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)X−g(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)J−g(J,U)U)=0.

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

D2dt2J+K(J−g(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.
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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[∇v∇vξ]=−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.

∇v∇vξ=−R(ξ,v)v

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