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Types of discontinuities | Limits and continuity | AP Calculus AB | Khan Academy


5m read
·Nov 11, 2024

What we're going to do in this video is talk about the various types of discontinuities that you've probably seen when you took algebra or pre-calculus, but then relate it to our understanding of both two-sided limits and one-sided limits.

So let's first review the classification of discontinuities. So here on the left, you see that this curve looks just like y equals x^2 until we get to x = 3. Instead of it being 3, at this point you have this opening, and instead the function at three is defined at four. But then it keeps going, and it looks just like y equals x^2. This is known as a point or a removable discontinuity, and it’s called that for obvious reasons. You're discontinuous at that point; you might imagine redefining the function at that point so it is continuous. So the discontinuity is removable.

But then how does this relate to our definition of continuity? Well, let's remind ourselves: our definition of continuity states f is continuous at x = c if and only if the limit as x approaches c of f(x) is equal to the actual value of the function when x is equal to c. So why does this one fail? Well, the two-sided limit actually exists. You could find, if we say c in this case is three, the limit as x approaches three of f(x) looks like if you graphically inspect this—and I actually know this is the graph of y equals x^2, except at that discontinuity right over there—this is equal to 9.

But the issue is, the way this graph has been depicted, this is not the same thing as the value of the function. The value of that function f(3), the way it's been graphed, is equal to 4. So this is a situation where this two-sided limit exists, but it's not equal to the value of that function. You might see other circumstances where the function isn't even defined there, so that isn't even there. In either case, you aren't going to meet this criteria for continuity, and so that's how a point or removable discontinuity is discontinuous with regards to our limit definition of continuity.

Now, let's look at this second example. If we looked at our intuitive continuity test, if we were just to try to trace this thing, we see that once we get to x = 2, I have to pick up my pencil to keep tracing it. That's a pretty good sign that we are discontinuous. We see that over here as well. If I'm tracing this function, I got to pick up my pencil; I can't go through that point. If I have to jump down here and then keep going right over there, in either case, I have to pick up my pencil.

So intuitively, it is discontinuous. But this particular type of discontinuity, where I'm making a jump from one point and then I'm making a jump down here to continue, is called a jump discontinuity. This is, of course, a point removable discontinuity. How does this relate to limits? Well, here the left and right-handed limits exist, but they’re not the same thing, so you don't have a two-sided limit.

For example, for this one in particular, but for all the x values up to and including x = 2, this is the graph of y = x^2. For x greater than 2, it's the graph of the square root of x. So in this scenario, if you were to take the limit of f(x) as x approaches 2 from the left, this is going to be equal to 4. You're approaching this value, and that actually is the value of the function.

But if you were to take the limit as x approaches 2 from the right of f(x), what is that going to be equal to? Well, we're approaching from the right, and this is actually the square root of x—so it's approaching the square root of 2. You wouldn't know it's the square root of 2 just by looking at this. I know that just because when I went onto Desmos and defined the function, that's the function that I used. But it’s clear, even visually, that you’re approaching two different values when you approach from the left than when you approach from the right.

So even though the one-sided limits exist, they're not approaching the same thing. Therefore, the two-sided limit doesn't exist, and if the two-sided limit doesn't exist, it for sure cannot be equal to the value of the function there, even if the function is defined. That's why the jump discontinuity is failing this test.

Once again, it's intuitive if you're seeing that, "Hey, I got to jump; I got to pick up my pencil." These two things are not connected to each other. Finally, what you see here is when you learned pre-calculus, often known as an asymptotic discontinuity—asymptotic discontinuity.

Intuitively, you have an asymptote here. It's a vertical asymptote at x = 2. If I were to try to trace the graph from the left, I'd just keep on going. In fact, I would be doing it forever because it's unbounded as I get closer and closer to x equals 2 from the left. If I try to get to x = 2 from the right, once again I get unbounded up. Even if I could—and when I say it's unbounded, it goes to infinity—it's actually impossible, in a mortal's lifespan, to try to trace the whole thing.

But you get the sense that, "Hey, there's no way that I could draw from here to here without picking up my pencil." If you want to relate it to our notion of limits, it's that both the left and right-handed limits are unbounded, so they officially don't exist. If they don't exist, then we can't meet the conditions.

So, if I were to say the limit as x approaches 2 from the left of f(x), we can see that it goes unbounded in the negative direction. You might sometimes see someone write something like this: negative infinity. But that's a little hand-wavy with the math. The more correct way to say it is it's just unbounded.

Likewise, if we thought about the limit as x approaches 2 from the right of f(x), it is now unbounded towards positive infinity. So this, once again, is also unbounded. Because it's unbounded and this limit does not exist, it can't meet these conditions.

So we are going to be discontinuous. This is a point or removable discontinuity, a jump discontinuity—I'm jumping—and then we have these asymptotes: a vertical asymptote. This is an asymptotic discontinuity.

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