Example of free particles
Storyboard 
Once we have defined the method for counting states and estimating probabilities in situations of interest, we can delve into how a system of many free particles behaves.
ID:(435, 0)
Case Classical Mechanics
Definition 
In classical mechanics, a system is described by the coordinates $q_1, q_2, \ldots, q_f$ and momenta $p_1, p_2, \ldots, p_f$, where $f$ represents the number of degrees of freedom. The state of the system is represented as a point in phase space, given by $(q_1, q_2, \ldos, q_f, p_1, p_2, \ldos, p_f)$.
In the case of a system consisting of $N$ free particles, described using a total of $3N$ coordinates, the number of degrees of freedom is defined as $f = 3N$.
ID:(524, 0)
Case Quantum Mechanics
Image 
In quantum mechanics, the state is described by the wave function $\psi$, which depends on the variables $q_1, q_2, \ldos, q_f$, where $f$ is the number of degrees of freedom of the system.
The wave function is a solution, in the non-relativistic case and for particles without spin, of the Schrödinger equation. Eigenvalues are associated with wave functions, which typically depend on integers. These integers represent possible states of the system that are bounded by the system's energy.
ID:(523, 0)
Calculation of the number of states
Note 
In classical mechanics, a system is described by the coordinates $q_1, q_2, \ldots, q_f$ and momenta $p_1, p_2, \ldots, p_f$, where $f$ represents the number of degrees of freedom. The state of the system is represented as a point in phase space, given by $(q_1, q_2, \ldots, q_f, p_1, p_2, \ldos, p_f)$.
In the case of a system consisting of $N$ free particles, described using a total of $3N$ coordinates, the number of degrees of freedom is defined as $f = 3N$.
ID:(10580, 0)
Example of free particles
Description 
Once we have defined the method for counting states and estimating probabilities in situations of interest, we can delve into how a system of many free particles behaves.
Variables
Calculations
Calculations
Equations
Examples
In classical mechanics, a system is described by the coordinates $q_1, q_2, \ldots, q_f$ and momenta $p_1, p_2, \ldots, p_f$, where $f$ represents the number of degrees of freedom. The state of the system is represented as a point in phase space, given by $(q_1, q_2, \ldos, q_f, p_1, p_2, \ldos, p_f)$.
In the case of a system consisting of $N$ free particles, described using a total of $3N$ coordinates, the number of degrees of freedom is defined as $f = 3N$.
(ID 524)
In quantum mechanics, the state is described by the wave function $\psi$, which depends on the variables $q_1, q_2, \ldos, q_f$, where $f$ is the number of degrees of freedom of the system.
The wave function is a solution, in the non-relativistic case and for particles without spin, of the Schr dinger equation. Eigenvalues are associated with wave functions, which typically depend on integers. These integers represent possible states of the system that are bounded by the system's energy.
(ID 523)
In classical mechanics, a system is described by the coordinates $q_1, q_2, \ldots, q_f$ and momenta $p_1, p_2, \ldots, p_f$, where $f$ represents the number of degrees of freedom. The state of the system is represented as a point in phase space, given by $(q_1, q_2, \ldots, q_f, p_1, p_2, \ldos, p_f)$.
In the case of a system consisting of $N$ free particles, described using a total of $3N$ coordinates, the number of degrees of freedom is defined as $f = 3N$.
(ID 10580)
ID:(435, 0)
