
Raymond L. answered 05/20/15
Tutor
4.8
(33)
Math, SAT Math, Physics
Let g=g(r)=GM/r^2;
By Taylor Expansion, g(r+Δr)=g(r)+g'(r)Δr+(g'(r)Δr^2)/2+higher order terms
Therefore, g(r+Δr)-g(r)=Δg=g'(r)Δr+(g'(r)(Δr)^2)/2+higher order terms
Use Linear approximation( from Calculus 1),which ignores contributions from 2nd order term and all higher order terms,
g(r+Δr)-g(r)=Δg≈g'(r)Δr
g(r)=GM/r^2 and derivative of g(r) respect to r is g'(r)=-2GM/r^3
So, Δg≈g'(r)Δr=(-2GM/r^3)Δr, but g=GM/r^2.
Therefore,Δg≈-2g(Δr/r)
By Taylor Expansion, g(r+Δr)=g(r)+g'(r)Δr+(g'(r)Δr^2)/2+higher order terms
Therefore, g(r+Δr)-g(r)=Δg=g'(r)Δr+(g'(r)(Δr)^2)/2+higher order terms
Use Linear approximation( from Calculus 1),which ignores contributions from 2nd order term and all higher order terms,
g(r+Δr)-g(r)=Δg≈g'(r)Δr
g(r)=GM/r^2 and derivative of g(r) respect to r is g'(r)=-2GM/r^3
So, Δg≈g'(r)Δr=(-2GM/r^3)Δr, but g=GM/r^2.
Therefore,Δg≈-2g(Δr/r)