In the displayed Fourier-series setup, a1 is the coefficient for cos(t), which corresponds to the base frequency of 2π1 hertz. a2 is the coefficient for cos(2t), corresponding to π1 hertz.
Conditions: The function is represented in the displayed form with cosine coefficients a1,a2,a3.; The comparison is about the coefficients multiplying cos(t) and cos(2t).
In the displayed Fourier-series setup, a1 is the coefficient for cos(t), which corresponds to the base frequency of 2π1 hertz. a2 is the coefficient for cos(2t), corresponding to π1 hertz.
Conditions: The function is represented in the displayed form with cosine coefficients a1,a2,a3.; The comparison is about the coefficients multiplying cos(t) and cos(2t).
The coefficients a1 and b1 act as weights that tell how much each component is involved in the function. If a1 is much larger than b1, the function has more cosine of t than sine of t.
Conditions: The series is being constructed as a weighted sum of sines and cosines.; The coefficients are real-valued.
The coefficients a1 and b1 act as weights that tell how much each component is involved in the function. If a1 is much larger than b1, the function has more cosine of t than sine of t.
Conditions: The series is being constructed as a weighted sum of sines and cosines.; The coefficients are real-valued.
If the base period is 2π, the term cos(t) has a frequency of 2π1 cycles per second. Doubling the argument to cos(2t) doubles the frequency, so cos(2t) has a frequency of π1 cycles per second.
Conditions: The base period of the function is 2π.; The frequency is defined as the reciprocal of the period.
If the base period is 2π, the term cos(t) has a frequency of 2π1 cycles per second. Doubling the argument to cos(2t) doubles the frequency, so cos(2t) has a frequency of π1 cycles per second.
Conditions: The base period of the function is 2π.; The frequency is defined as the reciprocal of the period.