjson
@@ -0,0 +1,152 @@
+{
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+  "text": [
+    "All right, this is the sub circuit.", 
+    "And what I've done here is I've have to turn the current", 
+    "source off.", 
+    "So notice that out here, I create an open circuit.", 
+    "And that is the result of my current source", 
+    "being turned off.", 
+    "And this is my usual ground note.", 
+    "And let me call this node voltage, with the voltage", 
+    "source acting alone, as ev. So ev is the partial response of", 
+    "the circuit to the voltage source acting alone.", 
+    "Now how do we go about solving for ev?", 
+    "Notice that we have a known pattern here.", 
+    "We have a voltage source connected to a pair of", 
+    "registers, R1 and R2.", 
+    "And ev is simply the voltage across R2.", 
+    "Now, this is a known pattern.", 
+    "So one thing you should keep in mind is that in circuits,", 
+    "and electronics, we use patterns a lot.", 
+    "Whenever we see a pattern, we can directly go and write down", 
+    "what the output response is going to look like.", 
+    "What I'm going to do is throughout this course, as we", 
+    "see more and more patterns, I'm going to alert you to", 
+    "these patterns.", 
+    "So right here is a voltage divider pattern.", 
+    "So for the voltage divider pattern, I can write down ev.", 
+    "I can write down ev as being some fraction of the source", 
+    "voltage v. And by the divider action, we simply R2 divide by", 
+    "R1 plus R2.", 
+    "So it is simply the voltage across R2, and that is given", 
+    "by R2 divided by R1 plus R2.", 
+    "And this is a known pattern that you'll find very helpful", 
+    "as you analyze circuits very quickly.", 
+    "Next, let's look at I acting alone.", 
+    "Before we do that, what do we have so far?", 
+    "Again, recall, this is the circuit", 
+    "we're trying to analyze.", 
+    "We are trying to get the voltage e.", 
+    "And so far, we have computed the partial voltage ev, due to", 
+    "the voltage source acting alone.", 
+    "As a next step-- again, this is still step one of the", 
+    "superposition method--", 
+    "let's look at the partial response of the circuit due to", 
+    "the current acting alone.", 
+    "To get the response for the current acting alone, I need", 
+    "to build a circuit in which the voltage", 
+    "source is turned off.", 
+    "I'll let you think for a couple of seconds as to what", 
+    "the circuit will look like before I draw it out for you."
+  ]
+}
\ No newline at end of file
diff --git a/subs/bmys8aKCjCo.srt.sjson b/subs/bmys8aKCjCo.srt.sjson
new file mode 100644
index 0000000000..af25915a53
--- /dev/null
+++ b/subs/bmys8aKCjCo.srt.sjson
@@ -0,0 +1,113 @@
+{
+  "start": [
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+  ], 
+  "text": [
+    "OK, let's go ahead.", 
+    "So to turn off this voltage source, all I have to do is", 
+    "replace it with a short circuit like so.", 
+    "So notice that I have replaced the voltage source with a", 
+    "short circuit, and I've left the current source in place.", 
+    "I have my ground node here.", 
+    "And notice that my goal is to find the partial voltage eI", 
+    "that is a result of the current source acting alone.", 
+    "So notice that I have a second pattern here.", 
+    "And in this case, this is a current divider pattern.", 
+    "Actually, this is a even simpler pattern.", 
+    "I simply have a current that is flowing", 
+    "into a pair of resistors.", 
+    "OK, so I have a current, I, that is flowing into a pair of", 
+    "resistors, R1 and R2.", 
+    "And so I can compute the voltage across the pair of", 
+    "resistors very straightforwardly.", 
+    "So eI is simply the resistance times the current.", 
+    "And the resistance of a paralel pair of resistors is", 
+    "simply R1 R2 divide by R1 plus R2 times the current I.", 
+    "OK, so now I have computed both ev and eI, the two", 
+    "partial voltages with each of the voltages acting alone.", 
+    "And now I am ready for step two of the", 
+    "superposition method.", 
+    "And the step two of the superposition method simply", 
+    "says that you sum the two partial voltages, ev and eI.", 
+    "So my resulting voltage e is simply the sum of the two", 
+    "partial voltages ev and eI.", 
+    "And I have those as R2 divide by R1 plus R2 times v. And I", 
+    "sum that to eI.", 
+    "And eI is R1 R2 divide by R1 plus R2 times I. And", 
+    "there you have it.", 
+    "Not surprisingly, this expression here is identical", 
+    "to the expression that you obtained by using the node", 
+    "method in the previous lecture."
