Among the Properties of a regular tetrahedron one is "The perpendicular from vertices to the opposite faces meet the faces at their centroid". How can I prove this by vector medhod?
About of a Regular Tetrahedron
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On
Here is a method which chooses a co-ordinate frame to put the tetrahedron in a standard form, and allow some simple calculations. This may not be quite permitted under your "vector method" requirement, but it does make things a deal easier.
Let the vertices of the tetrahedron be $\vec a=(1,1,1); \vec b=(1,-1,-1); \vec c=(-1,1,-1); \vec d=(-1,-1,1)$
The centroid of the last three points is $\frac 13(\vec b+\vec c+\vec d)=\frac 13(-1,-1,-1)$. The line joining this centre to the other vertex consists of the points $t \vec a$.
Now compute the scalar product of $t\vec a$ with two linearly independent vectors in the plane of the relevant face (eg $\vec b - \vec c, \vec b-\vec d$).
Alternatively, a vector perpendicular to the plane of the final three points is $(\vec b-\vec c)\times (\vec b-\vec d)$. Show that this is parallel to $\vec a$ and that the vector in direction $\vec a$ through the point with position vector $\vec a$ passes through the centroid.
On
For a pure vector method, let the vertices be at positions $0, \vec a, \vec b, \vec c$ so that the centroid of the final three is at $\frac 13 (\vec a+\vec b +\vec c)$.
If the side length is $d$ we have $$d^2=\vec a\cdot \vec a=\vec b\cdot \vec b=\vec c\cdot \vec c=(\vec a-\vec b)\cdot (\vec a-\vec b)=(\vec a-\vec c)\cdot (\vec a-\vec c)=(\vec c-\vec b)\cdot (\vec c-\vec b)$$From the last three we obtain $$\vec a\cdot \vec b =\vec a\cdot \vec c =\vec c\cdot \vec b =\frac 12d^2$$
Then we have $$\frac 13 (\vec a+\vec b +\vec c)\cdot(\vec a-\vec b)=\frac 13d^2(1-\frac 12+\frac 12-1+\frac 12-\frac 12)=0=\frac 13 (\vec a+\vec b +\vec c)\cdot(\vec a-\vec c)$$
Then we invoke symmetry to say this is true for each of the centroids of the sides.
On
Set the basis of the tetrahedron (an equilateral triangle) with the vertices at coordinates
$$v_k=\left(\cos\frac{2k\pi}3,\sin\frac{2k\pi}3,0\right)$$ for $k=0,1,2$. It is an easy matter to check that the origin is the centroid of the face.
Now it suffices to show that the remaining vertex lies on the $z$ axis, $v_3=(0,0,z)$.
Indeed,
$$\|\vec{v_kv_3}\|^2=\cos^2\frac{2k\pi}3+\sin^2\frac{2k\pi}3+z^2=1+z^2,$$
is independent of $k$. (And you can choose $z$ such that $\|\vec{v_kv_3}\|^2=\|\vec{v_0v_1}\|^2$). With $v_3$ off-axis, the $\|\vec{v_kv_3}\|$ would differ.
On
Let the unit vectors $a$,$b$, $c$ be the three edges emanating from the vertex $O$. Dropping the perpendicular from $C$ to the plane spanned by $a$ and $b$ requires solving $$(H=)\qquad c+\lambda(a\times b)=\mu a+\nu b$$ for $\lambda$, $\mu$, $\nu$. Taking the scalar product with $a$ and $b$ gives the equations $$c\cdot a=\mu+\nu\>b\cdot a,\qquad c\cdot b=\mu\>a\cdot b+\nu\ .$$ Since $a\cdot b=b\cdot c=c\cdot a={1\over2}$ this amounts to $\mu+{1\over2}\nu={1\over2}$,$\>{1\over2}\mu+\nu={1\over2}$ with the solution $\mu=\nu={1\over3}$. It follows that $$H={a+b+0\over3}\ .$$
Let $ABCD$ be our tetrahedron and $M$ be the centroid of $\Delta ABC$.
Thus, $$\vec{DM}=\frac{1}{3}\left(\vec{DA}+\vec{DB}+\vec{DC}\right)$$ and $$\vec{DM}\cdot\vec{AC}=\frac{1}{3}\left(\vec{DA}+\vec{DB}+\vec{DC}\right)\left(\vec{DC}-\vec{DA}\right)=$$ $$=\frac{1}{3}\left(DC^2-DA^2+\vec{DB}\cdot\vec{DC}-\vec{DB}\cdot\vec{DA}\right)=$$ $$=\frac{1}{3}\left(DB\cdot DC\cos60^{\circ}-DB\cdot DA\cos60^{\circ}\right)=0,$$ which says $$DM\perp AC.$$ By the same way we can prove that $$DM\perp AB$$ and since $\vec{AB}$ and $\vec{AC}$ they are the base of the plane $ABC$, we obtain $$DM\perp(ABC).$$ But there is an unique perpendicular from $D$ to the plane $ABC$ and we are done.