ABSTRACT

In this chapter, we will consider mechanical systems whose differential equations of motion can be represented in the form of the Lagrange equations https://www.w3.org/1998/Math/MathML"> d d t ∂ L ∂ q ˙ i - ∂ L ∂ q i = 0 ,   i = 1 , … , n , https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9780429180200/2b4bcca7-ca87-4769-8312-7c2815082e4f/content/eq2376.tif" xmlns:xlink="https://www.w3.org/1999/xlink"/>