Perhaps this analogous example might help:
We know that any finite sum of the kind
$$p_N(x) = \alpha_0 + \alpha_1 x + \cdots + \alpha_N x^N,$$ where ##\alpha_i## are real constants, is called a polynomial of degree ##N##. If the polynomial is associated with a function ##f(x)##, then
$$f_N(x) = a_0 + a_1 x + \cdots + a_N x^N$$ is called the Taylor polynomial of ##f(x)## of order ##N##, where ##a_i = f^{(i)}(0)/n!## are the usual Taylor series coefficients.
The difference in the text is that ##T_N(x)## is a generic trigonometric polynomial and the Fourier polynomial ##f_N(x)## is a specific trigonometric polynomial where the coefficients are the usual Fourier coefficients from the Fourier series.
It's not obvious that the Fourier polynomial of order ##N## obtained by truncating the Fourier series is the trigonometric polynomial of degree ##N## that best approximates the function ##f(x)## in the least-squares sense. Theorem 8 says it is.