Geometry and Trigonometry 605
=f^2 (−→v ×−→v′)×(−→v ×−→v′′).
By thecab-bacformula this is further equal to
f^2 (−→v′′·(−→v ×−→v′)−→v −−→v ·(−→v ×−→v′)−→v)=f^2 ((−→v ×−→v′)·−→v′′)−→v.
The equation reduces therefore to
f^2 ((−→v ×−→v′)·−→v′′)−→v =−→v.
By hypothesis−→v is never equal to
−→
0 , so the above equality implies
f=
1
√
(−→v ×−→v′)·−→v′′
.
So the equation can be solved only if the frame(−→v,−→v′,−→v′′)consists of linearly inde-
pendent vectors and is positively oriented and in that case the solution is
−→u =√^1
Vo l(−→v,−→v′,−→v′′)
−→v ×−→v′,
where Vol(−→v,−→v′,−→v′′)denotes the volume of the parallelepiped determined by the three
vectors.
(Revista Matematica din Timi ̧soara ̆ (Timi ̧soara Mathematics Gazette), proposed by
M. Ghermanescu) ̆
579.(a) Yes: simply rotate the plane 90◦about some axis perpendicular to it. For example,
in thexy-plane we could map each point(x, y)to the point(y,−x).
(b) Suppose such a bijection existed. In vector notation, the given condition states that
(−→a −
−→
b)·(f (−→a)−f(
−→
b))= 0
for any three-dimensional vectors−→a and
−→
b.
Assume without loss of generality thatfmaps the origin to itself; otherwise,g(−→p)=
f(−→p)−f(
−→
0 )is still a bijection and still satisfies the above equation. Plugging
−→
b =
( 0 , 0 , 0 )into the above equation, we obtain that−→a ·f(−→a)=0 for all−→a. The equation
reduces to
−→a ·f(−→b)−−→b ·f(−→a)= 0.
Givenany vectors−→a,
−→
b,−→c and any real numbersm, n, we then have
m(−→a ·f(
−→
b)+
−→
b ·f(−→a))= 0 ,