For more information, please see full course syllabus of Math Analysis
For more information, please see full course syllabus of Math Analysis
Formal Definition of a Limit
- We need two new greek letters: Delta⇒ δ Epsilon⇒ ε
- Formal Definition of a Limit: Let f be a function defined on some interval (a,b) of the real numbers, where a < b. Let c ∈ (a,b) and L be a real number. Then,
lim
f(x) = L - The first half of the definition sets up the groundwork. The function is defined, there is a horizontal location we're approaching (c), and some vertical location the function goes towards (L).
- The second half of the definition is the difficult part. It says that for any ε > 0 boundary around L, we can restrict our x to within some δ > 0 boundary of c to force f(x) to stay within the ε-boundary around L.
- Check out the video to see some diagrams and more explanation of this idea. It's a confusing idea at first, and it takes awhile to make sense of it.
- We can imagine a limit as a sort of never-ending debate between two people. One person gives hypothetical ε-boundaries, while the other person has to defend by giving a δ-boundary that would keep the function within the ε-boundary.
- To formally prove a limit exists, we must show that for any ε > 0, there will always be some δ > 0. This normally takes the form of creating a formula for δ based off ε, because if we can create such a formula, then we will have shown δ will exist no matter what ε is chosen.
Note: Very few students will have any use for what is in this lesson, let alone during a pre-calculus level course. Problems based on the formal definition of a limit are extremely rare in calculus class. This stuff won't come up in science classes, and will only be necessary in high-level college math. Still, if you're interested in math for math's sake or know that you want to one day study higher level mathematics, check this lesson out. It's okay if it doesn't all make perfect sense today, but seeing these ideas now will help you down the road when it starts mattering. Plus, it's fascinating stuff!
Formal Definition of a Limit
Lecture Slides are screen-captured images of important points in the lecture. Students can download and print out these lecture slide images to do practice problems as well as take notes while watching the lecture.
- Intro
- Introduction
- New Greek Letters
- Formal Definition of a Limit
- What does it MEAN!?!?
- The Groundwork
- Set Up the Limit
- The Function is Defined Over Some Portion of the Reals
- The Horizontal Location is the Value the Limit Will Approach
- The Vertical Location L is Where the Limit Goes To
- The Epsilon-Delta Part
- The Hard Part is the Second Part of the Definition
- Second Half of Definition
- Restrictions on the Allowed x Values
- The Epsilon-Delta Part, cont.
- The Adventure of the Delta-Epsilon Limit
- The Adventure of the Delta-Epsilon, cont.
- This Game is About Limits
- What If I Try Larger?
- Technically, You Haven't Proven the Limit
- Here is the Method
- What We Should Concern Ourselves With
- Investigate the Left Sides of the Expressions
- We Can Create the Following Inequalities
- Finally…
- Nothing Like a Good Proof to Develop the Appetite
- Example 1
- Example 2
- Intro 0:00
- Introduction 0:06
- New Greek Letters 2:42
- Delta
- Epsilon
- Sometimes Called the Epsilon-Delta Definition of a Limit
- Formal Definition of a Limit 4:22
- What does it MEAN!?!? 5:00
- The Groundwork 5:38
- Set Up the Limit
- The Function is Defined Over Some Portion of the Reals
- The Horizontal Location is the Value the Limit Will Approach
- The Vertical Location L is Where the Limit Goes To
- The Epsilon-Delta Part 7:26
- The Hard Part is the Second Part of the Definition
- Second Half of Definition
- Restrictions on the Allowed x Values
- The Epsilon-Delta Part, cont. 13:34
- Sherlock Holmes and Dr. Watson
- The Adventure of the Delta-Epsilon Limit 15:16
- Setting
- We Begin By Setting Up the Game As Follows
- The Adventure of the Delta-Epsilon, cont. 17:24
- This Game is About Limits
- What If I Try Larger?
- Technically, You Haven't Proven the Limit
- Here is the Method
- What We Should Concern Ourselves With
- Investigate the Left Sides of the Expressions
- We Can Create the Following Inequalities
- Finally…
- Nothing Like a Good Proof to Develop the Appetite
- Example 1 31:02
- Example 1, cont.
- Example 2 41:46
- Example 2, cont.
Math Analysis Online
Transcription: Formal Definition of a Limit
Hi--welcome back to Educator.com.0000
Today, we are going to talk about the formal definition of a limit.0002
In this lesson, we will explore the formal definition of a limit.0005
Previously, we defined a limit with intuitive terms, like "approach" and "goes to."0007
Now, we are getting serious, and it is time for some really technical stuff.0012
However, I want to point out that very few students will have any use for what is in this lesson, let alone during a precalculus-level course.0015
I want you to have the option to know the formal definition, if you are interested.0025
But most people will not need it, even in math class.0028
Problems based on the formal definition of a limit are extremely rare in calculus class--maybe as a bonus question, but probably no more.0031
This stuff won't come up in science classes, and it will only be necessary for high-level college math.0040
And when I say "high-level college math," I mean that this stuff is really going to only definitely start showing up0047
by the second or third year of taking advanced college math courses.0051
This stuff is not going to show up any time soon, so I really just want to be frank with you and honest:0055
what I am going to teach here is really a totally optional lesson.0060
It is not going to come up in the course that you are currently taking; I guarantee you that.0064
And it may or may not come up in the next course you take, if you go on to take calculus.0068
But it is really, really unlikely to be tested heavily.0072
It will maybe be a bonus question, or maybe one real question; but for the most part, you are not going to see this formal limit definition.0075
It just doesn't show up; it has very little direct applicability in the sciences; it is only used for some pretty advanced ideas in mathematics.0083
It is really important for building advanced ideas in mathematics.0091
But for day-to-day use of mathematics, we just never really need to see it.0094
Unless you are particularly interested in mathematics, or you know that you really want to go into high-level physics,0098
or you are interested in something like computer programming, where you will have to get enough mathematics learned,0103
at some point, that you will end up needing to be able to understand those advanced math concepts,0107
you are probably never going to end up encountering this formal definition, ever.0111
And that is totally OK; wanting to learn this sort of thing--I know that it is not for everybody.0115
But for me, I personally love this stuff; this is the reason I love math--because there are these really cool, complex,0119
strange, puzzling logic ideas that make this really interesting structure that is just fascinating--to me, at least.0127
So, I think this stuff is totally awesome.0133
If you are not interested, don't worry about it; skip this lesson.0136
There is going to be some really difficult stuff, and there is not really a whole lot of direct personal need to understand it.0139
But at the same time, there is not really a whole lot of direct personal need to go to a museum; you do it because you are interested in the art.0144
