By Unknown
Suppose we want to publish something that is as simple as
\[
1 + 1 = 2
\tag{1}
\]
This is not very impressive. If we want our article to be accepted by IEEE reviewers, we have to be more abstract. So, we could complicate the left-hand side of the expression by using
\[
\ln(e) = 1
\]
and
\[
\sin^2 x + \cos^2 x = 1,
\]
and the right-hand side can be stated as
\[
2 = \sum_{n=1}^{\infty}\frac{1}{2^n}.
\]
Therefore, Equation (1) can be expressed more scientifically as:
\[
\ln(e) + \left(\sin^2 x + \cos^2 x\right)
=
\sum_{n=1}^{\infty}\frac{1}{2^n}.
\tag{2}
\]
which is far more impressive. However, we should not stop here. The expression can be further complicated by using
\[
e = \lim_{z \to \infty}\left(1 + \frac{1}{z}\right)^z
\]
and
\[
1 = \cosh(y)\sqrt{1 - \tanh^2(y)}.
\]
Equation (2) may therefore be written as
\[
\ln\left[
\lim_{z \to \infty}
\left(1 + \frac{1}{z}\right)^z
\right]
+
\left(\sin^2 x + \cos^2 x\right)
=
\sum_{n=0}^{\infty}
\frac{\cosh(y)\sqrt{1 - \tanh^2(y)}}{2^n}.
\tag{3}
\]
Note: Other methods of a similar nature could also be used to enhance our prestige, once we grasp the underlying principles.
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