KelvinBei
例題
すべて開く すべて閉じる例 (6)
KelvinBei[2.5]ReImPlot[KelvinBei[x], {x, 0, 10}, PlotRange -> All]ComplexPlot3D[KelvinBei[2, z], {z, -2 - 2I, 2 + 2I}, PlotLegends -> Automatic]Series[KelvinBei[x], {x, 0, 15}]Infinityにおける級数展開:
Series[KelvinBei[x], {x, ∞, 2}]//FullSimplify//NormalSeries[KelvinBei[n, x], {x, -1, 2}, Assumptions -> x > 1]//FullSimplifyスコープ (37)
数値評価 (6)
KelvinBei[.5]KelvinBei[4588, 0]N[KelvinBei[-7, 8], 50]N[KelvinBei[-2], 50]KelvinBei[2, 0.20444444000555555008005]N[KelvinBei[2.47, 5 - I]]N[KelvinBei[I + 2.47, 5]]KelvinBei[7, 5`100]//TimingKelvinBei[7, 5`100000];//TimingAroundを使って平均的な場合の統計区間を計算する:
KelvinBei[Around[.9, 0.1]]KelvinBei[1, {{0, 1.2}, {1.2, 0}}]MatrixFunctionを使って行列のKelvinBei関数を計算することもできる:
MatrixFunction[KelvinBei[1, #]&, {{0, 1.2}, {1.2, 0}}]特定の値 (3)
KelvinBei[0]KelvinBei[1, 0]KelvinBei[0,x]の正の最小値を求める:
xmin = x /. FindRoot[D[KelvinBei[0, x], x] == 0, {x, 8}]Plot[KelvinBei[0, x], {x, -1, 10}, Epilog -> Style[Point[{xmin, KelvinBei[0, xmin]}], PointSize[Large], Red]]半整数次数でKelvinBeiを評価すると初等関数になる:
Table[KelvinBei[n, x Sqrt[2]], {n, {-1 / 2, 1 / 2}}]//FunctionExpand可視化 (3)
整数(
)と半整数(
)の次数でKelvinBei関数をプロットする:
Plot[{KelvinBei[0, x], KelvinBei[1, x], KelvinBei[-1 / 2, x]}, {x, 0, 10}]ComplexContourPlot[Re[KelvinBei[0, z]], {z, -3 - 6I, 3 + 6I}, IconizedObject[«PlotOptions»]]ComplexContourPlot[Im[KelvinBei[0, z]], {z, -3 - 6I, 3 + 6I}, IconizedObject[«PlotOptions»]]ComplexContourPlot[Re[KelvinBei[-1 / 4, z]], {z, -3 - 6I, 3 + 6I}, IconizedObject[«PlotOptions»]]ComplexContourPlot[Im[KelvinBei[-1 / 4, z]], {z, -3 - 6I, 3 + 6I}, IconizedObject[«PlotOptions»]]関数の特性 (12)
FunctionDomain[KelvinBei[0, x], x]FunctionDomain[KelvinBei[0, z], z, Complexes]FunctionDomain[KelvinBei[-1 / 2, x], x]FunctionDomain[KelvinBei[-1 / 2, z], z, Complexes]FunctionRange[KelvinBei[0, x], x, y]FunctionRange[KelvinBei[1, x], x, y]//QuietKelvinBei[0, -x]KelvinBei[1, -x]FunctionAnalytic[KelvinBei[0, z], z]KelvinBeiは非減少でも非増加でもない:
Table[FunctionMonotonicity[KelvinBei[n, x], x, PositiveReals], {n, 4}]Table[FunctionMonotonicity[KelvinBei[1 / n, x], x, PositiveReals], {n, 4}]KelvinBeiは単射ではない:
Table[FunctionInjective[KelvinBei[n, x], x], {n, 4}]Table[FunctionInjective[KelvinBei[1 / n, x], x], {n, 4}]Plot[{KelvinBei[1, x], KelvinBei[2, x], KelvinBei[1 / 3, x], -3, 1}, {x, 0, 7}]KelvinBeiは非負でも非正でもない:
Table[FunctionSign[KelvinBei[n, x], x, PositiveReals], {n, 4}]
は,
が整数でない場合,非正の実数において特異点または不連続点を持つ:
FunctionSingularities[KelvinBei[n, x], x]FunctionDiscontinuities[KelvinBei[n, x], x]KelvinBeiは凸でも凹でもない:
Table[FunctionConvexity[{KelvinBei[a, x], x > 0}, x], {a, 5}]TraditionalFormによる表示:
KelvinBei[n, x]//TraditionalForm微分 (3)
D[KelvinBei[x] , x]D[KelvinBei[1, x] , x]Table[D[KelvinBei[x], {x, k}], {k, 1, 5}]//SimplifyPlot[%, {x, -20, 20}, PlotLegends -> {"First Derivative", "Second Derivative", "Third Derivative", "Fourth Derivative", "Fifth Derivative"}]D[KelvinBei[x], {x, k}]// FullSimplify積分 (3)
