Jacobi equation

Also known as geodesic deviation equation, it relates geodesics and Gaussian curvature.
This equation describes how the separation between geodesics (as measured by a Jacobi field) evolves as we move along the geodesics.
The equation is

D2dt2J+R(J,U)U=0,

with the notation given here. R is the Riemann curvature tensor.

In surfaces

In a 2-dimensional Riemannian manifold, the Riemann curvature tensor simplifies significantly. In particular, it can be expressed entirely in terms of the Gaussian curvature K. The Riemann curvature tensor in 2 dimensions is given by:

R(X,Y)Z=K(g(Y,Z)Xg(X,Z)Y),

where X,Y,Z are vector fields on the manifold, g is the metric tensor, and K is the Gaussian curvature.
So substituting this in the Jacobi equation we obtain

D2dt2J+K(g(U,U)Jg(J,U)U)=0.

If the geodesic has a unitary tangent vector the equation simplifies to:

D2dt2J+K(Jg(J,U)U)=0.

Intuitive approach of Needham

Case n=2

In a surface

ξ¨=Kξ

being ξ(t) the "separation" of two geodesics (@needham2021visual page 269; and proof in 274)

Proof
It uses geodesic polar coordinates. Also uses Gauss lemma.
By the way, it let us to show Minding's theorem.

Formal statement is based on the notion of Jacobi field.

Case n>2

Pasted image 20220707193229.png

According to @needham2021visual there are two versions:

P[vvξ]=P[R(ξ,v)v]=K(Π)ξ

where Π is a plane containing the tangent vector v to the geodesic, P is the projection over this plane and K(Π) is the sectional curvature.

vvξ=R(ξ,v)v

When R(ξ,v)v is not contained in Π it happens the rotation of picture b) above.