Research Article | | Peer-Reviewed

The Solution to the Differential Equation with Linear Damping Describing a Physical Systems Governed by a Cubic Energy Potential

Received: 3 December 2025     Accepted: 16 December 2025     Published: 31 December 2025
Views:       Downloads:
Abstract

An analytical solution to the nonlinear differential equation describing the equation of motion of a particle moving in an unforced physical system with linear damping, governed by a cubic potential well, is presented in terms of the Jacobi elliptic functions. In the attractive region of the potential the system becomes an anharmonic damped oscillator, however with asymmetric displacement. An expression for the period of oscillation is derived, which for a nonlinear damped system is time dependent, and in particular it contains a quartic root of an exponentially decaying term in the denominator. Initially the period is longer as compared to that of a linear oscillator, however gradually it decreases to that of a linear damped oscillator. Transforming the undamped nonlinear differential equation into the differential equation describing orbital motion of planets, the perihelion advance of Mercury can be estimated to 42.98 arcseconds/century, close to present day observations of 43.1±0.5 arcseconds/century. Some familiarity with the Jacobi elliptic functions is required, in particular with respect to the differential behavior of these functions, however, they are standard functions of advanced mathematical computer algebra tools. The expression derived for the solution to the nonlinear physical system, and in particular the expression for the period of oscillation, is useful for an accurate evaluation of experiments in introductory and advanced physics labs, but also of interest for specialists working with nonlinear phenomena governed by the cubic potential well.

Published in Applied and Computational Mathematics (Volume 14, Issue 6)
DOI 10.11648/j.acm.20251406.17
Page(s) 367-377
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2025. Published by Science Publishing Group

Keywords

Linear Damping, Cubic Potential Well, Jacobi Elliptic Functions, Period of Oscillation, Asymmetric Oscillations, Perihelion Precession

References
[1] Thomson J M T 1989 Chaotic Phenomena Triggering the Escape from a Potential Well. Proc. R. Soc. Lond. A 421, 195-225
[2] Guckenheimer J and Homes P 1983 Nonlinear oscillations. Dynamical Systems and Bifurcation of Vector Fields. Springer-Verlag, New York
[3] Viswanathan K S 1957 The theory of the anharmonic oscillator. Proc. Indian Acad. of Sciences A 46(3), 201-217
[4] Laane J 1971 One-dimensional potential energy functions in vibrational spectroscopy. Q. Rev. Chem. Soc. 1971(4), 533-552
[5] Virgin L N 1988 On the harmonic response of an oscillator with unsymmetric restoring force. J. Sound Vib. 126(1), 157-166
[6] Apostol B F 2005 On anharmonic oscillators. Rom. J. Phys. 50(7-8) 915-918.
[7] Amore P and Fernandez F M 2005 Exact and approximate expressions for the period of anharmonic oscillators. Eur. J. Phys. 26(4), 589-603
[8] Cveticanin L, Zukovic M, Mester Gy, Biro I and Sarosi J 2016 Oscillators with symmetric and asymmetric quadratic nonlinearity. Acta Mech. 227, 1727-1742
[9] Robinett R W 1997 Average value of position for the anharmonic oscillator: Classical versus quantum results. Am. J. Phys. 65(3), 190-194
[10] Pina E 1992 On the motion of the symmetric Lagrange top. Investigacion Revista Mexicana de Fisica 39(1), 10-31 Corpus ID: 251922865
[11] Lawden D F 1989 Elliptic Functions and Applications. Applied Mathematical Sciences 60 Springer-Verlag New York
[12] Brizard A J 2009 A primer on elliptic functions with application in classical mechanics. Eur. J. Phys. 40(4), 729-751
[13] Y. Friedman and J. M. Steiner 2016 Predicting Mercury's Precession using Simple Relativistic Newtonian Dynamics. EPL (Europhysics Letters) 113(4), 39001
[14] Miller D R, Tam G, Rainey R C T and Ritch R 1986 Investigation of the use of modern ship motion prediction models in identifying ships with a larger than acceptable risk of dynamic capsize. Report prepared by Arctec Canada Ltd. for the Transportation Development Centre of the Canadian Government. Report no. TP7407E.
[15] Joukovskaya L 2009 Dynamics with Infinitely Many Time Derivatives in Friedmann- Robertson-Walker background and Rolling Tachyons. J. High Energy Phys. JHEP02(2009)045
[16] Calcagni G and Nardelli G 2010 Cosmological rolling solution of nonlocal theories. Int. J. Modern Phys. D 19, 329-339
[17] Vernov S Y 2011 Exact solutions for nonlocal nonlinear field equations in cosmology. Theor. and Math. Phys. 166(3), 392-406
[18] Korteweg D J and de Vries G 1895 On the Change of Form of Long Waves Advancing in Rectangular Canal, and on a New Type of Long Stationary Waves. Phil. Mag. 39(240), 422-443
[19] Parkes E J, Duffy B R and Abbott P C 2002 The Jacobi elliptic-function method for finding periodic-wave solutions to nonlinear evolution equations. Phys. Letters A 295, 280-286
[20] He J H 2006 Some asymptotic methods for strongly nonlinear equations Int. J. Mod. Phys. B 20 1141-1199
[21] Whittaker E T and Watson G N 1980 A Course of Modern Analysis 4th edn. (Cambridge: University Press)
[22] Abramowitz M & Stegun I 1980 Handbook of Mathematical Functions 9th edn. (New York: Dover)
[23] Walker P 2003 The analyticity of Jacobian functions with respect to the parameter k. Proc. R. Soc. Lond. A 459, 2569-2574
[24] Johannessen K 2014 An analytical solution to the equation of motion to the damped nonlinear pendulum. Eur. J. Phys. 35 035014
[25] Johannessen K 2015 The Duffing oscillator with damping. Eur. J. Phys. 36 065020
[26] Johannessen K 2017 The Duffing oscillator with damping for a Softening Potential. Int. J. of Appl. and Comp. Math., 3, 3805-3816
[27] Johannessen K 2021 The Exact Solution to the General Relativistic Differential doi describing Planetary Orbits, Int. J. of Appl. and Comp. Math., 7: 79,
Cite This Article
  • APA Style

