Linear transformations of forces introduced in the previous article are used. In the case of nonholonomic systems the Lagrange equations of the first and the second type are constructed. The basic forms for equations of motion in the case of nonholonomic systems are obtained.

Original languageEnglish
Pages (from-to)70-74
Number of pages5
JournalVestnik Sankt-Peterburgskogo Universiteta. Ser 1. Matematika Mekhanika Astronomiya
Issue number4
StatePublished - 2000

    Scopus subject areas

  • Mathematics(all)
  • Physics and Astronomy(all)

ID: 71886731