In Mathoverflow I wonder about the possibility of finding non-Euclidean versions of the generalized half-angle formulas $[1]$. The Russian mathematician Alexander Mednykh has kindly answered my question. Specifically, he has derived the hyperbolic version. Look at the following link:
Note: Generalized half-angle formula - Hyperbolic version
Reference
$[1]$ E. A. José García, Two Identities and their Consequences, MATINF, 6 (2020) 5-11.
lunes, 14 de junio de 2021
martes, 1 de junio de 2021
Using the half-angle formula for cosine to derive Zelich's lemma on mixtilinear incircles
Lemma (Ivan Zelich). Let $w$ be the $A$-mixtilinear incircle in $\triangle{ABC}$ touching side $AB$ at $E$, side $AC$ at $F$. Then
$$AE=AF=\frac{bc}{s}\tag{1}$$
where $s$ is the semiperimeter.
Proof 1. The radius of $w$ inscribed in $\angle{CAB}=\alpha$ is given by
$$\rho_a=r\sec^2{\frac{\alpha}{2}}\tag{2}$$
where $r$ is the inradius of the reference triangle and $\rho_a$ is the radius of $w$ (Durell and Robson 1935).
A proof of $(2)$ can be found here (see pp. 13).
$$AE=AF=\frac{bc}{s}\tag{1}$$
where $s$ is the semiperimeter.
Proof 1. The radius of $w$ inscribed in $\angle{CAB}=\alpha$ is given by
$$\rho_a=r\sec^2{\frac{\alpha}{2}}\tag{2}$$
where $r$ is the inradius of the reference triangle and $\rho_a$ is the radius of $w$ (Durell and Robson 1935).
A proof of $(2)$ can be found here (see pp. 13).
The half-angle formula for cosine states that
$$\cos^2{\frac{\alpha}{2}}=\frac{s(s-a)}{bc}\tag{3}$$
See here for a proof of $(3)$.
Call $I$ the Incenter of $\triangle{ABC}$ and $D$ the touchpoint between the incircle and $AC$. Denote $K$ the center of $w$. Notice that $\triangle{AID}\sim\triangle{AKF}$. Now, by similarity of triangles we have
$$\frac{r}{s-a}=\frac{\rho_a}{AF}\tag{4}$$
Combining $(2)$ and $(3)$ in $(4)$ we get $(1)$.
$\square$
Proof 2. We can also derive $(1)$ using the relationships $\Delta=rs$ and $\Delta=\frac{bc\sin{\alpha}}{2}$. Indeed, since
$$r=\frac{\Delta}{s}=\frac{\frac{bc\sin{\alpha}}{2}}{s}=\frac{bc\sin{\frac{\alpha}{2}}\cos{\frac{\alpha}{2}}}{s}.$$
Substituting in $(2)$ and simplifying we get
$$\rho_a=r\sec^2{\frac{\alpha}{2}}=\frac{bc}{s}\tan{\frac{\alpha}{2}}=\frac{bc\rho_a}{s\cdot{AF}}$$
from which the result holds.
$\square$
A proof using inversion can be found here.
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