Curves in differential geometry

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This page covers mathematical example of curves in differential geometry.

[edit] Constant curve

Given a point p0 in R3 and a subinterval I of the real line,

\mathbf{\gamma}:t \mapsto \mathbf{p_0} = \begin{pmatrix}  x_0\\  y_0\\  z_0\\ \end{pmatrix}\qquad (t \in I)

defines the constant curve, a parametric curve of class C. The image of the constant curve is the single point p. The curve is closed and analytic but not simple.

[edit] Line

A slightly more complex example is the line. A parametric definition of a line through the points p0 and p1 (p0p1 and p0,p1R3) is given by

\mathbf{\gamma}:t \mapsto \mathbf{p_0} + t(\mathbf{p_1} - \mathbf{p_0})= \begin{pmatrix}  x_0 + t (x_1 - x_0)\\  y_0 + t (y_1 - y_0) \\  z_0 + t (z_1 - z_0) \\ \end{pmatrix} \qquad (t \in I)

The image of the curve is a line. Note that

\mathbf{\gamma}:t \mapsto \mathbf{p_0} + t^3 (\mathbf{p_1} - \mathbf{p_0})= \begin{pmatrix}  x_0 + t^3 (x_1 - x_0)\\  y_0 + t^3 (y_1 - y_0) \\  z_0 + t^3 (z_1 - z_0) \\ \end{pmatrix} \qquad (t \in I)

is a different curve but the image of both curves is the same line.

[edit] Helix

Given r, ω in R

\mathbf{\gamma}:t \mapsto \begin{pmatrix}  r \cos (\omega t)\\  r \sin (\omega t)\\  t\\ \end{pmatrix}\qquad (t \in I)

defines a helix circling the z-axis.