• Study Resource
  • Explore
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Steiner Equiangular Tight Frames Redux
Steiner Equiangular Tight Frames Redux

May 2011 - Maths Genie
May 2011 - Maths Genie

... A particle of weight W newtons is held in equilibrium on a rough inclined plane by a horizontal force of magnitude 4 N. The force acts in a vertical plane containing a line of greatest slope of the inclined plane. The plane is inclined to the horizontal at an angle , where tan  = 34 as shown in Fi ...
The quadprog Package
The quadprog Package

Today`s Powerpoint
Today`s Powerpoint

2 Particle dynamics
2 Particle dynamics

dependence of light scattering cross
dependence of light scattering cross

... Ri ...
Work
Work

Non-Holonomic Motion Planning
Non-Holonomic Motion Planning

Relativity6
Relativity6

... The force is the cross-product of the velocity and magnetic field vectors, multiplied by the charge of the particle: F  q  v y Bz  vz By  xˆ  q  vx Bz  vz Bx  yˆ  q  vx By  v y Bx  zˆ ...
Skew-Tsankov algebraic curvature tensors in the Lorentzian setting
Skew-Tsankov algebraic curvature tensors in the Lorentzian setting

Physics 207: Lecture 2 Notes
Physics 207: Lecture 2 Notes

Problem Set #7 Solutions
Problem Set #7 Solutions

31GraphsDigraphsADT
31GraphsDigraphsADT

Magnetic monopoles
Magnetic monopoles

Other Coordinate Systems
Other Coordinate Systems

Introduction Initializations A Matrix and Its Jordan Form
Introduction Initializations A Matrix and Its Jordan Form

Sketching as a Tool for Numerical Linear Algebra Lecture 1
Sketching as a Tool for Numerical Linear Algebra Lecture 1

MATH 304 Linear Algebra Lecture 13: Span. Spanning
MATH 304 Linear Algebra Lecture 13: Span. Spanning

vector
vector

NECESSARY AND SUFFICIENT CONDITIONS FOR LTI SYSTEMS
NECESSARY AND SUFFICIENT CONDITIONS FOR LTI SYSTEMS

Math-12 (Pre-calculus)
Math-12 (Pre-calculus)

Math 3191 Applied Linear Algebra Lecture 11: Vector Spaces
Math 3191 Applied Linear Algebra Lecture 11: Vector Spaces

M1 January 2003 1. A railway truck P of mass 2000 kg is moving
M1 January 2003 1. A railway truck P of mass 2000 kg is moving

Treshold partitioning …
Treshold partitioning …

... Denoting Mx = y and setting y := y / || y ||, we have (I – WM -1) y = 0, where WM -1 is column stochastic matrix. Thus, the solution of the Problem is transformed to the solution of ...
Relation to the de Rham cohomology of Lie groups
Relation to the de Rham cohomology of Lie groups

< 1 ... 122 123 124 125 126 127 128 129 130 ... 214 >

Four-vector

In the theory of relativity, a four-vector or 4-vector is a vector in Minkowski space, a four-dimensional real vector space. It differs from a Euclidean vector in how its magnitude is determined. The transformations that preserve this magnitude are the Lorentz transformations, which include spatial rotations, boosts (a change by a constant velocity to another inertial reference frame), and temporal and spatial inversions. Regarded as a homogeneous space, the transformation group of Minkowski space is the Poincaré group, which adds to the Lorentz group the group of translations. The Lorentz group may be represented by 4×4 matrices.The article considers four-vectors in the context of special relativity. Although the concept of four-vectors also extends to general relativity, some of the results stated in this article require modification in general relativity.
  • studyres.com © 2025
  • DMCA
  • Privacy
  • Terms
  • Report