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The blue curve diverges from the red curve because it represents a finite polynomial (a partial sum) rather than the infinite series. Finite polynomials have a dominant highest-degree term that dictates their end behavior, causing them to shoot off to positive or negative infinity as $x$ grows large, whereas the infinite series converges to the bounded, periodic cosine function.

Conditions: The blue curve is a finite partial sum (e.g., the first four terms).; The red curve is the target function $\cos x$.; $x$ values are sufficiently large (far from the origin).

The blue curve diverges from the red curve because it represents a finite polynomial (a partial sum) rather than the infinite series. Finite polynomials have a dominant highest-degree term that dictates their end behavior, causing them to shoot off to positive or negative infinity as $x$ grows large, whereas the infinite series converges to the bounded, periodic cosine function.

Conditions: The blue curve is a finite partial sum (e.g., the first four terms).; The red curve is the target function $\cos x$.; $x$ values are sufficiently large (far from the origin).

Partial sums approximate the function by truncating the infinite series after a finite number of terms to create a polynomial. As more terms are added, the polynomial matches the target function's graph more closely over a wider interval around the origin.

Conditions: The approximation is evaluated near the center of expansion ($x=0$).; A finite number of terms is selected from the infinite series.

Partial sums approximate the function by truncating the infinite series after a finite number of terms to create a polynomial. As more terms are added, the polynomial matches the target function's graph more closely over a wider interval around the origin.

Conditions: The approximation is evaluated near the center of expansion ($x=0$).; A finite number of terms is selected from the infinite series.

The Maclaurin series for the cosine function is the infinite power series $\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \ldots$, which can be written in summation notation as $\sum_{k=0}^{\infty}\frac{(-1)^k x^{2k}}{(2k)!}$. The video reveals that the specific series-defined function $f(x)$ is exactly equivalent to $\cos x$ for all real numbers.

Conditions: The variable $x$ is a real number.; The series is evaluated at $x=0$ (Maclaurin series).

The Maclaurin series for the cosine function is the infinite power series $\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \ldots$, which can be written in summation notation as $\sum_{k=0}^{\infty}\frac{(-1)^k x^{2k}}{(2k)!}$. The video reveals that the specific series-defined function $f(x)$ is exactly equivalent to $\cos x$ for all real numbers.

Conditions: The variable $x$ is a real number.; The series is evaluated at $x=0$ (Maclaurin series).

Each successive term in the alternating series modifies the polynomial's end behavior and local curvature. The constant term sets the y-intercept, the negative quadratic term pulls the graph downward initially, the positive quartic term forces it back up for larger $x$, and the negative sextic term plunges it downward again, creating oscillations that approximate the cosine wave.

Conditions: The terms are evaluated in the context of the partial sum polynomial.; $x$ is a real variable.

Each successive term in the alternating series modifies the polynomial's end behavior and local curvature. The constant term sets the y-intercept, the negative quadratic term pulls the graph downward initially, the positive quartic term forces it back up for larger $x$, and the negative sextic term plunges it downward again, creating oscillations that approximate the cosine wave.

Conditions: The terms are evaluated in the context of the partial sum polynomial.; $x$ is a real variable.