@article{oai:soar-ir.repo.nii.ac.jp:00012989,
 author = {余越,  正一郎},
 journal = {信州大学工学部紀要},
 month = {Jul},
 note = {Working equation for the Lagrangian spectrum function over the entire range of Lagrangian turbulon frequencies is proposed. The principal assumptions are that the evolution of the state of a selected particle in time forms a Markov process and that the spectrum function is a rapidly decreasing function. The asymptotic form of the spectrum is expressed in the form, E₁₁(ω) = AL<ε>/ω₀² exp[-c²(ω/ω∞)²] / 1+(ω/ω₀)² where AL is the universal constant. AL ≈ c/4. 4. <ε> is the kinetic energy dissipation rate. ω is the Lagrangian turbulon frequency. The subscripts, 0 and ∞, mean the largest and the smallest turbulon respectively. This form behaves like ω⁻² in the inertial range and as an exponential decay in the viscous range. The result is applied to the estimation of the energy dissipation by solid particles suspended in a turbulent fluid., Article, 信州大学工学部紀要 32: 217-225 (1972)},
 pages = {217--225},
 title = {乱れの Lagrange スペクトルの漸近形},
 volume = {32},
 year = {1972}
}