AP Syllabus focus: 'The longest standing-wave wavelength is the fundamental or first harmonic. Higher harmonics have shorter wavelengths; systems with one node and one antinode allow only odd harmonics.'
Standing waves occur only at specific resonant patterns. This means a system does not support every possible frequency, but instead a limited set called harmonics, built from the fundamental frequency.
Fundamental frequency and the first harmonic
When a wave is confined to a region and reflects back and forth, only certain patterns fit the boundary conditions. Those allowed patterns are the basis of harmonic behavior.
Harmonic: An allowed standing-wave mode of a system, with a specific pattern, wavelength, and frequency.
The harmonics are labeled by a harmonic number, usually written as . The lowest allowed mode is especially important because every other allowed mode is compared to it.
Fundamental frequency: The lowest resonant frequency of a standing-wave system; it is also called the first harmonic.
The first harmonic has the longest wavelength that can fit in the system while still satisfying the boundaries. It is the simplest standing-wave pattern, with the fewest segments between boundaries. Because the wave speed in a given medium is fixed by the system, the longest allowed wavelength corresponds to the lowest allowed frequency.
This is why the fundamental frequency is often described as the system’s base resonant frequency. Any higher harmonic must fit more wave structure into the same length, so it must have a shorter wavelength and therefore a higher frequency.
Higher harmonics
A higher harmonic is any allowed mode above the first harmonic. These are not arbitrary vibrations. They are exact standing-wave patterns that match the system’s boundaries.
For systems with the same type of boundary condition at both ends, such as two nodes or two antinodes, all integer harmonics are allowed.

Normal-mode diagrams for a string with identical boundary conditions at both ends (e.g., fixed ends) illustrate the first harmonic and higher harmonics as increasingly segmented standing-wave patterns. Each increase in harmonic number adds another half-wavelength into the same length , so decreases while increases. Source
In these systems, the standing wave fits an integer number of half-wavelengths into the length .
= frequency of the th harmonic, in hertz
= wavelength of the th harmonic, in meters
= harmonic number,
= fundamental frequency, in hertz
= length of the standing-wave region, in meters
This relationship shows the core pattern clearly:
The second harmonic has twice the frequency of the fundamental.
The third harmonic has three times the frequency of the fundamental.
As harmonic number increases, the wavelength becomes shorter.
So, if the first harmonic is the longest wavelength, every higher harmonic must be shorter. That matches the AP Physics 2 idea that the fundamental is the longest standing-wave wavelength and that higher harmonics have shorter wavelengths.
A helpful way to think about this is geometric: the system length stays the same, but higher harmonics squeeze in more half-wavelengths. More wave segments in the same distance means a shorter wavelength.
Systems with one node and one antinode
Not all standing-wave systems have matching boundary conditions. Some systems require a node at one end and an antinode at the other. In that case, the allowed standing-wave patterns are more restricted.
Odd harmonics: The allowed harmonics whose harmonic numbers are odd integers, such as .
A system with one node and one antinode allows only odd harmonics.

A closed–open resonator (node at the closed end, antinode at the open end) supports standing waves whose lengths fit odd numbers of quarter-wavelengths. The diagrams show that the next allowed mode after the fundamental is the third harmonic, reinforcing that only satisfy the mixed boundary conditions. Source
The reason is that the length must contain an odd number of quarter-wavelength sections. An even-numbered harmonic would fail to produce the correct boundary type at one end.
For these systems, the allowed wavelengths and frequencies follow a different pattern.
= frequency of an allowed harmonic, in hertz
= wavelength of an allowed harmonic, in meters
= odd harmonic number,
= fundamental frequency, in hertz
= length of the standing-wave region, in meters
This means the allowed sequence is:
first harmonic
third harmonic
fifth harmonic
seventh harmonic
The second harmonic and fourth harmonic do not occur in such a system because they do not satisfy the required one-node, one-antinode arrangement.
Recognizing harmonic patterns
When identifying harmonics, the most important first step is to determine the boundary conditions. Once those are known, the harmonic pattern follows directly.
If both ends are the same type, all integer harmonics can occur:
If one end is a node and the other is an antinode, only odd harmonics can occur:
The fundamental is always the lowest-frequency allowed mode.
The fundamental is also the longest-wavelength standing wave the system can support.
Higher harmonics always correspond to shorter wavelengths and higher frequencies than the first harmonic.
In AP Physics 2, harmonic questions often depend more on recognizing allowed patterns than on heavy calculation, so identifying the boundary type is the key first move.
FAQ
A harmonic is counted from the fundamental, so the fundamental is the first harmonic.
An overtone counts only frequencies above the fundamental:
fundamental = not an overtone
next allowed mode = first overtone
Because of this, the first overtone is not always the second harmonic. In a system with only odd harmonics, the first overtone is the third harmonic.
They can have different relative strengths of their harmonics.
If one system produces a strong third harmonic and another produces a strong fifth harmonic, both may share the same fundamental frequency but still sound different. This difference in harmonic content is a major part of timbre, or tone quality.
So the fundamental sets the base pitch, but the harmonics shape the character of the sound.
A non-allowed frequency does not match a natural standing-wave mode of the system.
As a result:
a strong standing wave usually does not build up
the vibration is less efficient
resonance is weaker than at an allowed harmonic
The system may still move, but it will not form the large, stable standing-wave pattern seen at a resonant harmonic frequency.
Damping usually does not change the allowed harmonic pattern set by the boundaries.
Instead, damping mainly:
reduces amplitude
causes vibrations to die out faster
makes resonances less sharp
So the system still has the same ideal harmonic structure, but some harmonics may become harder to observe clearly because energy is lost more quickly.
Yes. Real systems are often close to the ideal pattern, but not perfectly exact.
Small deviations can happen because of:
stiffness in strings
end effects in air columns
nonuniform materials
energy losses
In ideal AP Physics 2 models, harmonic frequencies are treated as exact multiples of the fundamental when the boundary conditions allow it. In real devices, those values can be slightly shifted.
Practice Questions
A string fixed at both ends has a fundamental frequency of 150 Hz.
State the frequencies of the second and third harmonics.
1 mark for 300 Hz
1 mark for 450 Hz
A standing-wave system has one node at one end and one antinode at the other. Its fundamental frequency is 220 Hz.
(a) State whether the second harmonic is allowed, and explain why.
(b) Write the wavelength of the fundamental in terms of the system length .
(c) Determine the frequencies of the next two allowed harmonics after the fundamental.
(a) 1 mark for stating that the second harmonic is not allowed
(a) 1 mark for explaining that a one-node, one-antinode system allows only odd harmonics
(b) 1 mark for
(c) 1 mark for identifying the third harmonic as 660 Hz
(c) 1 mark for identifying the fifth harmonic as 1100 Hz