    Johannessen, K. (2025). The Solution to the Differential Equation with Linear Damping Describing a Physical Systems Governed by a Cubic Energy Potential. Applied and Computational Mathematics, 14(6), 367-377. https://doi.org/10.11648/j.acm.20251406.17

    Copy | Download

    ACS Style

    Johannessen, K. The Solution to the Differential Equation with Linear Damping Describing a Physical Systems Governed by a Cubic Energy Potential. Appl. Comput. Math. 2025, 14(6), 367-377. doi: 10.11648/j.acm.20251406.17

    Copy | Download

    AMA Style

    Johannessen K. The Solution to the Differential Equation with Linear Damping Describing a Physical Systems Governed by a Cubic Energy Potential. Appl Comput Math. 2025;14(6):367-377. doi: 10.11648/j.acm.20251406.17

    Copy | Download

  • @article{10.11648/j.acm.20251406.17,
      author = {Kim Johannessen},
      title = {The Solution to the Differential Equation with Linear Damping Describing a Physical Systems Governed by a Cubic Energy Potential},
      journal = {Applied and Computational Mathematics},
      volume = {14},
      number = {6},
      pages = {367-377},
      doi = {10.11648/j.acm.20251406.17},
      url = {https://doi.org/10.11648/j.acm.20251406.17},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.acm.20251406.17},
      abstract = {An analytical solution to the nonlinear differential equation describing the equation of motion of a particle moving in an unforced physical system with linear damping, governed by a cubic potential well, is presented in terms of the Jacobi elliptic functions. In the attractive region of the potential the system becomes an anharmonic damped oscillator, however with asymmetric displacement. An expression for the period of oscillation is derived, which for a nonlinear damped system is time dependent, and in particular it contains a quartic root of an exponentially decaying term in the denominator. Initially the period is longer as compared to that of a linear oscillator, however gradually it decreases to that of a linear damped oscillator. Transforming the undamped nonlinear differential equation into the differential equation describing orbital motion of planets, the perihelion advance of Mercury can be estimated to 42.98 arcseconds/century, close to present day observations of 43.1±0.5 arcseconds/century. Some familiarity with the Jacobi elliptic functions is required, in particular with respect to the differential behavior of these functions, however, they are standard functions of advanced mathematical computer algebra tools. The expression derived for the solution to the nonlinear physical system, and in particular the expression for the period of oscillation, is useful for an accurate evaluation of experiments in introductory and advanced physics labs, but also of interest for specialists working with nonlinear phenomena governed by the cubic potential well.},
     year = {2025}
    }
    

    Copy | Download

  • TY  - JOUR
    T1  - The Solution to the Differential Equation with Linear Damping Describing a Physical Systems Governed by a Cubic Energy Potential
    AU  - Kim Johannessen
    Y1  - 2025/12/31
    PY  - 2025
    N1  - https://doi.org/10.11648/j.acm.20251406.17
    DO  - 10.11648/j.acm.20251406.17
    T2  - Applied and Computational Mathematics
    JF  - Applied and Computational Mathematics
    JO  - Applied and Computational Mathematics
    SP  - 367
    EP  - 377
    PB  - Science Publishing Group
    SN  - 2328-5613
    UR  - https://doi.org/10.11648/j.acm.20251406.17
    AB  - An analytical solution to the nonlinear differential equation describing the equation of motion of a particle moving in an unforced physical system with linear damping, governed by a cubic potential well, is presented in terms of the Jacobi elliptic functions. In the attractive region of the potential the system becomes an anharmonic damped oscillator, however with asymmetric displacement. An expression for the period of oscillation is derived, which for a nonlinear damped system is time dependent, and in particular it contains a quartic root of an exponentially decaying term in the denominator. Initially the period is longer as compared to that of a linear oscillator, however gradually it decreases to that of a linear damped oscillator. Transforming the undamped nonlinear differential equation into the differential equation describing orbital motion of planets, the perihelion advance of Mercury can be estimated to 42.98 arcseconds/century, close to present day observations of 43.1±0.5 arcseconds/century. Some familiarity with the Jacobi elliptic functions is required, in particular with respect to the differential behavior of these functions, however, they are standard functions of advanced mathematical computer algebra tools. The expression derived for the solution to the nonlinear physical system, and in particular the expression for the period of oscillation, is useful for an accurate evaluation of experiments in introductory and advanced physics labs, but also of interest for specialists working with nonlinear phenomena governed by the cubic potential well.
    VL  - 14
    IS  - 6
    ER  - 

    Copy | Download

Author Information
  • Sections