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In summary: I get it now. So, because u(x+\Delta x) approaches u(x) as Δx approaches zero, the limit of the two expressions (u(x+\Delta x)-u(x)) equals zero. In summary, Mr. Miller is saying that as delta x approaches zero, delta v approaches zero, which is why they are equal.
  • #1
calcstudent1
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0
In the below video from approx. 12:00 onwards while explaining the proof for Quotient Rule, Mr. Miller says that while delta x approaches zero, delta v approaches zero. Can someone explain me why is that?



Thanks a lot!
 
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  • #2
Because ##\Delta v=v(x+\Delta x)-v(x)##, and by definition of "continuous", if v is continuous, then ##v(x+\Delta x)\to v(x)## as ##\Delta x\to 0##. Note that we don't have to assume that v is continuous, since this is implied by the assumption that v is differentiable.
 
  • #3
Thanks for your reply.

I understand that delta v = new v minus old v but the thing I don't understand is "if v is continuous then v(x+Δx)→v(x) as Δx→0." can you explain this statement. I understand that as delta x approaches zero, delta new v is same as old v but what does he bring continuous into picture?
 
  • #4
The question is: Why is "v(x+Δx)→v(x) as Δx→0" valid?
In other words, why is the following correct: [itex]\text{lim}_{x \rightarrow a} v(x + \Delta x) = v(x)[/itex]

For this to be valid you need v(x) to be a continuous function.
A function is continuous if you can pull the limit into the argument:
[itex]\text{lim}_{x \rightarrow a} f(x) = f(\text{lim}_{x\rightarrow a} x)[/itex]

Let's apply this to v(x):
[itex]\text{lim}_{\Delta x \rightarrow 0} v(x + \Delta x) = v(\text{lim}_{\Delta x\rightarrow 0} (x+\Delta x)) = v(x) [/itex],

where [itex]\text{lim}_{\Delta x\rightarrow 0} (x+\Delta x) = x[/itex]
 
  • #5
Edgardo said:
The question is: Why is "v(x+Δx)→v(x) as Δx→0" valid?
In other words, why is the following correct: [itex]\text{lim}_{x \rightarrow a} v(x + \Delta x) = v(x)[/itex]

For this to be valid you need v(x) to be a continuous function.
A function is continuous if you can pull the limit into the argument:
[itex]\text{lim}_{x \rightarrow a} f(x) = f(\text{lim}_{x\rightarrow a} x)[/itex]

Let's apply this to v(x):
[itex]\text{lim}_{\Delta x \rightarrow 0} v(x + \Delta x) = v(\text{lim}_{\Delta x\rightarrow 0} (x+\Delta x)) = v(x) [/itex],

where [itex]\text{lim}_{\Delta x\rightarrow 0} (x+\Delta x) = x[/itex]

wow. this sounds way too complicated for me. i am now feeling that i know so little about limits :(

can you please explain me in simple terms?
 
  • #6
calcstudent1 said:
wow. this sounds way too complicated for me. i am now feeling that i know so little about limits :(

can you please explain me in simple terms?

It might be helpful for you to draw a few continuous curves to convince you that if you look at some point and then go from the left and the right of that point, that as you move closer and closer to the point, that it converges to the point no matter if you approach it from the left or the right.

If something is differentiable then its a lot easier to do this intuitively. If it is not, then you can get potentially some really complicated functions that are harder to deal with.

The intuitiveness can help you understand the actual limit laws because when you need to prove it, you will need to use these laws since you can't rely on drawing nice graphs for general purpose problems.

As a counterexample for seeing where limits don't work, draw a few graphs that are discontinuous and you will see how limits break down for these cases (the left and right hand limits are not equal).
 
  • #7
This topic is not that easy if you want to learn it the rigorous way. So, don't worry too much if you don't get it immediately :smile:.

I'll go a little back. You wrote:
In the below video from approx. 12:00 onwards while explaining the proof for Quotient Rule, Mr. Miller says that while delta x approaches zero, delta v approaches zero. Can someone explain me why is that?

