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The Gergonne and Nagel centers of a tetrahedron证明了存在一个点P,AP,BP,CP,DP将相对的面分成3个三角形,共12个三角形,使公共边是一条棱的两个三角形的面积相等。
The Gergonne center [4] of a triangle $A B C$ is defined to be the point of intersection of the cevians $A A^{\prime}, B B^{\prime}, C C^{\prime}$ where $A^{\prime}, B^{\prime}, C^{\prime}$ are the points where the incircle of $A B C$ touches the sides $B C, C A, A B$ (Figure 1). Such cevians are concurrent by Ceva's Theorem since $A^{\prime}, B^{\prime}, C^{\prime}$ can be equivalently defined by the algebraic relations
\begin{align}
A B^{\prime}=A C^{\prime}, \quad B C^{\prime}=B A^{\prime}, \quad C A^{\prime}=C B^{\prime}
\end{align}
The Nagel center is defined similarly by taking $A^{\prime}, B^{\prime}, C^{\prime}$ to be the points where the excircles touch the sides (Figure 1). It can be easily seen that the points $A^{\prime}, B^{\prime}, C^{\prime}$ can also be defined by the relations
\begin{align}
B C^{\prime}=C B^{\prime}, C A^{\prime}=A C^{\prime}, \quad A B^{\prime}=B A^{\prime}
\end{align}
This note is a result of the question whether Gergonne and Nagel centers can be defined for a general tetrahedron in a similar way.
The generalized Ceva's Theorem [6] states that the cevians $A A^{\prime}, B B^{\prime}, C C^{\prime}, D D^{\prime}$ are concurrent if and only if one can assign masses $M_A, M_B, M_C, M_D$ to the vertices in such a way that the center of mass of each three of them is one of the points $A^{\prime}, B^{\prime}, C^{\prime}, D^{\prime}$. From Figure 2, this is equivalent to the conditions
\begin{align*}
& M_A: M_B: M_C=x: y: z, \quad M_B: M_C: M_D=Z: Y: x, \\
& M_C: M_D: M_A=X: y: Z, \quad M_D: M_A: M_B=z: Y: X .
\end{align*}
These in turn can be seen to be equivalent to the conditions
\begin{align}
X x=Y y=Z z \quad(=t, \text { say })
\end{align}
Denoting the areas of the faces by $\alpha, \beta, \gamma$, we see that
\begin{align}
x+y+z=\delta \\
x+Y+Z=\alpha \\
X+y+Z=\beta \\
X+Y+z=\gamma
\end{align}
Adding (5), (6) and (7) and subtracting (4), we get
\begin{align}
X+Y+Z=(\alpha+\beta+\gamma-\delta) / 2
\end{align}
Subtracting (8) from (5) and using the fact that $X=t / x$, we obtain
\[
x-t / x+(-\alpha+\beta+\gamma-\delta) / 2=0
\]
and hence
\[
x^2+x(-\alpha+\beta+\gamma-\delta) / 2-t=0 .
\] |
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