【SEOテキスト】宇田雄一「古典物理学」【3c3b3】0≦t-2nt0≦t0⇒θ(t)-2nθ0=cos-1[h2/r(t)+qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]【3c4】qm(2,1)=-ab2m(1,1)/2and∀t∈R;【3c4a】and【3c4b】and【3c4c】【3c4a】|t|=[m(1,1)]2/3[qm(2,1)]2[-qm(2,1)/m(1,1)r(t)+h2]√-2qm(2,1)/m(1,1)r(t)-h2【3c4b】t<0⇒θ(t)=-cos-1[h2m(1,1)/r(t)+qm(2,1)/-qm(2,1)]【3c4c】t>0⇒θ(t)=cos-1[h2m(1,1)/r(t)+qm(2,1)/-qm(2,1)]【3c5】-ab2m(1,1)/2<qm(2,1)<0and∀t∈R;【3c5a】and【3c5b】and【3c5c】【3c5a】|t|=1/K√K[r(t)]2-2qm(2,1)/m(1,1)r(t)-h2+qm(2,1)/m(1,1)K√Kcosh-1[Kr(t)-qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]【3c5b】t<0⇒θ(t)=-cos-1[h2/r(t)+qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]【3c5c】t>0⇒θ(t)=cos-1[h2/r(t)+qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]【3c6】0<qm(2,1)and∀t∈R;【3c6a】and【3c6b】and【3c6c】【3c6a】|t|=1/K√K[r(t)]2-2qm(2,1)/m(1,1)r(t)-h2+qm(2,1)/m(1,1)K√Kcosh-1[Kr(t)-qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]【3c6b】t<0⇒θ(t)=-cos-1[h2/r(t)+qm(2,1)/m(1,1)/√[qm(2,1)/m(1,1)]2+Kh2]
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