And that is the same reason that you might be interested in mathematics.0150
It is the reason I am interested in mathematics--just because I find it personally satisfying and cool.0153
If you are interested, let's go and check some stuff out.0157
OK, and before we keep going, I just want to say, for those of you who decided to stay around, thanks.0162
I think this stuff is really, really cool; I am glad to get the chance to share it with you.0166
And I think it is really, really cool; I hope you end up liking it as much as I do.0170
We few, we happy few, we mathematicians--we get to see this.0175
All right, we are going to need some new Greek letters before we get started.0180
That is right: this stuff is so cool that we need to bring out the new Greek letters.0183
Our first one is delta, and these are the lowercase versions; so δ is lowercase delta, and ε is lowercase epsilon.0187
Here is δ; and if you are going to draw it by hand, it is kind of hard to draw this thing exactly as it ends up getting typeset.0194
So, I would recommend...you want something on the top, and then sort of a curved loop like that.0201
You might end up seeing me write it like that, as I am writing it pretty quickly.0206
But that is a pretty good idea of what you are trying for.0209
This one is kind of not a very good one; but put some sort of curved loop on top, and then a sort of circular thing on the bottom.0211
And that will be enough for most people who understand mathematics to realize that you are trying to write delta.0217
You don't have to ahve it absolutely perfect, because they will know what the symbol is, especially when they end up seeing it a bunch of times.0221
Epsilon is considerably easier to draw; it is just sort of a backwards 3; that is it.0226
That is ε; that one is easier than δ, I would have to say.0231
All right, the formal definition that we are about to see involves these letters.0233
So, it is sometimes called the (ε,δ)-definition of a limit, or just the formal definition of a limit.0238
We just talked about the intuitive idea of what a limit is; and that is a really great way to think about limits.0244
But sometimes you really need to get to the basic facts and turn intuitive ideas into precise things, so that you can say "this is what it is."0249
And that is what this definition is for.0256
All right, let's get to it: the formal definition of a limit.0257
Let f be a function defined on some interval a to b of the real numbers, where a is less than b.0261
Let c be contained in a to b, and let l be a real number.0268
Then, the limit, as x goes to c, of f(x) = l means that, for any real ε greater than 0,0274
there exists some δ greater than 0 such that, for all x where 0 is less than the absolute value of x - c,0282
which is less than δ, we have the absolute value of f(x) minus l is less than ε.0289
What? Don't worry: if you found that definition confusing, that is exactly how I felt when I first heard it.0296
The first time you see this, you think, "What is going on?"0304
That is totally OK; it is something that you pick up and work through slowly, over time.0307
If you opened a book for the very first time, you wouldn't expect to be able to understand every word on the page.0311
It is something you have to work through; it is OK--you are building up these ideas of understanding it.0316
It is not something that is going to make sense exactly the first time.0319
It is something that makes sense over time; that is totally fine.0322
So, we will start working through it, step-by-step, and we will see some ways to understand what is going on in this definition--0325
to see how we can parse this thing and make sense of it.0330
All right, first, let's get the basics out of the way, the ground work here.0333
The first half of the definition is just setting up the limit; that is what we end up getting in this first half.0337
Let f be a function defined on some interval a to b (they are real numbers) where a is less than b, and c is contained in a to b, and l is some real number.0342
All right, let's break that down, piece by piece.0352
First, let f be a function defined on some interval a to b.0354
That just means that it is a function, and it is defined over some portion of the reals.0358
There is some piece of it that it ends up working in.0363
It is basically just saying that this function is defined somewhere; that is all that we are saying.0366
There is some chunk of the reals where this function makes sense.0370
This part where we say a < b is just a guarantee that we don't accidentally say a = b, and we end up having something that doesn't make sense.0373
It is so that we know that we are going from some a, up until some b; that is our interval of where the function is defined.0379
Next, the horizontal location c, contained inside of (a,b): remember, this symbol just means "inside of."0386
So, (a,b) is a set of all possible values; it is the interval, and that symbol just means that c is inside of that set of possible values.0393
So, the horizontal location c contained inside of (a,b) is the value that the limit will approach.0400
That is the thing where we are getting closer and closer to that, and we are seeing where we end up going to.0406
So, c is just a location that we are getting towards; that is the value that the limit will approach.0412
And finally, l is some real number; l's real number is the vertical location that we end up going to.0417
That is where the limit will go to; we are setting the l that we are saying our limit ends up going to as we approach this c.0424
So, that is the basics that we are setting up: f is some function; it works on some chunk.0432
c is where we are going to, and l is the value that we end up meeting up at, that we are headed towards.0436
All right, the hard part is the second half of the definition.0443
The limit as x goes to c of f(x) = l means that, for any real ε greater than 0, there exists some real δ greater than 0,0447
such that for all x where 0 < |x - c| < δ, we have f(x) - l < ε; OK.0455
To break this up, we want to be able to focus on this one piece at a time.0462
So, what we are going to do is focus on the ε portion first.0465
It will be easier to understand that; and then we will see the δ part in that idea.0468
So, for any real ε greater than 0: what that means is that, if we just grab some ε--0473
we just say some number, like 1 or 1/2 or whatever number we feel like saying,0479
we will end up having this be true later on: that the absolute value of f(x) - l is less than ε.0483
Now, that might be kind of hard to understand: the absolute value of f(x) - l is less than ε...0490
we are not used to working with absolute value that much; it is kind of confusing.0493
But remember one of the things we talked about when we first talked about absolute values.0496
Absolute value is a way of seeing the distance between two things.0499
If we have the absolute value of m - n, if we have the absolute value of q - r, that is a way of saying the distance between those two points.0502
The absolute value of some object minus some other object is just a way of saying how far those two objects are from each other.0512
That is one of the ideas that we have from absolute value.0519
When we say the absolute value of f(x) - l, what we are really saying is how far f(x) and l are from each other.0522
Now, that means, with the combination of ε being greater than 0, and the distance between f(x) and l being less than ε...0529
what we are doing is saying that there is this boundary around l.0537
