Given a vector function which has a derivative not equal to zero, for example $\mathbf{r}=(t,\,\cos(t)\,\sin(t))$, its derivative is called a tangent vector to the function $\mathbf{r}.$ $$\mathbf{r^\prime}=\left(\begin{array}{c}1\\-\sin(t)\\ \cos(t)\end{array}\right),\qquad 0\le t \le 2\pi.$$ If I graph $\mathbf{r^\prime}$ it just looks like a circle with center $\left(1,0,0\right),$ radius $1,$ and in the plane $x=1.$ However, I can choose some $t$ value and create a point on $\mathbf{r}$ as $P=\mathbf{r}(t)$ and that point will now be a vector of scalars. Indeed, $\mathbf{r^\prime}$ is a direction vector for a single tangent line which is tangent to the curve called $\mathbf{r}$ at the point $P$. Again, for example, if we let $t=\pi/2$, then $$\mathbf{r}\left(\frac{\pi}{2}\right) =P=\left(\begin{array}{c}\frac{\pi}{2}\\0\\1 \end{array}\right)$$ and "the" tangent line is $$\left(\begin{array}{c} x\\ y\\ z \end{array}\right)=P+\lambda\left(\begin{array}{c} 1\\ -\sin\left(\frac{\pi}{2}\right)\\ \cos\left(\frac{\pi}{2}\right) \end{array}\right) \tag{eq 1}$$ Call the tangent vector $\mathbf{\mathcal{T}}$ and note that wlog it could be $\mathbf{T}$ where $$\mathbf{T}=\frac{\mathbf{r^\prime}}{\Vert\mathbf{r^\prime}\Vert}$$ It just so happens that I want $\mathbf{\mathcal{T}}$ or $\mathbf{T}$ to be in the osculating plane, but I feel extraordinarily lucky that it occurred there, given that we could find an infinite number of other lines with corresponding direction vectors that would be tangent to point $P$. I am adding a picture, but my question is $\underline{\text{why does this math just happen to pick the tangent line that I want?}}$ Basically, I have the same question for the unit Normal, but perhaps if I can understand this one, I will figure the other out for myself. In context, I am trying to explain tangents, normals, and binormals to someone else and finally realized that I probably don't know it]1
Why is the tangent vector in $\mathbb{R}^3$ unique
differential-geometrymultivariable-calculusvectors
Related Solutions
Your fundamental error here is that $\mathbf u'$ is tangent to the curve, not normal to it. Once you’ve corrected that, you will still find that the gradient of $c$ is not equal to the normal (not “norm”) computed from the parameterization $\mathbf u(\theta)$, but this is to be expected—there’s no such thing as the normal to the curve. The vectors will be scalar multiples of each other, but there’s no guarantee that they’ll be equal. Indeed, you could just as well parameterize the circle as $(3+\cos\theta, 2-\sin\theta)$ or $(3+\cos2\theta,2+\sin2\theta)$, both of which will produce different tangent vectors.
Suppose you want to find the parametric equation of the circle passing through points A, B, C which you already know the coordinates of. This is the circumcircle of $\triangle ABC$. First you need to find the normal to the plane of the circle, which is along $v= (C - A) \times (B - A) $. Normalize it producing $n = \dfrac{v}{|v|} $
The center of the circle $O$ is on the perpendicular bisector of $AB$ and of $AC$, so find the two vectors
$u_1 = n \times (B - A) $ and $u_2 = n \times (C - A) $
Then the center is the solution of
$O = \frac{1}{2} (A + B) + t u_1 = \frac{1}{2} (A + C) + s u_2 $
This is a $3 \times 2$ system of equations in the variables $t, s$ which can be solved very easily, thus determining the center $O$.
Next, the radius $R$ is the circle is given $R = | O - A | = | O - B | = | O - C | $
Now the parametric equation is
$ p(t) = O + R v_1 \cos t + R v_2 \sin t $
where $v_1, v_2, n$ are normal to each other and of unit length.
The above described procedure is good for any three points $A, B, C$. In the case where these three points are vertices of a regular tetrahedron, then, the center of the circle is simply
$O = \frac{1}{3} (A + B + C) $
but we still have to compute the normal to the plane of the circle as described above.
Edit:
After a comment from the OP, that points $A, B, C$ are not available, and that what's available is the fourth vertex $D$ and the centroid of the tetrahedron $G$. In this case:
The center of the face opposing vertex $D$ (which is the face containing vertices $A, B, C$) is located at $O = G - \frac{1}{3} GD $
The normal to the face $ABC$ is along $GD$
The radius can be found as follows
$R = \sqrt{ |GD|^2 - \left(\frac{1}{3} |GD| \right)^2 } = \dfrac{\sqrt{8}}{3} | GD | $
Best Answer
You feel that you have many choices for the tangent, but that's not the case.
Intuitively, if you think you are "riding" the curve, you can think of the tangent vector as telling exactly what to do with your steering wheel (that would be the unit tangent vector) and the accelerator/brakes (that would be tangent's vector magnitude). So there is a single one.
Mathematically, you have $$ r(t+h)=r(t)+hr'(t)+ o(h^2).$$ If you have two "tangent vectors" $T_1$ and $T_2$, you would have $$ r(t+h)=r(t)+hT_1+o(h^2), \ \ \text{ and } r(t+h)=r(t)+hT_2+o(h^2). $$ This gives you $$ h(T_1-T_2)=o(h^2), $$ that can only happen when $T_1=T_2$.