AsymptoticDSolveValue[eqn,f,xx0]
计算微分方程 eqn 的渐近逼近,f[x] 以 x0 为中心.
AsymptoticDSolveValue[{eqn1,eqn2,…},{f1,f2,…},xx0]
计算微分方程组的渐近逼近.
AsymptoticDSolveValue[eqn,f,x,ϵϵ0]
计算 f[x,ϵ] 的渐近逼近,参数 ϵ 以 ϵ0 为中心.
AsymptoticDSolveValue[eqn,f,…,{ξ,ξ0,n}]
计算 n 阶渐近逼近.
AsymptoticDSolveValue
AsymptoticDSolveValue[eqn,f,xx0]
计算微分方程 eqn 的渐近逼近,f[x] 以 x0 为中心.
AsymptoticDSolveValue[{eqn1,eqn2,…},{f1,f2,…},xx0]
计算微分方程组的渐近逼近.
AsymptoticDSolveValue[eqn,f,x,ϵϵ0]
计算 f[x,ϵ] 的渐近逼近,参数 ϵ 以 ϵ0 为中心.
AsymptoticDSolveValue[eqn,f,…,{ξ,ξ0,n}]
计算 n 阶渐近逼近.
更多信息和选项
- 微分方程的渐近逼近亦被称为渐近展开式、摄动解、正则摄动和奇异摄动等. 也可用计算其中一些式子的特定方法来称呼它们,如 Frobenius 级数、WKB、边界层方法等.
- 渐近逼近通常用于求解无法找到精确解的问题,或者为计算、比较和解释寻求更简单的答案.
- AsymptoticDSolveValue[eqn,…,xx0] 计算 eqn 的渐近展开式的首项. 用 SeriesTermGoal 可指定计算更多的项.
- 如果精确结果为 g[x],在 x0 处的 n 阶渐近逼近为 gn[x],那么当 xx0 时,结果为 AsymptoticLess[g[x]-gn[x],gn[x]-gn-1[x],xx0] 或 g[x]-gn[x]∈o[gn[x]-gn-1[x]].
- 渐近逼近 gn[x] 常以和 gn[x]
αkϕk[x] 的形式给出,其中 {ϕ1[x],…,ϕn[x]} 是当 xx0 时的渐近尺度 ϕ1[x]≻ϕ2[x]≻⋯>ϕn[x]. 则当 xx0 时,结果为 AsymptoticLess[g[x]-gn[x],ϕn[x],xx0] 或 g[x]-gn[x]∈o[ϕn[x]]. - 常见的渐近尺度包括:
-

Taylor 尺度,当 xx0 时 
Laurent 尺度,当 xx0 时 
Laurent 尺度,当 x±∞ 时 
Puiseux 尺度,当 xx0 时 - 用于表示渐近逼近的尺度是从问题中自动推断出来的,通常可以包含更多的奇异尺度.
- 中心点 x0 可以为任意有限或无限大实数或复数.
- 阶数 n 必须为一个正整数,指定渐近解的近似阶数. 与多项式的次数无关.
- u∈Vectors[n] 或 u∈Matrices[{m,n}] 可分别用于表明因变量 u 是一个值为向量或矩阵的变量. 也可以用 VectorSymbol 或 MatrixSymbol 指定 u. » »
- 可以给出以下选项:
-
AccuracyGoal Automatic 寻求的绝对准确度 Assumptions $Assumptions 对参数的设定 GenerateConditions Automatic 是否给出与参数的条件有关的答案 GeneratedParameters None 怎样命名生成的参数 Method Automatic 所用的方法 PerformanceGoal $PerformanceGoal 优化目标 PrecisionGoal Automatic 寻求的精度 SeriesTermGoal Automatic 近似式的项数 WorkingPrecision Automatic 内部计算中使用的精度 - PerformanceGoal 的可能设置包括 $PerformanceGoal、"Quality" 和 "Speed". 当设置为 "Quality" 时,AsymptoticDSolveValue 通常可以解出更多的问题或者产生更简单的结果,但是可能会耗费更多的时间和内存.
