일 | 월 | 화 | 수 | 목 | 금 | 토 |
---|---|---|---|---|---|---|
1 | 2 | 3 | 4 | 5 | ||
6 | 7 | 8 | 9 | 10 | 11 | 12 |
13 | 14 | 15 | 16 | 17 | 18 | 19 |
20 | 21 | 22 | 23 | 24 | 25 | 26 |
27 | 28 | 29 | 30 | 31 |
Tags
- Paulo Freire
- Theories of Education
- bayesian
- Pen Art
- Noether's thm
- Orbital Dynamics
- Quantum Mechanics
- Dirichlet problem
- induced emf
- Quantum electodynamics
- Conformal Mapping
- Topological Tensor
- spinor QED
- Electromagnetics
- Lagrangian Mechanics
- electromotive force
- pedagogy
- General Relativity
- Hamiltonian Mechanics
- Classical Mechanics
- RG flow
- scalar QED
- Quantum Field Theory
- higher derivatives
- Rigid Body Dynamics
- 프레이리
- Covariant derivatives
- Taylor expansion
- Tensor Calculus
- Complex analysis
Archives
- Today
- Total
목록Rigid Body Dynamics (1)
Physvillain

이 글은 2020.10.14에 작성됨. This post was written on Oct 14, 2020. In the rigid body system, all particles consistituting rigid body satisfy $\vec{v}=\vec{w} \times \vec{r}$. It is an example of holomonic constraints. In arbitrary dimension, angular momentum is defined as the form of 2-vector : $$\vec{\vec{L}}=\vec{x} \wedge \vec{p} \:\:\:\:\: \Leftrightarrow \:\:\:\:\: L^{ij}=x^i p^j$$ And in 3 spati..
Classical Mechanics
2020. 10. 30. 11:20