05 - coordinate systems and parametric curves
Parametric Curves
Definition
Parametric Equation in ℝ3: A vector-valued function ( \mathbf{F}: I \subset \mathbb{R} \to \mathbb{R}^3 ) defined as:
( t \mapsto \mathbf{F}(t) = f(t) \mathbf{i} + g(t) \mathbf{j} + h(t) \mathbf{k} )
Points on the curve: M with coordinates ( (f(t), g(t), h(t)) )
Basics of Parametric Curves
Any curve has infinite parametric descriptions.
A curve is described by:
Parametric equations
Domain ( I )
Assume functions are differentiable sufficient times.
Parametric Descriptions of Lines
Straight Line AB:
Points A and B in ( \mathbb{R}^3 )
Parametric description:
( x(t) = x_A + t(x_B - x_A) )
( y(t) = y_A + t(y_B - y_A) )
( z(t) = z_A + t(z_B - z_A) )
( t \in \mathbb{R} )
Segment [AB]:
( t \in [0, 1] )
Same equations apply.
Parametric Description of Circles
Circle of center O and radius R:
( x(t) = R \cos(t) )
( y(t) = R \sin(t) )
( t , \in , [0, 2\pi) )
Tangent Vector to the Curve
Derivative of parametric equation:
( \mathbf{F}'(t) = f'(t) \mathbf{i} + g'(t) \mathbf{j} + h'(t) \mathbf{k} )
Determines the motion of point particles:
Velocity: ( \mathbf{v}(t) = \frac{dOM}{dt} )
Acceleration: second derivative gives trajectory's curvature.
Application in Mechanics
Parameter t corresponds to time.
Trajectory is described as motion of a particle M.
Coordinate Systems
Introduction
Used to:
Locate points in ( \mathbb{R}^3 )
Define displacement
Compute areas and volumes
Several systems are available based on problem geometry.
Usual Coordinate Systems
Cartesian Coordinates (x, y)
Cylindrical Coordinates (r, \theta, z):
Use when there's symmetry around z-axis.
Spherical Coordinates (\rho, \phi, \theta):
Use for spherical symmetry.
Local Frames in Coordinates
Defined by:
Orthonormal direct frame based on local unit vectors tangent to coordinate curves.
Derivative of local frames required for velocity calculations.
Differentiation of Curves in Coordinates
Depend on chosen frame, leading to:
Displacement approximations for small variations of coordinates.
Parametric Curves Summary (80/20 Rule):
Definition: A parametric equation in 3D represents a curve via a vector-valued function, defining points by coordinates based on time parameter t.
Basics: Any curve can be described in infinite ways using parametric equations which depend on differentiable functions.
Lines: Straight lines in (\mathbb{R}^3) are defined by their endpoints with equations for x, y, and z based on parameter t.
Circles: Parametric equations for a circle center O and radius R involve trigonometric functions.
Tangent Vector: The derivative of a parametric equation provides velocity and acceleration of point particles, determining trajectory.
Applications: In mechanics, t represents time as the trajectory of a particle in motion.
Coordinate Systems: Different systems (Cartesian, Cylindrical, Spherical) help locate points and compute geometry based on the problem context.
Coordinate Systems
Introduction
Used to locate points in ( ( \mathbb{R}^3 ) ), define displacement, and compute areas and volumes.
Several systems are available based on problem geometry.
Usual Coordinate Systems
Cartesian Coordinates (x, y): Standard system for locating points.
Cylindrical Coordinates (r, ( \theta ), z): Useful when there's symmetry around the z-axis.
Spherical Coordinates (( \rho ), ( \phi ), ( \theta )): Used for spherical symmetry.
Local Frames in Coordinates
Defined by an orthonormal direct frame based on local unit vectors tangent to coordinate curves.
The derivative of local frames is required for velocity calculations.
Differentiation of Curves in Coordinates
Differentiation depends on the chosen frame, which leads to displacement approximations for small variations of coordinates.