范例
打开所有单元 关闭所有单元基本范例 (3)
AsymptoticDSolveValue[{y''[x] - y[x] == 0, y[0] == 0, y'[0] == 1}, y[x], x -> 0]AsymptoticDSolveValue[{y''[x] + y[x] == 0, y[0] == 1, y'[0] == 0}, y[x], {x, 0, 10}]Plot[%, {x, 0, 3π / 2}]AsymptoticDSolveValue[{ϵ y''[x] + y'[x] + x y[x] == 0, y[0] == 0, y[1] == 1 / 2}, y[x], x, {ϵ, 0, 1}]Plot[Evaluate[Table[%, {ϵ, {1 / 30, 1 / 10, 1 / 5}}]], {x, 0, 1}]范围 (50)
基本用法 (8)
AsymptoticDSolveValue[{y''[x] + x y[x] == 0, y[0] == 0, y'[0] == 1}, y[x], {x, 0, 10}]sol = AsymptoticDSolveValue[{y'[x] - y[x] == 0, y[0] == 1}, y[x], {x, 0, 4}]用 Accumulate 来构建逼近解的列表:
accum = Accumulate[List@@sol]Plot[Evaluate[accum], {x, 0, 5}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[{y''[x] + 2 y[x] == 0, y[3] == 1, y'[3] == 0}, y[x], {x, 3, 10}]AsymptoticDSolveValue[y''[x] + y[x] == 0, y[x], {x, 0, 8}]AsymptoticDSolveValue[{ y'[x] + 3y[x] == 1, y[0] == 2}, y[x], {x, 0, 3}]AsymptoticDSolveValue[{ y'[x] + 3y[x] == 1, y[0] == 2}, y[x], {x, 0, 5}]AsymptoticDSolveValue[{y'[x] == z[x] + 3, z'[x] == -y[x], y[0] == 1, z[0] == 5}, {y[x], z[x]}, {x, 0, 5}]AsymptoticDSolveValue[{y'[x] + ϵ y[x] == Cos[x], y[0] == 0}, y[x], x, {ϵ, 0, 1}]AsymptoticDSolveValue[{y'[x] + ϵ y[x] == Cos[x], y[0] == 0}, y[x], x, {ϵ, 0, 2}]AsymptoticDSolveValue[{y'[x] + ϵ y[x] == Cos[x], y[0] == 0}, y[x], x, {ϵ, 0, 3}]AsymptoticDSolveValue[{ y''[x] + ϵ y'[x] + y[x] == 0, y[0] == 1, y'[0] == 0}, y[x], x, {ϵ, 0, 2}]//SimplifyPlot[Evaluate[Accumulate[CoefficientList[%, ϵ] /. {ϵ -> 1 / 100}]], {x, 0, π / 2}]常点 (7)
AsymptoticDSolveValue[{ y'[x] - x y[x] == 0, y[0] == 1}, y[x], {x, 0, 10}]Plot[Evaluate[Accumulate[List@@%]], {x, 0, 3}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[{y''[x] + x y'[x] - y[x] == 0, y[0] == 1, y'[0] == 0}, y[x], {x, 0, 10}]Plot[Evaluate[Accumulate[List@@%]], {x, 0, 3}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[{y'[x] + 7y[x] == E ^ x, y[0] == 1}, y[x], {x, 0, 5}]AsymptoticDSolveValue[{y''[x] + E ^ x y'[x] + 7 Sin[x] ^ 2 y[x] == Cos[2x], y[0] == 1, y'[0] == 5}, y[x], {x, 0, 5}]AsymptoticDSolveValue[{y''''[x] + 26 y''[x] + 25 y[x] == 0, y[0] == 1, Derivative[1][y][0] == 0, Derivative[2][y][0] == -1, Derivative[3][y][0] == 5}, y[x], {x, 0, 8}]AsymptoticDSolveValue[{y''[x] + 5y[x] == Cos[2x], y[1] == 1, y'[1] == 5}, y[x], {x, 1, 3}]AsymptoticDSolveValue[{y''[x] + 5y[x] == 0}, y[x], {x, 1, 3}]正则奇点 (5)
求线性一阶常微分方程在正则奇点 x=0 处的 Frobenius 级数解:
AsymptoticDSolveValue[Sin[x] y'[x] + y[x] == 0, y[x], {x, 0, 7}]Plot[Evaluate[Accumulate[List@@(Expand[% /. {C[1] -> 1}])]], {x, 0, 3}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[2 x ^ 2 y''[x] + 3x y'[x] - (x ^ 2 + 1)y[x] == 0, y[x], {x, 0, 5}]AsymptoticDSolveValue[x ^ 4 y''''[x] + y[x] == 0, y[x], {x, 0, 4}]//FullSimplify(x ^ 4 y''''[x] + y[x] == 0 /. {y -> Function[{x}, Evaluate[%]]})//SimplifyAsymptoticDSolveValue[(x - 1)y''[x] + y[x] == 0, y[x], {x, 1, 2}]具有无理系数的线性常微分方程在正则奇点 x=0 处的级数解:
