Analyzing the Geometry of the V-Shape
Imagine you are standing on a coordinate plane, looking at the graph of f(x)=∣x−1∣. It is a beautiful, sharp V-shape that kisses the x-axis exactly at x=1.
That sharp corner is a warning sign in calculus; it tells us the function is non-differentiable there. However, we are looking for the left-hand derivative, p.
Since we are approaching 1 from the left, we are strictly in the region where x<1. In this territory, the absolute value function behaves like 1−x. The derivative of 1−x is simply −1.
So, our value for p is locked in: p=−1. This is our target.
The Limit Setup
Shifting the Perspective
Now, we face the main challenge:
x→1+limlogcosm(x−1)(x−1)n=−1
Dealing with x approaching 1 is like trying to solve a puzzle while the pieces are moving. Let us freeze the frame by substituting x=1+h.
As
x approaches
1 from the right,
h approaches
0 from the positive side. Our limit transforms into:
h→0+limlogcosmhhn=−1
The Logarithmic and Trigonometric Dance
We have a power
m inside the logarithm. Using the power rule
log(ab)=bloga, we pull the
m out:
h→0+limmlogcoshhn=−1
Now, look at the denominator. We need to evaluate logcosh as h→0. We know the standard limit limt→0tlog(1+t)=1.
Let us rewrite cosh as 1+(cosh−1). By multiplying and dividing by (cosh−1), we force the expression into the standard form. As h→0, the log term effectively becomes (cosh−1).
Our expression simplifies to:
h→0+limm(cosh−1)hn=−1
The Final Power Balance
We know that for small h, 1−cosh≈2h2. Therefore, cosh−1≈−2h2.
Substituting this into our limit, we get:
h→0+limm(−2h2)hn=−1
Rearranging this, we find:
h→0+limm−2⋅hn−2=−1
For this limit to be a finite, non-zero value, the power of h must be zero. If n−2>0, the limit is 0; if n−2<0, the limit is undefined.
Thus, n−2=0, which means n=2.
With
n=2, the
h terms cancel out, leaving us with:
m−2=−1
Solving this gives m=2. We have conquered the problem!