The Illusion of Discontinuity
Imagine you are standing on a path, and suddenly, the ground beneath you seems to break. That is the feeling many students get when they encounter the greatest integer function, [x].
It is notorious for its jumps, its breaks, and its refusal to be smooth. When you see f(x)=[x]cos(22x−1)π, your intuition might scream, "Discontinuity!"
But in mathematics, as in life, things are not always what they seem. Let us peel back the layers of this function together.
The Trigonometric Transformation
Before we panic about the greatest integer function, let us look at the trigonometric term: cos(22x−1π). This looks a bit messy, so let us distribute the π and the denominator:
Now, recall the property that cos(−θ)=cos(θ). We can flip the terms inside the cosine to get cos(2π−xπ).
Suddenly, the fog clears. We are looking at the complementary angle identity: cos(2π−θ)=sin(θ).
With a stroke of algebraic elegance, our intimidating cosine term collapses into sin(xπ). Our function is now:
The Great Neutralizer
Now, we return to the greatest integer function. We know that [x] is discontinuous at every integer n.
To check for continuity at any integer n, we must verify if the Left Hand Limit (L.H.L.), the Right Hand Limit (R.H.L.), and the function value f(n) are all equal.
Let us look at the L.H.L. as x→n−:
As x approaches n from the left, [x] is n−1. However, the sine term sin(xπ) approaches sin(nπ), which is 0.
Thus, the L.H.L. is (n−1)⋅0=0.
Now, consider the R.H.L. as x→n+:
As x approaches n from the right, [x] is n. Again, the sine term approaches sin(nπ)=0.
The R.H.L. is n⋅0=0.
Finally, the function value at x=n is:
The Conclusion
Look at what happened! The jump in the greatest integer function was completely neutralized by the zero of the sine function.
The L.H.L., the R.H.L., and the function value are all 0. Therefore, the function is continuous at every integer.
Since it is also continuous at every non-integer, we have proven that f(x) is continuous for every real x.
This problem teaches us a vital lesson: never judge a function by its most intimidating part. Sometimes, the solution lies in how the different parts of the function interact.