AsymptoticDSolveValue[Sin[x] ^ 2 * y''[x] + x y[x] == 0, y[x], {x, 0, 2}]非正则奇点 (3)
AsymptoticDSolveValue[x ^ 2 y'[x] + (x ^ 2 + 1)y[x] == 0, y[x], {x, 0, 4}]Plot[Evaluate[Accumulate[List@@(Expand[% /. {C[1] -> 1}])]], {x, 0, 3}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[x ^ 3 y''[x] + y[x] == 0, y[x], {x, 0, 2}]AsymptoticDSolveValue[x ^ 4 y'''[x] - 2 y'[x] + y[x] == 0, y[x], {x, 0, 2}]非线性常微分方程 (7)
AsymptoticDSolveValue[{ y'[x] - x y[x] ^ 3 == 0, y[0] == 1}, y[x], {x, 0, 8}]Plot[Evaluate[Accumulate[List@@%]], {x, 0, 1}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[{y''[x] + 2y'[x] - y[x] ^ 2 == 0, y[0] == 1, y'[0] == 0}, y, {x, 0, 6}]Plot[Evaluate[Accumulate[List@@%]], {x, 0, 3}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[{y'[x] + y[x] ^ 2 == E ^ (2x), y[0] == 1}, y[x], {x, 0, 5}]AsymptoticDSolveValue[{y''[x] + y'[x] ^ 2 + 7 Sin[x] ^ 2 y[x] == Cos[2x], y[0] == 1, y'[0] == 5}, y[x], {x, 0, 5}]AsymptoticDSolveValue[{y''''[x] + y''[x] ^ 2 + 3y[x] == 0, y[0] == 1, Derivative[1][y][0] == 0, Derivative[2][y][0] == -1, Derivative[3][y][0] == 5}, y[x], {x, 0, 8}]AsymptoticDSolveValue[{y''[x] + 7y[x] ^ 2 == Cos[2x], y[1] == 1, y'[1] == 5}, y[x], {x, 1, 3}]AsymptoticDSolveValue[{y''[x] + 3y[x] ^ 3 == 0}, y[x], {x, 0, 3}]无穷大处的解 (4)
AsymptoticDSolveValue[x ^ 2 y'[x] + y[x] == 0, y[x], {x, ∞, 4}]Plot[Evaluate[Rest@Accumulate[List@@(% /. {C[1] -> 1})]], {x, 0, 60}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[x ^ 3 y''[x] + x * y'[x] + y[x] == 0, y[x], {x, ∞, 3}]AsymptoticDSolveValue[y''[x] - x ^ 2 y[x] == 0, y[x], {x, ∞, 2}]AsymptoticDSolveValue[{x ^ 2 y'[x] - 5y[x] ^ 2 == 0, y[∞] == 1}, y[x], {x, ∞, 4}]常微分方程组 (8)
AsymptoticDSolveValue[{u'[x] == x v[x] + 3, v'[x] == -x u[x], u[0] == 1, v[0] == 3}, {u[x], v[x]}, {x, 0, 5}]ParametricPlot[Evaluate[%], {x, 0, 2}]AsymptoticDSolveValue[{y''[x] == z[x], z'[x] == -y[x], y[0] == 1, z[0] == 3, y'[0] == 4}, {y[x], z[x]}, {x, 0, 3}]AsymptoticDSolveValue[{y'[x] + z[x] == E ^ x, z'[x] == 5y[x] + 1, y[0] == 1, z[0] == 3}, {y[x], z[x]}, {x, 0, 5}]AsymptoticDSolveValue[{y'[x] == x z[x] + 2, z'[x] == -x y[x], y[1] == 1, z[1] == 3}, {y[x], z[x]}, {x, 1, 3}]AsymptoticDSolveValue[{y'[x] == 3 z[x], z'[x] == y[x]}, {y[x], z[x]}, {x, 1, 3}]使用向量变量在寻常点 x=0 处的 ODE 线性方程组的级数解:
m = {{0, 1}, {-1, 0}};AsymptoticDSolveValue[{y'[x] == m.y[x], y[0] == {1, 1}}, Element[y[x], Vectors[2]], {x, 0, 3}]或者将
定义为 VectorSymbol:
y = VectorSymbol["y", 2]AsymptoticDSolveValue[{y'[x] == m.y[x], y[0] == {1, 1}}, y[x], {x, 0, 3}]使用矩阵变量在寻常点 x=0 处的 ODE 线性方程组的级数解:
m = {{0, 1}, {-1, 0}};
x0 = {{1, 2}, {3, 4}};AsymptoticDSolveValue[{y'[x] == m.y[x], y[0] == x0}, Element[y[x], Matrices[{2, 2}]], {x, 0, 3}]//MatrixForm或者将
