MHB Limit as x approaches negative infinity.

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The limit as x approaches negative infinity for the function is calculated as $$\lim_{{x}\to{-\infty}}\frac {x} {\sqrt{x^2}} = -1$$ because as x becomes increasingly negative, the expression simplifies to the sign function. The confusion arises from the square root of x squared, which is defined as the absolute value, leading to $$\sqrt{x^2} = |x|$$. For negative values of x, this results in $$|x| = -x$$, confirming that the limit evaluates to -1. Thus, the limit correctly reflects the behavior of the function as x approaches negative infinity.
tmt1
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For this function:

$$\lim_{{x}\to{-\infty}}\frac {x} {\sqrt{x^2}} = -1$$

Why is this correct?

If x is equal to -1, for example, -1 square is 1. And the square root of 1 is 1. So should the answer be 1?
 
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If $x=-1$, then you have:

$$\frac{-1}{1}=-1$$

The expression in the limit is one way to define the sign function:

$$\text{sgn}(x)\equiv\frac{x}{|x|}$$ where $$x\ne0$$

This is equivalent to the piecewise definition:

$$\text{sgn}(x)\equiv\begin{cases}-1, & x<0 \\[3pt] 1, & 0<x \\ \end{cases}$$
 
MarkFL said:
If $x=-1$, then you have:

$$\frac{-1}{1}=-1$$

The expression in the limit is one way to define the sign function:

$$\text{sgn}(x)\equiv\frac{x}{|x|}$$ where $$x\ne0$$

This is equivalent to the piecewise definition:

$$\text{sgn}(x)\equiv\begin{cases}-1, & x<0 \\[3pt] 1, & 0<x \\ \end{cases}$$

so $$\sqrt{ (-x)^2} = x$$?
 
tmt said:
so $$\sqrt{ (-x)^2} = x$$?

No, what we have is:

$$\sqrt{(-x)^2}=\sqrt{x^2}\equiv|x|$$

Recall that:

$$|x|\equiv\begin{cases}-x, & x<0 \\[3pt] x, & 0\le x \\ \end{cases}$$
 
Good morning I have been refreshing my memory about Leibniz differentiation of integrals and found some useful videos from digital-university.org on YouTube. Although the audio quality is poor and the speaker proceeds a bit slowly, the explanations and processes are clear. However, it seems that one video in the Leibniz rule series is missing. While the videos are still present on YouTube, the referring website no longer exists but is preserved on the internet archive...

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