The maximum distance f(x) can be from l, the distance between f(x) and l, has to be less than ε, this thing right here.0540
Since the distance between our f(x) and our l is less than ε, it means that our f(x) has to be within ε distance of l.0549
We effectively create a boundary that we hold f(x) inside of.0556
Whatever our f(x) ends up being, it has to be somewhere inside of this boundary.0560
If it is outside of the boundary, like this, that is not allowed, because it would fail to be within ε distance of the l.0565
We end up seeing...we have that our l is here, and then the ε's here are just the distance that we end up having for that boundary.0574
We are setting a boundary that is ε distance out from the l.0583
But notice: it has to be true for any ε that we set, so we will be able to create a boundary at whatever size we decide to make,0587
whether it is a giant ε boundary or a really tiny ε boundary.0593
It will always end up working for this next part that we are about to work towards.0596
OK, the second half of the definition (continuing with that): previously, we saw ε as a boundary around the height l.0600
The absolute value of f(x) - l is less than ε means that f(x) has to be, at most (has to be less than), the distance of ε from l.0607
We know that we have to be somewhere contained inside of this boundary in here.0617
OK, now let's move on to looking at δ.0624
What does δ get us? What we did is went and set up for any real ε greater than 0; we had this boundary get set up.0628
So, with that boundary in mind, we now have to go on to say that there exists some real δ greater than 0,0639
such that, for all x where 0 is less than x - c, which is less than δ, we will end up having this |f(x) - l| < ε be true.0646
So, what we are doing is putting a restriction on the allowed x-values.0657
The δ sets some restriction on it: you can't get any farther from c than δ.0663
So, what we are doing is saying, "Remember: the |x - c| is saying the distance between x and c."0669
So, the distance between x and c has to be less than δ.0677
So, if the distance between x and c is less than δ, that means that we have set up, once again, a boundary of how far our x is allowed to roam.0681
And we know that what has to come out of this is: we have to have...0689
if we set x's within that boundary, we will end up having the |f(x) - l| being less than ε.0693
So, if you use x's from inside of this boundary here, we know that we end up having to be mapped into the f(x) that is within that vertical boundary.0702
We are setting up some set of boundaries on what x is that we can have.0713
And we know for sure that we have to have it so that they end up getting mapped inside of this ε.0718
The other thing to notice is that it says that 0 is less than |x - c|, that 0 is strictly less than the absolute value of x - c.0724
It means that x cannot be equal to c, because then we would have an absolute value of 0.0731
We would have x = c; but since it is a limit, we are not concerned with x = c.0735
Remember: we are not concerned with the destination; we are concerned with the journey.0738
So, that means we care about the part with the boundary, but not the actual thing in the middle.0741
That is what that 0 < |x - c| means: that we are guaranteed that we can't have x equal to c,0745
and |x - c| < δ means that we are bounded δ distance, at maximum, from the c in that middle.0753
And everything inside of it ends up getting mapped inside of this boundary here.0761
It will be easier to see what is going on if we erase some of this.0767
What we are doing here is: we can think of it as: some ε gets created around our l that sets up a boundary.0770
We know that you have to be somewhere on this portion vertically.0781
And then, we set some δ radius around our c, so that it ends up mapping only to those vertical locations there.0785
We set ε, and then we have to be able to always set some δ from that ε0797
that will end up mapping us inside of that vertical chunk--that we say that,0801
if we are close enough to this value of c, we will always come out close enough to that value of l.0805
OK, now the really important idea is that we can do this for any ε greater than 0 whatsoever.0813
That is, for any ε greater than 0, there has to exist some δ greater than 0,0818
such that, for x within δ of c, if we are close enough to c, f(x) will end up getting mapped within ε of l.0825
If you are close enough to c, you will end up being close enough to l.0833
We can imagine this process as a never-ending dialogue of ε challenges against δ defenses.0836
Someone says, "Is it possible to stay within this distance of our l?" and we say, "Yes, as long as we are within this distance of our c."0842
And then, they say, "OK, is it possible to stay within this distance of our l, this ε of our l?"0849
We say, "Yes, as long as we are within δ distance of c."0853
So, some ε gets named; for any ε named, there has to be a δ that will cause us to stay within ε away from that l.0856
Otherwise, if we can't do this, then the limit does not exist.0865
But if we can do it, forever and ever and ever, then that means that the limit does exist.0869
If for any ε that gets named, there is always a δ, then that means that the limit does exist.0872
Now, of course, we can't actually have this process of ε challenge and δ defense; we can't do this forever.0877
We can't do this for eternity, so we have to figure out another way to do this.0882
If we wish to truly prove a limit, we have to prove that there will always be some δ greater than 0,0885
given some ε greater than 0--that if some ε gets named, there is always a method0892
that will create the appropriate δ, so that we can get within ε of that limit l.0896
OK, now what we are going to go onto is: we are going to see both of these ideas.0902
Both of these ideas will be explored in the next scene that will be played out by Sherlock Holmes and Dr. Watson.0906
All right, the setting is late afternoon in Sherlock Holmes's apartment.0912
He and Dr. Watson are lounging about.0918
"Let us play a game, Watson!" "All right, Holmes, what type of game?"0921
"A game of limits." "I do not believe I have ever..."0924
"Do not worry: I shall teach it to you. We begin by setting up the game as follows."0927
"One of us (I, in this case) claim the existence of a limit; I name some function f(x)0932
and some value l that the function will approach as x approaches some number c."0938
"Written out, we have the limit as x goes to c of f(x) is equal to l."0944
"All right, that makes sense enough." "Good; after that, the game in earnest begins."0951
"The opposing player (you, in this case) names an ε greater than 0."0955
"It will then be the first player's job to name some δ greater than 0, such that,0959
for all values of x within δ distance of c, except x = c (we don't care about x = c in this game),0964
they will cause f(x) to be within ε of l."0972
"So, if we use one of those x's that is within δ of c, we know that the f(x) that will be produced by that x will have to be within ε of l."0975
"I think I understand." "Let me write it out: I will name some ε greater than 0 that sets up some boundary around l."0983
"So, we have some l - ε to l + ε boundary; we are going to be in that interval vertically."0990
"Then, you name a δ greater than 0 such that, for x contained within c - δ to c + δ,0997
that horizontal bounding, we will end up getting f(x) contained in l - ε to l + ε;1005
that is to say, the boundary that we set around l in the first place."1012