The MIT professor uses the shorthand notation [itex]\Delta u[/itex] and [itex]\Delta v[/itex], where
[itex]\Delta u =u(x+\Delta x) - u(x)[/itex] and
[itex]\Delta v =v(x+\Delta x) - v(x)[/itex]
see 7m35s.

He then let's [itex]\Delta x[/itex] approach zero. Intuitively this means that [itex]u(x+\Delta x)[/itex] will approach [itex]u(x)[/itex]. Hence, [itex]\Delta u[/itex] approaches zero. The same goes for [itex]\Delta v[/itex].

More formally we can write:

[itex]\text{lim}_{\Delta x \rightarrow 0}\Delta u= \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)][/itex] = 0

Read this as: The limit of "u(x+Δx)-u(x)" as Δx approaches zero equals zero.

But I'll ask you this question: Why should [itex]u(x+\Delta x)[/itex] approach [itex]u(x)[/itex]? Or in other words, why is [itex] \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)] = 0[/itex] valid?

This is our goal: We want to show that [itex] \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)][/itex] = 0 (Goal-Equation)

-----

Let's examine the expression [itex] \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)][/itex] carefully. We wish this expression to equal zero.

It turns out that you can turn it into:
[itex]\text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)] = \text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) - \text{lim}_{\Delta x \rightarrow 0} u(x)[/itex] (Limit-Equation)

Do you see what I've done? I have applied the limit to each addend.

Now, let's plug the (Limit-Equation) into the (Goal-Equation):
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) - \text{lim}_{\Delta x \rightarrow 0} u(x)[/itex] = 0

Let's manipulate it further:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) = \text{lim}_{\Delta x \rightarrow 0} u(x) = u(x)[/itex]

(Make sure you understand why the last equal sign is valid)

So the final form is:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) =u(x)[/itex] (Goal-Equation 2)

However, how can you show that Goal-Equation 2 is true?

-------

We will now show that Goal-Equation 2 is true:
We assume that we can pull the limit into the argument of u. What I mean is the following:

Consider the left hand side of Goal-Equation 2: [itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x)[/itex]

Now, let's pull the limit into the argument of u, i.e. we throw the limit between the brackets:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) = u( \text{lim}_{\Delta x \rightarrow 0} [x+\Delta x])[/itex]

Assumption: We are allowed to pull the limit into the argument

Since [itex]\text{lim}_{\Delta x \rightarrow 0} [x+\Delta x] = x[/itex], we can write:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) = u( \text{lim}_{\Delta x \rightarrow 0} [x+\Delta x]) = u(x)[/itex].

Thus, we have arrived at our Goal-Equation 2.
Note however: We have used an assumption. This assumption is also called continuity of a function.

Prof. Francis Su mentions this in his excellent lecture on Real Analysis at 48m07s. This lecture involves rigorous mathematics, i.e. it is very formal and uses proofs.
 
  • #8
calcstudent1 said:
I understand that delta v = new v minus old v but the thing I don't understand is "if v is continuous then v(x+Δx)→v(x) as Δx→0." can you explain this statement. I understand that as delta x approaches zero, delta new v is same as old v but what does he bring continuous into picture?
You have already received a few answers, so I'll just show you an example of what can happen when v isn't continuous. Suppose e.g. that v is the function defined by $$v(x)=
\begin{cases}
1 &\text{if }x=0\\
0 &\text{if }x\neq 0.
\end{cases}$$ This function is continuous at all points in its domain except 0. We have ##v(0)=1##, but ##\lim_{\Delta x\to 0} v(0+\Delta x)=0##.
 
  • #9
Edgardo said:
This topic is not that easy if you want to learn it the rigorous way. So, don't worry too much if you don't get it immediately :smile:.

I'll go a little back. You wrote:


The MIT professor uses the shorthand notation [itex]\Delta u[/itex] and [itex]\Delta v[/itex], where
[itex]\Delta u =u(x+\Delta x) - u(x)[/itex] and
[itex]\Delta v =v(x+\Delta x) - v(x)[/itex]
see 7m35s.

