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Properties of Vector Fields Parallel to a Curve 📂Geometry

Properties of Vector Fields Parallel to a Curve

Properties

Let X(t)\mathbf{X}(t) and Y(t)\mathbf{Y}(t) be vectors parallel to a regular curve α(t)\alpha (t) on the surface MM. Then the angle between X\mathbf{X} and X(t),Y(t)\mathbf{X}(t), \mathbf{Y}(t), and the magnitude of X(t)\left\| \mathbf{X}(t) \right\| are constants.

Description

In other words, both the angle and magnitude are conserved.

Proof

Let f(t)=X(t),Y(t)f(t) = \left\langle \mathbf{X}(t), \mathbf{Y}(t) \right\rangle. Differentiating ff, by the differentiation of inner products, we get:

dfdt=dXdt,Y+X,dYdt=0+0=0 \dfrac{d f}{d t} = \left\langle \dfrac{d \mathbf{X}}{d t}, \mathbf{Y} \right\rangle + \left\langle \mathbf{X}, \dfrac{d \mathbf{Y}}{d t} \right\rangle = 0 + 0 = 0

Here, X(t),Y(t)\mathbf{X}(t), \mathbf{Y}(t) is the tangent vector of MM, and dXdt(t),dYdt(t)\dfrac{d \mathbf{X}}{d t}(t), \dfrac{d \mathbf{Y}}{d t}(t), by definition, is orthogonal to the tangent vector, so the inner product is 00. Hence f(t)f(t) is constant. If we set Y=X\mathbf{Y}=\mathbf{X}, we get that X(t)\left\| \mathbf{X}(t) \right\| is also constant.

Now, if we denote the angle between X(t)\mathbf{X}(t) and Y(t)\mathbf{Y}(t) as θ\theta, we obtain:

f(t)X(t)Y(t)=cosθ \dfrac{f(t)}{\left\| \mathbf{X} (t) \right\| \left\| \mathbf{Y}(t) \right\|} = \cos \theta

Since f(t),X(t),Y(t)f(t), \left\| \mathbf{X} (t) \right\|, \left\| \mathbf{Y}(t) \right\| are both constants, cosθ\cos \theta is also constant. Therefore, the angle between them is constant.