Integrateを使って不定積分を計算する:
Integrate[KelvinBei[x], x]// FullSimplifyFullSimplify[D[%, x]]// FullSimplifyIntegrate[KelvinBei[x], {x, 0, 5}]Integrate[x KelvinBei[x]^2, x]// FullSimplifyIntegrate[x^2 KelvinBei[x], {x, 0, 5}]// FullSimplify級数展開 (5)
Seriesを使ってテイラー(Taylor)展開を求める:
Series[KelvinBei[n, x], {x, 0, 4}]terms = Normal@Table[Series[KelvinBei[x], {x, 1, m}], {m, 1, 5, 2}];
Plot[{KelvinBei[x], terms}, {x, 0, 10}, PlotRange -> {{0, 9}, {-10, 10}}]SeriesCoefficientを使った級数展開における一般項:
SeriesCoefficient[KelvinBei[x], {x, 1, m}]// FullSimplifyInfinityにおける級数展開を求める:
Series[KelvinBei[x], {x, Infinity, 1}]//Normal//FullSimplifySeries[KelvinBei[x], {x, DirectedInfinity[z], 1}, Assumptions -> x > 0 && z > 0]//Normal//FullSimplify//QuietSeries[KelvinBei[x], {x, x0, 2}]//FullSimplify関数の恒等式と簡約 (2)
KelvinBei[n, x] == (x/2 Sqrt[2] n)(-KelvinBei[-1 + n, x] - KelvinBei[1 + n, x] + KelvinBer[-1 + n, x] + KelvinBer[1 + n, x])//FullSimplifyKelvinBei[n, x] == -KelvinBei[2 + n, x] - (Sqrt[2] (1 + n) (KelvinBei[1 + n, x] + KelvinBer[1 + n, x])/x)//FullSimplify一般化と拡張 (1)
KelvinBeiはベキ級数に適用できる:
KelvinBei[Log[1 + x] + O[x] ^ 7]アプリケーション (3)
DSolve[x^4 Derivative[4][f][x] + 2 x^3 Derivative[3][f][x] - (1 + 2 n^2) (-x Derivative[1][f][x] + x^2 Derivative[2][f][x]) + (-4 n^2 + n^4 + x^4) f[x] == 0, f[x], x]円形の断面を持つワイヤの電気抵抗に対する交流周波数(表皮効果)をプロットする:
Plot[ω / 2 ( KelvinBer[ω]KelvinBei'[ω] - KelvinBei[ω]KelvinBer'[ω]) / (KelvinBer'[ω] ^ 2 + KelvinBei'[ω] ^ 2), {ω, 0, 4}]ある特定の値については,HypergeometricPFQRegularizedはKelvinBeiで表される:
(π z^2/16) HypergeometricPFQRegularized[{}, {(3/2), (3/2), 1}, -(z^4/256)]特性と関係 (5)
KelvinBei[x]FullSimplifyを用いてケルビン関数を含む式を簡約する:
D[x KelvinBei[1, x], x]FullSimplify[%]FunctionExpandを使って半整数次のケルビン関数を展開する:
FunctionExpand[KelvinBei[1 / 2, x]]Integrate[x (KelvinBer[x]^2 + KelvinBei[x]^2), x]KelvinBeiはMeijerGによって表すことができる:
MeijerGReduce[KelvinBei[n, x], x]Activate[%]//FullSimplifyテクニカルノート
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▪
- 特殊関数
関連するガイド
関連リンク
テキスト
Wolfram Research (2007), KelvinBei, Wolfram言語関数, https://reference.wolfram.com/language/ref/KelvinBei.html.
CMS
Wolfram Language. 2007. "KelvinBei." Wolfram Language & System Documentation Center. Wolfram Research. https://reference.wolfram.com/language/ref/KelvinBei.html.
APA
Wolfram Language. (2007). KelvinBei. Wolfram Language & System Documentation Center. Retrieved from https://reference.wolfram.com/language/ref/KelvinBei.html
BibTeX
@misc{reference.wolfram_2026_kelvinbei, author="Wolfram Research", title="{KelvinBei}", year="2007", howpublished="\url{https://reference.wolfram.com/language/ref/KelvinBei.html}", note=[Accessed: 21-June-2026]}
BibLaTeX
@online{reference.wolfram_2026_kelvinbei, organization={Wolfram Research}, title={KelvinBei}, year={2007}, url={https://reference.wolfram.com/language/ref/KelvinBei.html}, note=[Accessed: 21-June-2026]}