"I will set some boundary vertically, and then you will respond with some horizontal boundary that will put our function inside of that vertical boundary."1016
"Very good, except one important thing: we do not concern ourselves with x = c."1024
"For this game, x is not equal to c; we never actually consider x equaling c, so x is not equal to c, generally."1034
"All right, I understand: you set up a limit; I challenge it with some ε greater than 0, and then you defend with some δ greater than 0."1042
"One question, though: why can't ε equal 0?"1050
"I understand that δ must be greater than 0, because we must have x not equal to c;1054
if δ is greater than 0, then we know that we can't actually be on top of x = c, so x is not equal to c. But why not ε = 0?"1059
"Because this is a game about limits! If you set ε = 0, we would be stuck on l."1067
"We wouldn't have a boundary around it; we would be stuck there."1074
"We need a boundary around l, so that we can talk about approaching it;1077
the entire idea about a limit is to talk about going towards it, approaching it."1082
"It is similar to why we must have x not equal to c; otherwise there is no approaching it, if we are stuck on top of it."1086
"So, we can't be stuck on top of it, either vertically or horizontally; that is why we can't have ε or δ equal to 0."1092
"Makes sense; so what comes next?" "That is it; we stay with the same limit,1098
but the process of ε challenges and δ defenses repeats for as long as we care to play."1103
"If you manage to give an ε that stumps me, you win! You will have shown the limit false."1109
"Let us begin; what will your limit be?" "I choose the following limit to defend: limit as x goes to 3 of x^{2} + 2 = 11."1115
"All right, I begin by challenging with ε = 1." "I defend with δ = 0.1."1123
"Since x contained within the interval 2.9 to 3.1 (notice: that is a δ of .1 away from our c of c = 3),1130
if x is contained within 2.9 to 3.1, it will give f(x) contained within 10.41 to 11.61."1141
"And that means I am easily within an ε value of 1 from our l of 11."1148
"Thus, my defense stands: using δ = .1, I stay within ε of 11."1153
"OK, how about ε = 0.05." "I will go with δ = 0.005."1159
"Since x contained within 2.995 to 3.005 causes f(x) to be contained within 10.97 to 11.03, I am within ε of 11, so my defense stands again."1167
"What if I tried larger...I set ε = 10!" "Nice try, old chap, but I already showed that δ = 0.1 works for ε = 1."1179
"Therefore, it must work for ε = 10 as well; if you started out small, and then you get bigger,1190
well, I can just leave my δ the same, and it will work just fine for the larger vertical boundary, as well."1195
"Thus, there is no hope for going larger with your ε.1200
Since I have already shown that it works for a small ε, it will automatically work for a larger ε, as well."1204
"Hmm...fine, deal with this: ε = 0.000001." "Elementary, my dear Watson: δ = 0.0000001."1209
"Notice that, if x is contained within 2.9999999 to 3.0000001, we will have f(x) contained within 10.9999994 to 11.0000006."1220
"That is to say, it will be contained within an ε of 11; thus, my defense is still standing."1237
"All right, Holmes; you have me convinced--I believe that, no matter what ε I say, you will be able to defend with an appropriate δ."1244
"But technically, you haven't proven the limit; we can't play this game for eternity."1251
"So, how can you prove that δ will always exist?"1257
"An astute question, Watson; the answer is by showing that there exists some method1261
to create δ from any given ε, and that the method never fails."1266
"I will tell you the method I am using, and then show that it always works."1272
"Of course, you already have a method." "Naturally; here it is: for any ε greater than or equal to 1,1276
I will simply respond with δ = 0.1; as we discussed earlier, δ = 0.1 works for ε = 1,1281
so it will work for any ε greater than or equal to 1."1288
"On the other hand, for ε between 0 and 1 (that is, 0 < ε < 1), I will use δ = ε/10."1291
"Wait; how do we know that δ is greater than 0?"1301
"Well, we know that ε is greater than 0; and since we are creating δ1304
by dividing ε by 10, we know that δ must be greater than 0, as well."1310
"If ε is greater than 0, then we know that dividing something that is greater than 0 doesn't cause it to become 0,1316
and doesn't cause it to become negative; it simply makes it smaller."1322
"So we know that δ must be greater than 0, as well, because we simply divided1325
something that was already greater than 0 by some positive number--in this case, positive 10."1329
"Now, let me prove to you that δ = ε/10 always works."1333
"Notice that, since we are working with the function x^{2} + 2,1339
the values farthest from c = 3 will produce the values farthest from l = 11, because 3^{2} + 2 = 11."1343
"Thus, we only have to concern ourselves with x = 3 - δ and x = 3 + δ.1352
"If that didn't quite make sense, Watson, what we have here is that, at some horizontal location 3,1356
we know that it puts out the vertical height of 11."1362
"So, as we get farther and farther to either side, we will end up getting farther and farther to 11."1365
"We know that this is a parabola; we are used to working with parabolas; so we see that, the farther we end up getting away from c = 3,1371
the more extreme we are from c = 3, the more extreme we will be from our l = 11."1378
"That is how 3^{2} + 2 would work; as long as we don't go so incredibly far1384
that we end up wrapping the parabola to the other side, we are safe from this; we don't have to worry about it."1388
"So, as long as we can be absolutely sure of that fact, where we don't to -3 or go past 0, we will be fine."1393
"And we know that δ must be less than or equal to .1, because of our earlier restriction on it always being less than or equal to .1."1400
"So, we know that we can't get too far; the most extreme values for our x will end up being using the whole of δ--1407
that is, we only have to concern ourselves with x = 3 - δ and x = 3 + δ."1414
"Now, I want to point out, before we continue, that this logic is specific to the function we are working with, Watson."1420
"It is specific to working with x^{2} + 2, the fact that, as we get farther and farther away horizontally,1425
we will get farther and farther away vertically, as well; so looking at maximum horizontal distance means maximum vertical distance."1431
"A different function, though, might require different logic; so we have to think specifically1438
about the function that we are working with, if we are going to prove something."1442
"In this case, though, we see that this method will work."1445
"Thus, we can show that our δ = ε/10 works by showing that, if we use the above x1448
(that is x = 3 - δ and x = 3 + δ--if they both work) in our function,1454
for being within ε of l, if we have that they end up coming out like that,1460
we know without a doubt that our δ will always work, because it worked for the most extreme possible values."1467
"We must show that the absolute value of 11 minus f(x)...in this case, if we are plugging in 3 - δ,1474
and our f(x) is x^{2} + 2, we would have the absolute value of 11, our l, minus...1481
plugging in our function's maximum, most extreme possible value for x, that is (3 - δ)^{2} + 2 must be less than ε."1486
"Similarly, over here, for our other extreme value for x, x = 3 + δ,1495
if we plug in our f(x), we have the l that we are going to (11) minus the quantity (3 + δ)^{2} + 2, is less than ε."1501