+  ]
+}
\ No newline at end of file
diff --git a/subs/eLAyO33baQ8.srt.sjson b/subs/eLAyO33baQ8.srt.sjson
new file mode 100644
index 0000000000..4d2f5069ab
--- /dev/null
+++ b/subs/eLAyO33baQ8.srt.sjson
@@ -0,0 +1,326 @@
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+  "text": [
+    "SPEAKER 1: In this sequence, are going to look at a whole", 
+    "bunch of techniques for analyzing circuits.", 
+    "Think of these as your tool chest. So you are embarking on", 
+    "6.002 and going on to build lots of useful electronic", 
+    "systems.", 
+    "But before we go and build these systems, much like a", 
+    "carpenter who needs to go build a house, much like a", 
+    "carpenter has to go and buy a set of tools from the local", 
+    "store, we need to go and make sure that you have the tools", 
+    "in your tool chest to analyze these circuits.", 
+    "This tool chest will include things like the KVL KCL", 
+    "method, the Node method and so on.", 
+    "But before I begin talking about these techniques for", 
+    "your tool chest, I'd like to do a extremely quick review--", 
+    "as is my usual practice--", 
+    "of what you've covered so far.", 
+    "So remember our EECS playground.", 
+    "We've gotten into this place by promising that we are going", 
+    "to observe the lumped matter discipline.", 
+    "By observing the discipline recall that the complexities", 
+    "of Maxwell's equations and the differential equations that", 
+    "you have to solve-- the partial differential", 
+    "equations-- goes away.", 
+    "And you're left with very simple linear equations.", 
+    "And you will see a lot of that today.", 
+    "As you make the lumped matter discipline, you end up with", 
+    "these lumped elements, like resistors and voltage", 
+    "sources and so on.", 
+    "And what you do with these lumped elements is we can", 
+    "label what are called the branch variables or the", 
+    "terminal variables for these lumped elements, OK?", 
+    "So for example, v is the voltage across the element.", 
+    "And i is the current through the element.", 
+    "The power consumed by the element is given by vi.", 
+    "Continuing with our review, the lumped matter discipline", 
+    "enables us to create the lumped circuit abstraction.", 
+    "So you take these lumped elements and you connect them", 
+    "with ideal wires.", 
+    "So in this case, I have a resistor which is a lumped", 
+    "element, a voltage source.", 
+    "And I connect them with these ideal wires.", 
+    "And what you end up with is called a lumped circuit.", 
+    "But this is your lumped circuit abstraction.", 
+    "Well as we made the transition from physics to EECS by", 
+    "adhering to the lumped matter discipline.", 
+    "I had discussed in the last sequence that Maxwell's", 
+    "equations turn into very simple algebraic equations.", 
+    "And these are captured by Kirchoff's voltage and current", 
+    "laws, called KVL and KCL.", 
+    "So KVL says that for all loops in your circuit, the sum of", 
+    "the voltages around the loops add up to zero.", 
+    "Similarly for all the nodes in the circuit, the currents that", 
+    "enter into a node add up to zero.", 
+    "And in the same matter, if I just summed the currents", 
+    "leaving a node, they also add up to zero.", 
+    "So whether you sum the currents entering the node or", 
+    "currents leaving a node, they would add up to zero by KCL.", 
+    "And the beauty of this was by adhering to lump matter", 
+    "discipline, recall the complexities Maxwell's", 
+    "equations whether an integral form or", 
+    "differential form went away.", 
+    "And we were now left with extremely simple algebraic", 
+    "expressions of the sort.", 
+    "And you will see shortly that you will end up solving", 
+    "extremely simple linear equations", 
+    "as we analyze circuits.", 
+    "So as one example here is a linear circuit.", 
+    "It has one, two, three, four, five, six elements.", 
+    "It's got a voltage source of a voltage v zero.", 
+    "It's got a resistor, r one and so on and so forth.", 
+    "So for this circuit according to our abstraction and the", 
+    "laws of KVL and KCL, the following", 
+    "are going to be true.", 
+    "So for instance if I look at node a, then according to KCL,", 
+    "the currents entering the node must be zero.", 
+    "So in other words, the current here is ica.", 
+    "And I can sum to that the current", 
+    "entering from the d direction.", 
+    "So that would be plus ida.", 
+    "And then there is a current from the ba direction and iba.", 
+    "Those are going to sum to zero.", 
+    "Now I can multiply the whole thing by minus 1.", 
+    "And that would give me the sum of the currents leaving the", 
+    "node are also going to be zero.", 
+    "So that is KCL.", 
+    "Now I can also write KVL in this case for this loop, for", 
+    "instance, here.", 
+    "For this loop I can add up the voltages around the loop.", 
+    "And by KVL they must add up to zero.", 
+    "So for example if I look at the voltage vca, I can add", 
+    "that to the next voltage here.", 
+    "That is to vab and then add that to the", 
+    "final voltage, vbc.", 
+    "And by KCL--", 
+    "so all of those must add up to be zero.", 
+    "Now if you go back to our circuit here that you see on", 
+    "the left hand side, I am going to show you a little demo that", 
+    "will look at these currents, ica, ida, and iba, and also", 
+    "look at the voltages, vcabab and bbc and actually go and", 
+    "look at the circuit, make the measurements, and show that", 
+    "they indeed sum up to zero.", 
+    "Not surprising.", 
+    "KVL and KCL really work.", 
+    "And so the demo should also work.", 
+    "OK.", 
+    "So let's go and do our demo."
