Loring Tu in his book Differential geometry [page 104] states (in my own words) the following on geodesics on spheres:
Consider the 2 sphere of radius $a$ in $\mathbb{R}^3$ .
- Parameterise a great circle by arc length $\gamma$.
- $\gamma''(t)$ is perpendicular to $\gamma'(t)$
- $\gamma''(t)$ lies in the plane of the circle (does this mean $T_{\gamma(t)}M?)$
- $\gamma''(t)$ is perpendicular to the tangent plane at $\gamma(t)$
I'm not sure why $(4).$ holds, why is $\gamma''(t)$ in the normal space $N_{\gamma(t)}M$?
Please do not explain using curvature.
Note that the plane of the great circle contains the origin (i.e. the center of the sphere). $\gamma''$ is orthogonal to $\gamma'$, so because $\gamma'$ is parallel to the circumference, $\gamma''$ must be parallel to the radius of the great circle.
Now, note that the radius of the great circle is also a diameter of the sphere. So, $\gamma''$ is parallel to the radius of the sphere and hence orthogonal to its tangent plane.