"Those are the most extreme values there; we are doing the absolute value of l minus f(x) must be less than ε."1511
"That is what we want to show; so to show that this is the case, we will investigate the left sides of the expressions."1519
"Let's work with the 3 - δ part first; we have |11 - (3 - δ)^{2} + 2|."1524
"Let's begin by expanding 3 minus δ squared; we expand 3 minus δ squared, and now,1531
we have the absolute value of 11 minus (9 - 6δ + δ^{2}); 3 - δ, squared, gets us 9 - 6δ + δ^{2}."1535
"We have minus here, and we have 9 and 2 inside; so minus 9, minus 2, cancels out the 11."1544
"We are left with -6δ + δ^{2}, but there is still this minus sign, so it distributes on,1551
canceling that and making this negative; and we have the absolute value of 6δ minus δ^{2}, when we plug in x = 3 - δ."1560
"Over here, on the other one, we have |11 - (3 + δ)^{2} + 2|."1569
"We expand 3 + δ, squared; we get 9 + 6δ + δ^{2};1576
so now we have |11 - (9 + 6δ + δ^{2}) + 2|; once again, we are subtracting by what is inside of that."1581
"So, the 9 and the 2 go together to combine and take out the 11, leaving us with 6δ + δ^{2}."1588
"The minus sign distributes, and we now have -6δ - δ^{2} if we had plugged in x = 3 + δ."1593
"So, that is what the distance between l and our f(x) is when we plug in our most extreme possible x's, 3 - δ and 3 + δ."1602
"Continuing from this, we can see that, since 0 is less than δ, which is less than or equal to 0.1--1611
remember: we set that δ must be less than or equal to 0.1 at the beginning,1616
because the largest ε that we were allowed to really care about was ε = 1,1619
and we know that δ = 0.1 works there, so we always kept our δ's smaller than 0.1, and δ must be greater than 0."1624
"We can write the above as 6δ - δ^{2} and 6δ + δ^{2}."1631
"If you are not quite sure about this, since 6δ...well, we know that δ must be greater than 0;1636
thus, 6δ must be positive, and minus δ^{2}...well, δ^{2} must be smaller than δ,1641
because δ is less than or equal to .1; if we square something that is smaller than 1,1648
it must end up being smaller than had it not been squared."1655
"So, 6δ - δ^{2}...well, 6δ is positive; minus δ^{2} is negative, but smaller than 6δ."1659
"So, when we take the absolute value of this expression, we are left simply with 6δ - δ^{2}, even after the absolute value."1666
"Over here, we have -6δ - δ^{2}; well, that means the -6δ and the -δ^{2} are both negative."1673
"So, they combine forces and, after the absolute value is finished with them, they will end up coming out as positive, so we will have 6δ + δ^{2}."1679
"From this, we can create the following inequalities, the right side, in this case,1687
being because δ < 0.1 implies that δ^{2} < δ, which we talked about very recently."1690
"If we have 6δ - δ^{2}, well, if we had 7 - 5, that would clearly be less than simply 7, if we got rid of the thing subtracting from it."1696
"So, we just get rid of the thing subtracting from it, and we have 6δ - δ^{2} < 6δ."1706
"That is certainly true; furthermore, since δ^{2} is less than δ,1712
we have that 6δ + δ^{2} < 6δ + δ, which is the same thing as 7δ."1716
"So, we now know that 6δ + δ^{2} is less than 7δ."1723
"At this point, we can use our δ = ε/10 that we originally set; and we have 6δ = 6ε/10."1727
"Remember: that is less than the most extreme value; and 6ε/10 is clearly less than ε."1736
"Furthermore, the other most extreme value was going to be less than 7δ, and we have 7ε/10,1741
which is indeed less than ε; thus, we have shown that plugging in our most extreme values1746
will show that the distance between f(x) and l is always less than ε."1751
"We plug in our most extreme possible value; that gives us our most extreme possible vertical distance,1756
and it still ends up being less than ε when we work the whole thing through."1761
"So, the method of choosing δ always works; we see that this δ = ε/10 will always work; it will never fail."1765
"Very good, Holmes; my only question is how you decided on setting δ equal to ε/10 in the first place."1774
"How did you think, 'ε/10; that is the thing for me'?"1782
"Indeed, that is the most difficult part of proving a limit."1785
"In general, once you have a sense of how the function works, it helps to set it up as if you knew what δ was."1789
"As you work forward, you will find its requirements."1797
"For example, with this limit, I realized that whatever δ was, whatever I ended up choosing for δ,1800
it would end up having to get to the point where we would see that 6δ + δ^{2} had to be less than ε."1805
"So, if 6δ + δ^{2} had to be less than ε, I could restrict δ < 0.1,1812
because a smaller δ will never cause any harm, and see that 6δ + δ^{2}1817
would be the same thing as saying that it is less than 7δ; and 7δ would certainly work if δ was ε/10."1823
"I could have gone with ε/7, but I figured, 'Why not have a little bit of extra room?'"1830
"And ε divided by 10 just seems so nice and round;1834
so I saw that δ = ε/10 would do fine, at which point I was prepared to work through the proof."1836
"Ah, I am feeling a mite peckish; nothing like a good proof to develop the appetite--what are you in the mood for, Watson?"1842
"Somehow, I find myself craving Greek." "Excellent--good! A brace of gyros it will be!"1848
And they make their exit for the neighborhood gyro shop.1854
All right, with Sherlock Holmes and Watson having helped us see what is going on here,1857
the idea of an ε challenge and a δ defense, and how to prove this stuff in general,1860
by showing that this δ method will always give us a δ that works, we are ready to start working through some examples.1864
Our first example: Below is the graph of f(x) = xsin(1/x).1870
First, we need to determine if the function has a limit, as x goes to 0, and if so, find it and prove it.1876
We can see, right from the beginning, that it looks like it is going to 0.1883
We can see from this nice, convenient graph that it looks like it is going to end up having a limit.1887
It would appear to be the case; however, we notice that we can't simply plug in x = 0.1893
If we did that, we would have 0sin(1/0); we are dividing by 0, so f(0) does not exist.1900
We can't simply go down that method; we can't simply plug in a number and figure out what is going to come out.1910
So, we have to show this by proving it directly; we have to go and see that this is going to always work.1915
We have to figure out a way; so we can see from the graph that, yes, it makes sense that it is going to end up coming out to be 0.1921
But it will be our job to now prove it through a good proof.1926
Let's try to get an understanding of why this thing looks like this.1931
We can see, from the graph, that it looks like this; but let's see what is going on.1934
What we can do is break this down into multiple pieces.1937
We can first see this as sine of...well, let's look, actually, first, at 1/x; what does 1/x graph as?1940
Well, 1/x is going to end up graphing something like this; we are going to go asymptotic as we approach that vertical axis.1951
Then, how does sine of some value graph?1960
Well, sine of some value ends up graphing like this; it has that nice repeating nature.1965
If you watched the last lesson, you probably ended up seeing this in the previous lesson.1975
We talked about just sin(1/x), and how it went crazy and came really, really close.1979
That is the same idea so far; we have that part going on so far.1983
If we plug these two things in--if we plug 1/x in for sine of t, then what we are concerned with,1987
as we get close to 0, as x goes to 0, is that part that is getting close to that.1992