+  ]
+}
\ No newline at end of file
diff --git a/subs/pnHDLuxmXHo.srt.sjson b/subs/pnHDLuxmXHo.srt.sjson
new file mode 100644
index 0000000000..6a6f2be8d6
--- /dev/null
+++ b/subs/pnHDLuxmXHo.srt.sjson
@@ -0,0 +1,251 @@
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+  "text": [
+    "SPEAKER 1: OK.", 
+    "I'm now going to show you a demo of superposition in", 
+    "action with something you see every day in real life.", 
+    "So in this demo, I am going to have an empty", 
+    "vat to begin with.", 
+    "And then what I'm going to do is I'm going to pour some salt", 
+    "water into it.", 
+    "OK, some salt water poured into it will behave like a", 
+    "distributed resistance.", 
+    "And so each small volume of water can be modeled as a", 
+    "lumped resistor.", 
+    "And so you end up with this three-dimensional connected", 
+    "network of resistors.", 
+    "Now, this is a linear circuit.", 
+    "And we will see superposition in action with this circuit.", 
+    "So what do is I'll connect one input to it, which will be a", 
+    "high-frequency triangular wave, like so.", 
+    "OK, that'll be input at one part of the water.", 
+    "And then I will input a low-frequency sinusoid at a", 
+    "different location.", 
+    "So those are my two inputs.", 
+    "And as we've seen before, you can think of", 
+    "these as V1 and V2.", 
+    "And what I'm going to do is I'm going to observe the", 
+    "output at a third port.", 
+    "And my goal will be to take a look at what", 
+    "this input looks like.", 
+    "If superposition truly holds true, then this output should", 
+    "really show both a component that relates to V1 and another", 
+    "component that clearly relates to V2, if", 
+    "superposition really worked.", 
+    "OK?", 
+    "So let's go on to the demo.", 
+    "And as I said before, in the demo, you will see a vat, an", 
+    "empty vat to begin with, into which I will add salt water.", 
+    "And then we will take a look at what happens at the output", 
+    "as I apply two input voltages to it.", 
+    "This is a vat of nothing, right, and it's all empty.", 
+    "So this is a screen of the oscilloscope now.", 
+    "So notice that I have a sinusoid, and I have a", 
+    "triangular wave.", 
+    "And the output is zero.", 
+    "And the reason is there's nothing in this vat.", 
+    "It's empty.", 
+    "Previously when I taught this course, I would get salt water", 
+    "and pour salt water.", 
+    "Then we discovered a much better source of water that", 
+    "conducted electricity, like one real mean", 
+    "fluid, Cambridge water.", 
+    "It just works very pleasantly.", 
+    "It just conducts electricity like nothing at all.", 
+    "And I've been thinking of using Charles River water next", 
+    "time and see what happens.", 
+    "Although there, we'd probably get some biological organisms", 
+    "doing strange things at you.", 
+    "But go ahead.", 
+    "OK, so our friendly demonstration expert, Lorenzo,", 
+    "will pour some water into the vat.", 
+    "And you should begin seeing the output begin superposition", 
+    "now of the two.", 
+    "You see that?", 
+    "So you do see the sinusoidal articulation", 
+    "and the jagged waveform.", 
+    "And just to have some more fun, what I can do is increase", 
+    "one of the voltages.", 
+    "And you'll see.", 
+    "[LAUGHTER]", 
+    "SPEAKER 1: Now you know what would have happened if I'd", 
+    "used Charles River water.", 
+    "OK.", 
+    "So my output keeps increasing as I increase the", 
+    "corresponding waveform.", 
+    "OK?", 
+    "I could do this.", 
+    "This is fun.", 
+    "OK.", 
+    "So let me pause there and go on to the next topic.", 
+    "So that little demonstration showed you that even something", 
+    "as simple as this physical entity, a vat of water,", 
+    "behaves like a linear system.", 
+    "And we can model that linear system as a set of resistors."
