Andrei from Romania sent in a good solution
to this problem.
(1)(a) We have to show that $qq^{1} = 1$: $$q^{1} = ({1\over
\sqrt 2} + {1\over \sqrt 2}{\bf i}) ({1\over \sqrt 2}  {1\over
\sqrt 2}{\bf i}) = {1\over 2}(1  {\bf i}^2) = 1$$ (b)Take $x = ti$
to be any point on the xaxis. Then $qx = ({1\over \sqrt 2} +
{1\over \sqrt 2}{\bf i})t{\bf i} = {1\over \sqrt 2} + {1\over
\sqrt 2}{\bf i})t = xq.$
We have shown that $qx = xq$ and so $qxq^{1} = x$.

Let $F(v) = qvq^{1}$ be a mapping of points $v$ in $R^3$ to
images in $R^3$ where the 4dimensional quaternion $q$ acts as an
operator. We have proved that this mapping fixes every point on the
x axis. 
(c)What effect does this mapping have on other points in
$R^3$? $$F({\bf j})= qjq^{1} = ({1\over \sqrt 2} + {1\over \sqrt
2}{\bf i})({\bf j}) ({1\over \sqrt 2}  {1\over \sqrt 2}{\bf i})$$
$$ = {1\over 2}(1+{\bf i})({\bf j})((1  {\bf i})$$ $$ = {1\over
2}({\bf j} + {\bf k})(1  {\bf i})$$ $$ = {1\over 2}({\bf j} + {\bf
k} + {\bf k}  {\bf j})$$ $$= {\bf k}.$$ Similarly $F{\bf k} =
{\bf j}$. Parts (b) and (c) together show that the mapping $F(v) =
qvq^{1}$, where $q = \cos (\pi /4) + \sin (\pi /4) {\bf i}$, gives
a rotation of $\pi /2$ about the x axis.

(2) In this section we consider the mapping $G(v) = qvq^{1}$
of $R^3$ to $R^3$ where the quaternion $q = \cos \theta + \sin
\theta {\bf k}$ is an operator. 
(a) $(cos \theta + \sin\theta k)(\cos \theta  \sin \theta k)
= \cos^2 \theta + \sin^2 \theta = 1$ so these two quaternions are
multiplicative inverses.
(b) We have $qk = \sin \theta + \cos \theta k = kq$ and hence
$qkq^{1} = k$. So the mapping $G(v) = qvq^{1}$ fixes the
zaxis.
(c) What effect does the mapping $G$ have on vectors in $R^3$?
We consider the vector $v = r(\cos \phi {\bf i} + \sin \phi {\bf
j})$. $$ qvq^{1} =(\cos \theta + \sin \theta {\bf k})r(\cos \phi
{\bf i} + \sin \phi {\bf j}) (\cos \theta  \sin \theta {\bf k}) $$
$$= r((\cos \theta\cos \phi  \sin \theta \sin \phi){\bf i} +(\cos
\theta \sin \phi + \sin \theta \cos \phi){\bf j}) \cos \theta {\bf
i} \sin \theta {\bf k}) $$ $$ = r(\cos (\theta + \phi) {\bf i} +
\sin (\theta + \phi){\bf j}) (\cos \theta {\bf i} \sin \theta {\bf
k}) $$ $$= r((\cos (\theta +\phi)\cos \theta  \sin (\theta +
\phi)\sin \phi){\bf i} + (\cos (\theta +\phi)\sin \theta + \sin
(\theta + \phi)\cos phi){\bf j})$$ $$= r(\cos (2\theta + \phi){\bf
i} + \sin (2\theta + \phi){\bf j}).$$

We have shown $qkq^{1} = k$ so $G(v+tk)= q(v +tk)q^{1} =
qvq^{1} + qtkq^{1} = qvq^{1} + tk$ for all $t$.
We can see that the vector $v$ in the $xy$ plane is rotated
about the $z$ axis by an angle $2\theta$ and all points on the vertical line through
it are also rotated about the $z$axis by an angle
$2\theta$.
So by the mapping $G(v) = qvq^{1}$ all points in $R^3$ are
rotated by $2\theta$ about the $z$axis.
Note that, for any rotation of $R^3$, we can make a
transformation of the coordinate system so that the axis of the
rotation is made to coincide with the $z$axis, then perform the
rotation by the given angle about the $z$axis, and finally
transform back to the original coordinate system.