If we end up looking at that, if we look at sin(1/x), we are going to end up getting this part where,1998
as it is far away from 0, it is going to end up going sort of slowly.2008
But as it gets closer, it is going to speed up, and it is going to start to go crazy.2011
And it is going to bounce back and forth between 1 and -1 really, really fast, because it has to go through all of infinity.2015
We shoot off to infinity as we get towards 0; so since it is shooting off towards infinity, 1/x is shooting off towards infinity inside of the sine.2021
So, the sine is now going to have to speed up faster and faster and faster, because it has to go through all of infinity by the time it makes it to 0.2029
We see the same thing from both sides: it shoots up and gets really, really, really, really fast, bouncing up and down.2035
And so, that is the behavior we see.2040
If it was simply sin(1/x), it wouldn't have a limit, as we talked about in the previous lesson,2041
because it is never going to agree on a single location that it is working towards.2046
However, in this case, we also have x showing up; well, if we graph just x, what does just x look like?2051
Well, that looks just like this; so x times something is going to end up expanding it or shrinking it by whatever x's current value is.2059
As x gets closer and closer to 0, it is going to end up squishing it and squishing it and squishing it, closer and closer to that x-axis.2070
Now, notice: sine of anything always produces values that are going to be between -1 and +1,2076
based on how the unit circle works and what we can see from the graph of just sine.2089
So, what we are going to have is either a positive x, effectively, or a negative x.2095
So, if we graph in that -x...here is -x in green...then as we plug in x times sin(1/x), it is going to get...2099
the maximum value that they can have is whatever the x is that it is next to.2114
So, as it gets far away, it ends up bouncing between these things.2117
But as it gets closer and closer and closer, it ends up bouncing faster and faster and faster and faster.2120
But because there is that x, it shrinks it down and crushes it to go down to 0.2125
So, it is not actually going to be defined at x = 0; but it will end up being crushed into this point right here.2130
So, with all of these ideas in mind, we can now say that the limit as x goes to 0 of x times sin(1/x) equals 0.2137
We figured out that, yes, it does have a limit; it makes sense; we understand what is going on2150
in a thing that now makes sense with this graph.2155
And notice: you can also see that the x is going out like this in the graph.2157
And then, -x goes out here; so this nice, computer-generated graph--we end up seeing the same behavior2165
of the sine bouncing infinitely quickly...it gets trapped between +x and -x, because it has to multiply x times sin(1/x).2172
So now, we see that this is what our limit ends up being.2181
And at this point, we can try to work out a proof here.2184
So, if we are going to prove that this is the case, then it must be that, for any ε greater than 0,2187
there exists some δ that will end up making us within that appropriate distance of our vertical ε.2195
For any ε greater than 0, what δ do we choose--what is the appropriate method?2204
Well, notice: if we go back to our x (here is a graph of x, once again; and I will also map the -x here, as well...2208
sorry; that should be dots all the way through); if we have -x and x mapped here, well, what is the biggest thing that x allows?2221
Well, the biggest thing that x is going to allow that sine to get expanded out to is whatever x currently is.2229
For any ε greater than 0, if we want to talk about the maximum vertical size we can allow,2235
then we can allow x to go out as far as that ε, and that will be the maximum allowed vertical size.2238
So, we can simply say that our δ (since that is how far out our x can go from 0) is simply equal to ε.2244
We set δ = ε now, it is going to be our job...what we want to show now is that,2251
for any f(x) - l, it is going to be less than ε if we have our x within δ distance of our c.2260
All right, so let's start working through this.2276
We can swap out what f is and what l is, and we can swap things out, and we can start working and showing that this is true.2277
f(x) - l...what is the left side there? f(x) is this thing right here, x times sin(1/x), minus l...2286
well, l is just 0 in this case, so minus 0...it just closes up, and we have that it is less than ε.2297
So, at this point, we can look at this and say, "Well, x times sin(1/x)...the absolute value of all of that2304
is just going to be the same thing as the absolute value of x, times the absolute value of sin(1/x)."2308
If we strip any possible negative signs after they have multiplied,2313
or strip any possible negative signs before they multiply, it is not going to have an effect on the product.2316
So, we have that this thing right here...2320
Oh, we don't know that it is less than ε; what we want to show is that it comes out to be less than ε.2321
We want to work towards showing that; I'm sorry about that.2326
The absolute value of xsin(1/x) is just the same thing as |x| times |sin(1/x)|.2328
Well, what is the absolute value of sin(1/x)?2338
Well, the absolute value of sin(1/x)...the absolute value of sine of anything at all is going to be less than or equal to 1.2341
You can't get larger than 1 or larger than -1 when you plug something into sine.2355
The absolute value of sin(1/x) is going to still be less than or equal to 1,2360
except for that specific value of x = 0, which would cause the whole thing to break.2365
But we don't have to worry about that, because it is x going to 0; so we have 0 < x - c.2369
So, we don't have to worry about x = 0; so we know that sin(1/x) ≤ 1 will always be true,2375
because we don't have to worry about actually plugging in x = 0.2380
So, we can now use this information up here; and we have that |x| times |sin(1/x)| is less than or equal to...2383
we swap out that fact that sin(1/x) is less than or equal to 1, and we have |x| times 1.2391
So, |x| times |sin(1/x)| is less than or equal to |x| times simply 1.2397
We have that that is just the same thing as saying x; great.2403
Now, at this point, we also know that x - c is less than δ.2407
Let's use yet another color here; so...well, what is our c?2412
Our c is equal to 0 in this case, because that is what we are going towards.2416
So, we have that the absolute value of x - 0...well, we will just leave it as the absolute value of x...has to be less than δ.2420
The absolute value of x is less than δ; we can now swap that in here.2427
And we have that the absolute value of x is less than δ.2431
What did we set our δ to? We know that δ is equal to ε, because that is what we decided to make our method.2437
We have that that is equal to ε; so at this point, we have now shown that the absolute value of x,2442
times the sine of 1/x, gets to being less than or equal to x, which we know is less than δ, which...2450
δ is equal to ε, but at this point we can stack together our signs.2459
The most extreme sign that we ended up having was that direct strictly less than;2462
so at this point, we now see that the absolute value of x times sin(1/x) is, indeed (close that absolute value), less than ε.2466
So, that always ends up being true, if we use this method.2478
We have now completed our proof; this limit does, indeed, work out.2481
We have shown that whatever ε we end up choosing, there will always be an appropriate δ,2485
