【SEOテキスト】宇田雄一「古典物理学」【1d12】とは【1d12a】and【1d12b】のことだ。【1d12a】Qm(2,1)=abZ0【1d12b】∀t∈R;[t≦0⇒【1d12b1】]and[t≧0⇒【1d12b2】]【1d12b1】∃z∈R;z=r(t)-Qm(2,1)/E
and t=-1/α√αz2+2βz+c+β/α√αcosh-1(αz+β/√β2-αc)and θ(t)=h/β'√2β'/r(t)+A【1d12b2】∃z∈R;z=r(t)-Qm(2,1)/E
and t=1/α√αz2+2βz+c-β/α√αcosh-1(αz+β/√β2-αc)and θ(t)=-h/√β'√2β'/r(t)+A【1d13】とは【1d13a】and【1d13b】のことだ。【1d13a】Qm(2,1)>abZ0【1d13b】∀t∈R;[t≦0⇒【1d13b1】]and[t≧0⇒【1d13b2】]【1d13b1】∃z∈R;z=r(t)-Qm(2,1)/E
and t=-1/α√αz2+2βz+c+β/α√αcosh-1(αz+β/√β2-αc)and θ(t)=-h/√α'cosh-1(-α'/r(t)-β'/√β'2-α'A)【1d13b2】∃z∈R;z=r(t)-Qm(2,1)/E
and t=1/α√αz2+2βz+c-β/α√αcosh-1(αz+β/√β2-αc)and θ(t)=h/√α'cosh-1(-α'/r(t)-β'/√β'2-α'A)
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