【SEOテキスト】宇田雄一「古典物理学」【3c6c】t>0⇒θ(t)=cos-1[h2/r(t)+qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]ケプラー運動∀f∈F2,1;∀E∈F3;∀Z∈F4,1;∀q∈R;∀M∈R(1);∀m∈R(2×1);[【1】and【2】]⇒【3】【1】m(1,1)M(1)=-qm(2,1)and
m(1,1)>0 and M(1)>0 and Z=0【2】∀ξ∈N01;∀i∈3;E(ξ,i,1)=qγ(i;ξ(3),0)and
E(ξ,i,2)=0【3】e2(f,E,m)⇔e1(f(□,□,1),Z,M,m(□,1))]二体問題∀f∈F2,2;∀Z∈F4,1;∀m∈R(2×2);∀m'∈R(1);【1】⇒[[∃f1,f2∈F1;【2】and【3】]⇔e2(f,0,m)]【1】m(1,1)>0
and m(1,2)>0 and m'(1)=m(1,1)+m(1,2)and Z=0【2】f(□,□,1)=1/m'(1)f1+m(1,2)/m'(1)f2
and f(□,□,2)=1/m'(1)f1-m(1,1)/m'(1)f2【3】e1(f1,Z,0,M)and e1(f2,Z,m',M)平面電磁波∀f∈F3;∀a∈R(R);[∀ξ∈N01;f(ξ,1,1)=f(ξ,3,1)=f(ξ,1,2)=f(ξ,2,2)=0
and f(ξ,2,1)=f(ξ,3,2)=a(ξ(1)-ξ(4))]⇒e3(f,Y,0)
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