+  ]
+}
\ No newline at end of file
diff --git a/subs/rysqcHqcuBw.srt.sjson b/subs/rysqcHqcuBw.srt.sjson
new file mode 100644
index 0000000000..92b5ee3afb
--- /dev/null
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+  "start": [
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+  "text": [
+    "INSTRUCTOR: Based on the previous method or the", 
+    "previous property that you saw for linear circuits, we are", 
+    "now ready to define the superposition method for", 
+    "circuit analysis.", 
+    "Note that the superposition method", 
+    "applies to linear circuits.", 
+    "And again, to refresh your memory, remember, we are in", 
+    "the EECS playground that we got into by adhering to the", 
+    "lumped matter discipline.", 
+    "And within that, we looked at the node method and the KVL", 
+    "KCL method that applies all over the EECS playground.", 
+    "And then what we'll now do is look at some methods that will", 
+    "apply to only a region of this playground where linear", 
+    "circuits reside.", 
+    "So the first of these methods is the superposition method.", 
+    "And again, it applies to linear circuits.", 
+    "So the method is very simple and inspired by the", 
+    "superposition property that we studied for linear circuits.", 
+    "So the method simply says this.", 
+    "You first find the responses of the circuit to each source", 
+    "acting alone.", 
+    "Think of this as a divide and conquer method where you take", 
+    "your entire circuit, and you find the responses of the", 
+    "circuit to each source acting alone.", 
+    "You turn off all the sources, and you find the response to", 
+    "each source acting alone.", 
+    "Then what you do is simply sum those individual responses.", 
+    "Note that this technique applies to", 
+    "independent sources only.", 
+    "So if I have a linear circuit, then this technique applies to", 
+    "independent sources only.", 
+    "Now we will look at what happens when you have", 
+    "dependent sources and so on in later lectures.", 
+    "OK, let's move ahead.", 
+    "The first step was find the response of the circuit to", 
+    "each source acting alone.", 
+    "But what does it mean for each source to act alone?", 
+    "What it means is that you turn off all the other sources.", 
+    "So for example, suppose we are focused on a", 
+    "voltage source here.", 
+    "What does it mean to turn off this voltage source?", 
+    "In other words, if I want to set this voltage to 0, what", 
+    "does it mean in terms of my circuit?", 
+    "So in terms of my circuit, what this means is that I am", 
+    "going to short the source.", 
+    "So what you do is you short the source, and you end up", 
+    "with a short circuit here.", 
+    "And that is my voltage source having been set to 0.", 
+    "And so I take all my voltage sources in the circuit and", 
+    "simply short them out.", 
+    "And this would be making each of the sources to act alone.", 
+    "OK, next let's look at a current source and see what it", 
+    "means to set a current source to 0.", 
+    "So in this case, what you do is much as you set a voltage", 
+    "source to 0 by shorting it out, you set the current", 
+    "source to 0 by open-circuiting it like so.", 
+    "So you create an open circuit in place of the current", 
+    "source, and that's what it means to set a", 
+    "current source to zero.", 
+    "OK, so now we are ready to go try out an example using the", 
+    "method of superposition.", 
+    "And again, remember the method of superposition has", 
+    "two parts to it.", 
+    "In the first part, you find the responses of the circuit", 
+    "to each source acting alone.", 
+    "And then second, you sum up the partial responses.", 
+    "So let's go back to our old faithful example.", 
+    "In this example, we have two sources, a voltage source and", 
+    "a current source.", 
+    "And let's say our goal is to find the node voltage e taken", 
+    "with respect to this ground.", 
+    "And we are going to use the superposition", 
+    "method to do the circuit.", 
+    "So I showed the circuit on the right-hand corner here.", 
+    "And notice that e is the node voltage that I", 
+    "need to figure out.", 
+    "So by the superposition method, I have two steps.", 
+    "My first step is find the responses of the circuit to", 
+    "each source acting alone.", 
+    "So what I'm going to do is let me start with finding the", 
+    "response of the circuit to the voltage source acting alone.", 
+    "So what do I do to get a subcircuit in which the", 
+    "voltage source is acting alone?", 
+    "So I want you to think about this and try to figure out", 
+    "what the resulting subcircuit is going to look like.", 
+    "I'll give you a few seconds to do that before I do it myself."