He then let's [itex]\Delta x[/itex] approach zero. Intuitively this means that [itex]u(x+\Delta x)[/itex] will approach [itex]u(x)[/itex]. Hence, [itex]\Delta u[/itex] approaches zero. The same goes for [itex]\Delta v[/itex].

More formally we can write:

[itex]\text{lim}_{\Delta x \rightarrow 0}\Delta u= \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)][/itex] = 0

Read this as: The limit of "u(x+Δx)-u(x)" as Δx approaches zero equals zero.

But I'll ask you this question: Why should [itex]u(x+\Delta x)[/itex] approach [itex]u(x)[/itex]? Or in other words, why is [itex] \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)] = 0[/itex] valid?

This is our goal: We want to show that [itex] \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)][/itex] = 0 (Goal-Equation)

-----

Let's examine the expression [itex] \text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)][/itex] carefully. We wish this expression to equal zero.

It turns out that you can turn it into:
[itex]\text{lim}_{\Delta x \rightarrow 0}[u(x+\Delta x)-u(x)] = \text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) - \text{lim}_{\Delta x \rightarrow 0} u(x)[/itex] (Limit-Equation)

Do you see what I've done? I have applied the limit to each addend.

Now, let's plug the (Limit-Equation) into the (Goal-Equation):
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) - \text{lim}_{\Delta x \rightarrow 0} u(x)[/itex] = 0

Let's manipulate it further:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) = \text{lim}_{\Delta x \rightarrow 0} u(x) = u(x)[/itex]

(Make sure you understand why the last equal sign is valid)

So the final form is:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) =u(x)[/itex] (Goal-Equation 2)

However, how can you show that Goal-Equation 2 is true?

-------

We will now show that Goal-Equation 2 is true:
We assume that we can pull the limit into the argument of u. What I mean is the following:

Consider the left hand side of Goal-Equation 2: [itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x)[/itex]

Now, let's pull the limit into the argument of u, i.e. we throw the limit between the brackets:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) = u( \text{lim}_{\Delta x \rightarrow 0} [x+\Delta x])[/itex]

Assumption: We are allowed to pull the limit into the argument

Since [itex]\text{lim}_{\Delta x \rightarrow 0} [x+\Delta x] = x[/itex], we can write:
[itex]\text{lim}_{\Delta x \rightarrow 0}u(x+\Delta x) = u( \text{lim}_{\Delta x \rightarrow 0} [x+\Delta x]) = u(x)[/itex].

Thus, we have arrived at our Goal-Equation 2.
Note however: We have used an assumption. This assumption is also called continuity of a function.

Prof. Francis Su mentions this in his excellent lecture on Real Analysis at 48m07s. This lecture involves rigorous mathematics, i.e. it is very formal and uses proofs.

+1.

You are awesome. Now, I need to sit and digest this concept. I understand bit and pieces but now I need to put everything together.
 
  • #10
Fredrik said:
You have already received a few answers, so I'll just show you an example of what can happen when v isn't continuous. Suppose e.g. that v is the function defined by $$v(x)=
\begin{cases}
1 &\text{if }x=0\\
0 &\text{if }x\neq 0.
\end{cases}$$ This function is continuous at all points in its domain except 0. We have ##v(0)=1##, but ##\lim_{\Delta x\to 0} v(0+\Delta x)=0##.

+1

Thanks for clarification.
 
  • #11
You guys rock!
 
  • #12
By the way, the quotient rule can also be proved from the product rule, the chain rule and the result that d/dx(1/x)=-1/x2.
$$\left(\frac{f}{g}\right)' =\left(f\frac{1}{g}\right)' =f'\left(\frac{1}{g}\right) +f\left(\frac{1}{g}\right)' =\frac{f'}{g}+f\left(-\frac{1}{g^2}g'\right) =\frac{f'g-fg'}{g^2}$$
 
  • #13
This is a great place to learn mathematics. :)
 

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