if we simply set δ = ε it will end up satisfying any and every ε.2490
Thus, we have completed the proof; the limit does exist; the limit is, indeed, 0.2496
Awesome; all right, the second example (and there are only going to be two of these examples,2500
total, because they clearly take a little while to get through):2503
consider the piecewise function f(x) = 1 when x is rational, -1 when x is irrational.2506
Prove that f(x) has no limit anywhere.2512
The very first thing we want to do here, before we try to prove anything, is understand just what f(x) = 1 when x is rational, -1 when x is irrational, means.2515
First, we need to remember what it means for a number to be rational.2524
A number is rational when it can be put as some a/b, where a and b are integers; that is what it means for a number to be rational.2528
A number is irrational when it can't be expressed as a rational.2540
A rational means any decimal number that has a fixed length to it, and also decimals that end up having repeating patterns.2544
But it will actually be enough, with just a fixed length, to understand what is going on here.2551
2.000000001, stop, is a rational number.2555
An irrational number is a decimal number, or something that can be expressed as a decimal number,2562
where the decimals continue going on forever; they never establish a single pattern,2566
and they just constantly are changing forever and ever and ever.2570
For example, π is 3.1415...stuff going on forever; √2, e...we have seen some irrational numbers that are pretty important.2572
But they are also everywhere total; imagine...we had that rational at 2.000000001,2584
but we could also have an irrational that is right next to it, practically, at 2.000000001...2590
and then a random string forever and ever, like 158234671111583...it just keeps changing and changing and changing.2595
So, we can have an irrational number right next to any rational number.2608
We can get as close as we want to any rational number.2612
And we can get as close as we want to any irrational with a rational, by just putting as many decimals as we want, and then stopping at a certain point.2615
So, the rationals and the irrationals are right next to each other, everywhere total.2621
Every single place on the number line has a rational and then an irrational, effectively, infinitely close to it;2627
and then, a rational right next to that and an irrational right next to that...everything is just infinitely mashed together.2632
2 isn't both a rational and an irrational; 2 is simply rational.2638
But right next to it is an irrational; you can get as close to it as you want, with 2.0000000...random pattern.2642
And then, you can get as close as you want to 2.000000...random pattern with a rational, like 2.0000000000000, stop.2648
In matching the random pattern 2.00000000....match the first 50 thousand digits of the random pattern,2658
and then stop, and that is still going to be a rational number, because it is technically an integer divided by an integer.2664
It will be a large integer divided by a large power of 10, but it is still technically an integer over an integer, so it is going to be a rational number.2668
What that means is that rationals and irrationals are right next to each other everywhere.2676
If we tried to graph this, what would f(x) end up looking like?2682
Well, we would end up having some that looked like this, where, let's say, we use blue when one x is rational;2685
so we are going to end up having...everything that ends up being a rational will come out at 1.2693
There are always going to be points, but between any point and the next point over,2700
it is going to end up having a little, tiny hole for the irrationals.2703
And where do the irrationals show up? Well, they show up at -1.2707
So, we end up having the same thing here; down below them are our irrationals.2709
And so, there are a bunch of irrationals; there are infinitely many irrationals down there; there are infinitely many rationals up here.2714
And they both are just right next to each other.2720
You are constantly jumping back and forth and back and forth and back and forth and back and forth, if we were to try to plot this thing out.2722
It is certainly not continuous, because it is two things simultaneously.2728
So, why can't we have a limit? Now let's try to think about why there will be no limit anywhere.2731
Well, consider: if we tried to talk about some location c, then that means that that location c would have to be in either the top or the bottom.2737
And if it ended up being in either the top or the bottom--let's just say the top for argument's sake--2746
then that means that we can put some ε boundary that is small enough to contain just one of these.2750
We make ε equal to a half or something, so that it can just contain one of these height strings, one of these lines.2757
So, since it can only contain one of these lines, no matter what δ we end up choosing,2765
if we choose any δ, then we are going to end up having points that are both on the bottom and on the top.2770
So, if we were in the top, we can make ε only contain the top;2779
but whatever δ size we choose, since the rationals and the irrationals are right next to each other,2783
if we have some rationals, we have to have some irrationals with it, as well.2787
If we have some irrationals, we have to have some rationals with it, as well.2791
If you catch this stuff, it has both types, no matter what, if you take any interval chunk of it.2794
So, since δ will always produce some interval chunk, it has to have both rationals and irrationals in that interval chunk.2800
We grab a chunk, and it is going to have both the top and the bottom,2806
even though we have restricted our ε to only contain either the top or the bottom.2810
And this is the idea of why there can be no limit anywhere: because we can always choose an ε2814
that is going to only take either the top or the bottom line, but no matter what δ we end up choosing,2820
we are going to have to be in both the top and the bottom lines.2825
So, we won't be stuck just inside of that ε it will fail to end up having a limit.2827
If we are going to actually prove this formally, that will be a little bit difficult.2835
But understanding the idea is 90% of the battle.2839
I would much prefer that you understand this idea, and the proof doesn't make sense,2841
than that you really, really work hard through the proof and have a vague understanding of doing the proof,2846
but you don't understand the idea of the limit.2849
At this point (and probably ever), the most important thing, by far, is understanding the general idea,2851
and having a sense of what is going on, rather than being able to do the specific mechanics.2858
The specific mechanics can always come later; understanding the idea is the goal.2862
All right, but let's work through those specific mechanics.2865
OK, proof by contradiction; how do we show this?2868
We will show by assuming it is possible; and then we will see that, if we were to assume that it is possible, crazily impossible things will occur--2871
that if this were true, that we did have a limit, then it won't work--it just doesn't make any sense.2879
And so, we will have contradicted it, and we will know that it must be the case that the limit cannot exist.2885
So, what we do is begin by assuming (there will be a lot of writing for this; I'm sorry)2890
that there exists some limit that as x goes to c; our f(x) is equal to some value of l.2900
