Physic Labs

Frontier physics

Modes of a vibrating string

Visualize normal modes of a one-dimensional string and relate harmonic number to mode frequency, illustrating the idea that particle types can correspond to string excitations.

Advanced

Equipment

  • Animated one-dimensional string with a selectable standing-wave mode
  • Controls for harmonic number, tension, and string length

Procedure

  1. Choose a normal mode

    Move the harmonic slider. The string displays nn loops (antinodes) and fixed nodes at both ends.

  2. Change the string properties

    Vary tension or length and observe the normal-mode frequency fn=n2Lτ/μf_n=\frac{n}{2L}\sqrt{\tau/\mu}, with linear density held fixed.

  3. Connect modes and particle states

    Compare harmonics: in a quantized string model, each allowed excitation is a distinct state with characteristic properties. The tabletop string is an analogy, not a full string-theory calculation.

Simulation

Experiment history

In 1968, Gabriele Veneziano introduced an amplitude that described important features of hadron scattering and later became known as the Veneziano amplitude. Its mathematical structure was recognized as naturally connected to an extended, vibrating object rather than pointlike constituents. In 1969, Yoichiro Nambu, Holger Bech Nielsen, and Leonard Susskind independently developed the interpretation of the dual-resonance model as a relativistic string. This marked an early emergence of string theory from attempts to describe strong interactions; later work transformed it into a broader framework for quantum gravity and fundamental physics. The animated classical string here illustrates only the mode-and-state analogy.

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