+  ]
+}
\ No newline at end of file
diff --git a/subs/wO-WqB_k9QQ.srt.sjson b/subs/wO-WqB_k9QQ.srt.sjson
new file mode 100644
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+  "text": [
+    "SPEAKER 1: So before I wrap up the node method, I wanted to", 
+    "take some time and show you something interesting, largely", 
+    "for your cultural interest. This is not required for the", 
+    "course, and so this is optional.", 
+    "I want to show you how these equations are really solved in", 
+    "real life and how computers can be used to do this for us.", 
+    "So if you go back to step four of the node method, you recall", 
+    "we had these two equations and two unknowns, where the", 
+    "unknowns were e1 and e2.", 
+    "I can turn these into matrix form, like so, where I have", 
+    "matrix times a column vector equals another column vector,", 
+    "and where I get a two-by-two matrix called the", 
+    "conductivity matrix.", 
+    "I get a column vector of the unknown node voltages.", 
+    "And I get a column vector of the source voltages.", 
+    "So I've taken my system of equations and converted them", 
+    "into the matrix notation, like so.", 
+    "And the way this works is each of these equations can be", 
+    "obtained by doing a row column multiply.", 
+    "So if I multiply the first row with this column here, I take", 
+    "e1, multiply that by G1 plus G2 plus G3, I get", 
+    "the first term here.", 
+    "I take e2, multiply that by minus G3, I", 
+    "get the second term.", 
+    "And I equate that to G1V0.", 
+    "Similarly, to get the second equation, I would take the", 
+    "second row and multiply that by the same column vector.", 
+    "Now, let's take a look at how things like", 
+    "this might be solved.", 
+    "So here is my matrix equation again, with a two-by-two", 
+    "matrix multiplying a column vector equal", 
+    "another column vector.", 
+    "So we can use many sophisticated techniques to", 
+    "analyze systems like this.", 
+    "And if you've done courses in linear algebra, you would've", 
+    "noticed that linear algebra spends a lot of time trying to", 
+    "analyze systems of this sort, where A is some matrix, x is a", 
+    "column vector of unknowns, and b is a", 
+    "column vector of knowns.", 
+    "And so you often have to go and solve for the column", 
+    "vector of unknowns.", 
+    "Now, with circuit analysis, if I have a circuit containing", 
+    "millions of elements, I would have a column vector here,", 
+    "which had a million elements.", 
+    "And so clearly we would love to use computers to do that.", 
+    "And not surprisingly, that is what to", 
+    "do in circuit analysis.", 
+    "In fact, the lab that you work on in 6002-X has the schematic", 
+    "capture system where you can build circuits.", 
+    "But for the analysis, the computer programs that are", 
+    "used to analyze the voltages and so on, and show them to", 
+    "you, use methods very similar to this, where you use these", 
+    "sophisticated linear algebraic solvers that solve systems of", 
+    "equations of the form Ax equals b.", 
+    "So back to our system.", 
+    "I can go ahead and solve the system.", 
+    "I won't bore you with the details of", 
+    "the agony of algebra.", 
+    "I've gone ahead and solved these equations for you.", 
+    "And so I get e1 and e2 are expressed as fairly big", 
+    "equations of the sort.", 
+    "So one interesting fact that I mentioned to you was you end", 
+    "up with systems of equations that you", 
+    "can solve with computer.", 
+    "There's one other interesting fact.", 
+    "Notice that the circuit that we used, our demo", 
+    "circuit, was linear.", 
+    "It was composed of linear elements and so on.", 
+    "And so notice here that e1 is also related to a set of", 
+    "linear terms. So notice that this equation here is linear", 
+    "in V0, i1, V0, and so on.", 
+    "And it is all in linear terms. Also note that there are no", 
+    "negatives in the denominator.", 
+    "So the fact that this is linear in the constant sources", 
+    "will be used in a later sequence that we will cover in", 
+    "a few days.", 
+    "So watch out for that.", 
+    "So just to wrap up and just go through the motions here, let", 
+    "me just go ahead and solve for e2 just for kicks.", 
+    "And I'll do it for values G1, G5, and then so on and so", 
+    "forth, given here, and for i1 chosen to be 0, just for fun.", 
+    "And so if I plug these numbers into the equation for e2 that", 
+    "I just showed you, I'm going to get e2 as a function of V0,", 
+    "as follows.", 
+    "Then e2 is going to be 0.6 times V0.", 
+    "And so if I pick V0 to be three volts, then e2 is going", 
+    "to be 1.8 volts.", 
+    "So there you have it."
+  ]
+}
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