Then, for any ε greater than 0, by the definition of how a limit works,2909
we know that there exists some δ greater than 0 such that...2917
and from here on, when I write "such that," I will probably just use s.t. if I have to write that again...2925
such that, for any 0 < |x - c| < δ--that is to say, an x that is less than δ distance2930
away from whatever our c happens to be--we know that it must be the case that the absolute value of f(x) - l,2943
that is, the distance between the f(x) that gets mapped from that x and l, what our limit goes to--has to be less than ε.2951
So, that has to be true; that is what it means for it to have a limit.2959
If there exists a limit, then it must be that for any ε greater than 0, there will always exist a δ greater than 0,2964
such that if x is within δ of c, f(x) must be within ε of l; that is what the formal definition is.2969
Now, let us consider (let me actually change colors, because now we are changing ideas)...2978
that was the setup to this thing: the next thing is: Consider ε = 1/2.2984
Therefore, there must exist, by this thing up here (for any ε greater than 0, there exists a δ greater than 0)...2995
there exists a δ greater than 0 such that it does this thing here.3003
There exists δ greater than 0, such that it follows this idea right here.3010
OK, now, let's continue to talk about this ε equal to 1/2.3016
Notice: by the absolute value of f(x) - l being less than ε, being less than 1/2, it must be either...3022
well, what are the possible values that can come out of f(x)? 1 and -1.3042
It must be either |1 - l| < 1/2, or |-1 - l| < 1/2.3047
The distance that our f(x) is from l must be less than 1/2; so either 1 - l is less than 1/2, or -1 - l is less than 1/2.3058
That is what |f(x) - l| < 1/2 has to come out meaning.3066
But also notice: only one of these can be true.3071
These two ideas right here, |1 - l| < 1/2 and |-1 - l| < 1/2, can't both be true,3085
because if our l is within 1/2 of -1, it can't possibly also reach to being 1/2 of 1.3094
And if our l is within 1/2 of 1, it can't possibly also be within 1/2 of -1.3101
It has to pick one of the two bands; our l can't be 1/2 away from both bands, because 1 and -1 are two apart.3107
If you are within one of them, you can't be near both of them; so it can't be near both of them.3115
Only one of these can be true; we are going to use that fact very soon.3123
Now, we go on to say, "Well, there existed some δ greater than 0 such that it made 0 < |x - c| < δ, which means that |f(x) - l| < ε."3129
So, by our δ, we know that 0 is less than x - c, which is less than δ,3141
and that that ends up having to mean that the absolute value of f(x) - l has to be less than our 1/2, this thing right here.3155
We know that our δ has to end up making our f(x) within 1/2 of l, since we set our ε as 1/2.3166
But 0 < |x - c| < δ--that is to say, x is within δ of c--must contain rational and irrational x.3173
Since we know that δ has to be greater than 0, and our x is within δ of c--3200
it is within some interval of c - δ to c + δ--well, any interval...remember: rationals and irrationals are right on top of each other;3205
then that means our interval, this interval here, the one set up by 0 < |x - c| < δ, must contain both rational and irrational x-values.3224
If it contains both rational and irrational x-values, we know, because it has to be true for any x in this interval,3235
and since we contain both rational and irrational, we now have 1 and -1 popping out of our f(x).3246
Thus, the absolute value of 1 - l is less than 1/2, and the absolute value of -1 - l is less than 1/2 must be true simultaneously,3252
because we know that, within our δ bound, we are going to have both rationals and irrationals.3269
And anything within that δ bound, by the definition (for any ε greater than 0,3275
there exists δ greater than 0, such that, if you are contained within that boundary of δ,3279
it must map within that boundary of ε) that we are contained within that boundary of δ;3284
we are contained within c - δ to c + δ; but there are going to be rationals and irrationals in there.3289
So, that means that our ε boundary must contain both 1 and -1.3293
So, the absolute value of 1 - δ must be less than 1/2, and the absolute of -1 - δ must be less than 1/2.3299
But only one can be true; this and this are mutually exclusive, because you can't be in both bands at once,3304
if the band can only be a total distance of 1 wide around positive 1 or around -1.3312
1/2 down and 1/2 up don't manage to reach each other; they can't reach across, so you can't end up being in both bands at once with that ε of 1/2.3317
So, it says that they must be true simultaneously; but we know that only one can be true.3326
Since only one can be true, and we know that they have to be true simultaneously, those are impossible statements to be true at the same time.3330
We have a contradiction; there is a contradiction in our logic.3336
And because we know everything else in our logic was flawless, except for our assumption that there existed some limit,3340
we know, therefore, that no δ can exist that will satisfy ε equal to 1/2; so no limit can exist.3347
And we have completed our proof.3365
All right, I think that is really cool; it is not for everyone, but I think it is so beautiful.3367
So, I hope you enjoyed it; I hope you get a cool sense of this.3372
And remember: what we talked about here is not something that is necessary for virtually any students--3374
certainly no student currently at a precalculus level.3381
If you are just in the level of this course, you don't need to know this stuff.3383
I am honest; I won't have to use this stuff at all.3386
It is going to maybe, maybe, maybe end up showing up when you take calculus, but probably not even then.3389
It is really something that you only need if you are getting into advanced math.3395
However, I think that this stuff is so cool; and there is no reason that, if you end up liking this stuff...3398
it is like going and checking out art for me; if you end up liking this stuff, you might as well check it out any time that you are able to enjoy it.3402
It is really cool stuff; it gets your brain thinking in all of these totally new ways.3409
And you can end up exploring this stuff for years and years and years.3413
You can make an entire career out of exploring this stuff.3416
If you think this is kind of cool, you can study mathematics in college, go on to become a mathematician, and just study math for the rest of your life.3418
There is a whole bunch of other stuff to explore; math is really, really cool.3425
All right, see you at Educator.com later--goodbye!3428
1 answer
Last reply by: Professor Selhorst-Jones
Mon Aug 3, 2015 5:54 PM
Post by Mike Petersen on July 3, 2015
Would this be considered the "squeeze theorem"?
1 answer
Last reply by: Professor Selhorst-Jones
Mon Jul 21, 2014 8:29 PM
Post by Teemu S on July 20, 2014
What an awesome lecture! I know I'm going have to deal with this definition in a couple of months and this has cleared it up for me.
I really appreciate all the lectures you've given. You are by far the most motivating and inspiring math teacher I've come across. A big thank you from Finland!
2 answers
Last reply by: Jamal Tischler
Sun Mar 1, 2015 7:09 AM
Post by Jason Todd on July 27, 2013
Awesome Video!!! It grabbed my intuition and slammed it into synchrony with this concept. Thank you! The dialogue made things really enjoyable.
P.S. f(x)= x sin(1/x) is my new favorite function! Do you have a list of really cool functions like this?