
In this lecture Lagrangian of a mechanical system is written as a function of independent generalized coordinates.
In this lecture Euler-Lagrange equations (or Lagrange equations of second kind) which are derived from the Least Action Principle, are introduced without proof.
In this lecture you will learn how to derive generalized momentum and force, corresponding to a generalized coordinate in classical systems.
In this lecture, you will learn how to apply Lagrangian formalism to the perfectly elastic spring and find its equation of motion.
In this lecture, you will learn how to apply Lagrangian formalism to the simple pendulum and find its equation of motion.
In this lecture, you will learn how to apply Lagrangian formalism to the double pendulum and find its equations of motion.
This lecture is the solution of this problem:
A block of mass m is held motionless on a frictionless plane of mass M and angle of inclination θ. The plane rests on a frictionless horizontal surface. The block is released. Use Lagrangian mechanics to determine the accelerations of both plane and block once the block is released.
In this problem we have a pendulum with an oscillating support and we find the angle of pendulum as a function of time.
In this lecture you will learn how to find conservative forces from Lagrangian.
In this lecture you will learn how to use Lagrange equations of first kind, and find constraint forces.
In this lecture you will learn how to apply Lagrange equations of the first kind to the Atwood machine, and find its constraint force (tension) along with its equation of motion and conservative force.
In this lecture you will learn how to identify the cyclic coordinate in Lagrangian, and find its corresponding momentum (that is conserved).
In this lecture, you will find conserved momentum and energy of the projectile, and from them, its equations of motion.
This is an introductory course in Lagrangian mechanics provided for college students and anyone who is familiar with Newtonian mechanics and calculus.
In this course you will learn how to apply Lagrangian mechanics to the classical systems and find their equations of motion and physical quantities. When applied to the classical systems, Lagrangian mechanics is equivalent to the Newtonian mechanics, but more easier than Newtonian mechanics, especially when you are dealing with more complicated systems.
This course is made of three sections:
Lagrangian Dynamics: this section begins with writing Lagrangian (or Lagrange function) of a system in a generalized coordinates in terms of independent coordinates, by finding constraint functions and number of degrees of freedom of the system. You will learn how to apply Euler-Lagrange equations (Lagrange's equations of the second kind) to the independent coordinates and find the equations of motion of the system. Some example of Lagrangian of classical systems are discussed in this section.
Generalized Forces: This section begins with definition of generalized conservative forces. Then by writing Lagrangian without imposing constraint functions and by applying Lagrange's equations of first kind, you learn how to find constraint forces of a system.
Conservation Laws: in this section you will learn how to find conserved generalized momentum (linear and angular momentum) if there is a cyclic coordinate in Lagrangian (i.e. Lagrangian is not implicit function of a coordinate); and how to find conserved energy of the system if Lagrangian is not a implicit function of time.
Register to this course and enjoy learning Lagrangian mechanics!