Fundamental frequency
The fundamental frequency, often referred to simply as the fundamental, is defined as the lowest frequency of a periodic waveform. In music, the fundamental is the musical pitch of a note that is perceived as the lowest partial present. In terms of a superposition of sinusoids, the fundamental frequency is the lowest frequency sinusoidal in the sum of harmonically related frequencies, or the frequency of the difference between adjacent frequencies. In some contexts, the fundamental is usually abbreviated as , indicating the lowest frequency counting from zero. In other contexts, it is more common to abbreviate it as , the  first harmonic. (The second harmonic is then = 2⋅, etc. In this context, the zeroth harmonic would be 0 Hz.) According to Benward's and Saker's "Music: In Theory and Practice": Explanation. All sinusoidal and many non-sinusoidal waveforms repeat exactly over time – they are periodic. The period of a waveform is the smallest value of formula_1 for which the following is true: Where formula_2 is the value of the waveform at formula_3. This means that the waveform's values over any interval of length formula_1 is all that is required to describe the waveform completely (for example, by  the associated Fourier series). Since any multiple of period formula_1 also satisfies this definition, the fundamental period is defined as the smallest period over which the function may be described completely. The fundamental frequency is defined as its reciprocal: When the units of time are seconds, the frequency is in formula_6, also known as Hertz. Fundamental frequency of a pipe. For a pipe of length formula_7 with one end closed and the other end open the wavelength of the fundamental harmonic is formula_8, as indicated by the first two animations. Hence, Therefore, using the relation where formula_9 is the speed  of the wave, the fundamental frequency can be found in terms of the speed of the wave and the length of the pipe: If the ends of the same pipe are now both closed or both opened as in the last two animations, the wavelength of the fundamental harmonic becomes formula_10 . By the same method as above, the fundamental frequency is found to be In music. In music, the fundamental is the musical pitch of a note that is perceived as the lowest partial present. The fundamental may be created by vibration over the full length of a string or  air column, or a higher harmonic chosen by the player. The fundamental is one of the harmonics. A harmonic is any member of the harmonic series, an ideal set of frequencies that are positive integer multiples of a common fundamental frequency. The reason a fundamental is also considered a harmonic is because it is 1 times itself. The fundamental is the frequency at which the entire wave vibrates. Overtones are other sinusoidal components present at frequencies above the fundamental. All of the frequency components that make up the total waveform, including the fundamental and the overtones, are called partials. Together  they form the harmonic series. Overtones which are perfect integer multiples of the fundamental are called harmonics. When an overtone is near to being harmonic, but not exact, it is sometimes called a harmonic partial, although they are often referred to simply as harmonics. Sometimes overtones are created that are not anywhere near a harmonic, and are just called partials or inharmonic overtones. The fundamental frequency is considered the "first harmonic" and the "first partial". The numbering of the partials and harmonics is then usually the same; the second partial is the second harmonic, etc. But if there are inharmonic  partials, the numbering no longer coincides. Overtones are numbered as they appear the fundamental. So strictly speaking, the "first" overtone is the "second" partial (and usually the "second" harmonic). As this can result in confusion, only harmonics are usually referred to by their numbers, and overtones and partials are described by their relationships to those harmonics. Mechanical systems. Consider a spring, fixed at one end and having a mass attached to the other; this would be a single degree of freedom (SDoF) oscillator. Once set into motion, it will oscillate at its natural frequency. For a single degree of freedom  oscillator, a system in which the motion can be described by a single coordinate, the natural frequency depends on two system properties: mass and stiffness; (providing the system is undamped). The natural frequency, or fundamental frequency, , can be found using the following equation: where: To determine the natural frequency, the omega value is divided by 2. Or: where: While doing a modal analysis, the frequency of the 1st mode is the fundamental frequency.