定义为 MatrixSymbol:
y = MatrixSymbol["y", {2, 2}]AsymptoticDSolveValue[{y'[x] == m.y[x], y[0] == x0}, y[x], {x, 0, 3}]//MatrixForm求解 ϵ=0: 处的扰动 Fuchsian 线性常微分方程组:
AsymptoticDSolveValue[{Derivative[1][y1][x] == ϵ ((3 y1[x]/-6 + x) + ((1/-8 + x) + (2/-6 + x)) y2[x] + ((2/-8 + x) + (3/-6 + x)) y3[x]), Derivative[1][y2][x] == ϵ (-(4 y1[x]/-8 + x) + ((3/-8 + x) + (2/-6 + x)) y3[x]), Derivative[1][y3][x] == 0, y1[0] == 1, y2[0] == 2, y3[0] == 3}, {y1[x], y2[x], y3[x]}, x, {ϵ, 0, 2}]正则摄动 (2)
AsymptoticDSolveValue[{y''[x] - y'[x] - ϵ x y[x] == 0, y[0] == 0, y'[0] == 1}, y[x], x, {ϵ, 0, 3}]//SimplifyPlot[Evaluate[CoefficientList[%, ϵ] /. {ϵ -> 1 / 10}], {x, 0, 3}, PlotLegends -> "Expressions"]AsymptoticDSolveValue[{u''[x] + u[x] + ϵ u[x] ^ 2 == 0, u[0] == 1, u'[0] == 2}, u[x], x, {ϵ, 0, 2}]//SimplifyPlot[Evaluate[% /. {ϵ -> 1 / 100}], {x, 0, 10}]奇异摄动 (3)
AsymptoticDSolveValue[{ϵ y''[x] + (x + 1) y[x] == 0, y[0] == 1, y[1] == 0}, y[x], x, {ϵ, 0, 1}]Plot[% /. {ϵ -> 1 / 500}, {x, 0, 1}]NDSolveValue[{(1 / 500) y''[x] + (x + 1) y[x] == 0, y[0] == 1, y[1] == 0}, y[x], {x, 0, 1}];Plot[%, {x, 0, 1}]AsymptoticDSolveValue[{ϵ y''[x] - (2x + 1) y[x] == 0, y[0] == 1 / 3, y[1] == 0}, y[x], x, {ϵ, 0, 2}]Plot[Table[%, {ϵ, {1 / 10, 1 / 30, 1 / 50}}]//Evaluate, {x, 0, 1}]AsymptoticDSolveValue[{y''[x] + λ (x + 1) ^ 2y[x] == 0, y[0] == 1, y[1] == 0}, y[x], x, {λ, ∞, 2}]Plot[% /. {λ -> 160}, {x, 0, 1}, WorkingPrecision -> 20]NDSolveValue[{y''[x] + 160(x + 1) ^ 2y[x] == 0, y[0] == 1, y[1] == 0}, y[x], {x, 0, 1}]Plot[%, {x, 0, 1}]分数阶常微分方程 (ODE) (3)
AsymptoticDSolveValue[{CaputoD[y[x], {x, 0.7}] + 3 y[x] == 0, y[0] == 1}, y[x], {x, 0, 5}]使用 DSolveValue 求解同一个 ODE:
dsol = DSolveValue[{CaputoD[y[x], {x, 0.7}] + 3 y[x] == 0, y[0] == 1}, y[x], x]asol[n_] := AsymptoticDSolveValue[{CaputoD[y[x], {x, 0.7}] + 3 y[x] == 0, y[0] == 1}, y[x], {x, 0, n}];Plot[Evaluate[{dsol, asol[5], asol[10], asol[15], asol[20]}], {x, 0, 2}, PlotLegends -> {"Exact", "n=5", "n=10", "n=15", "n=20"}]sol = AsymptoticDSolveValue[{CaputoD[y[x], {x, 1 / 2}] - x y[x] == 0, y[0] == 1}, y[x], {x, 0, 15}]eqns = {CaputoD[x1[t], {t, 0.95}] == 2x1[t] - x2[t], CaputoD[x2[t], {t, 0.95}] == 4x1[t] - 3x2[t], x1[0] == 1.2, x2[0] == 4.2};asol = AsymptoticDSolveValue[eqns, {x1, x2}, {t, 0, 15}]Plot[asol, {t, 0, 2}, PlotRange -> All]选项 (1)
应用 (7)
计算 Cos 的泰勒多项式近似:
sol1 = AsymptoticDSolveValue[{y''[x] + y[x] == 0, y[0] == 1, y'[0] == 0}, y[x], {x, 0, 8}]Plot[{sol1, Cos[x]}, {x, 0, 3Pi}, PlotRange -> {-2, 5}]sol2 = AsymptoticDSolveValue[{y''[x] + y[x] == 0, y[0] == 1, y'[0] == 0}, y[x], {x, 0, 16}]Plot[{sol2, Cos[x]}, {x, 0, 3Pi}, PlotRange -> {-2, 5}]sol[n_] := AsymptoticDSolveValue[{y''[x] + y[x] == 0, y[0] == 1, y'[0] == 0}, y[x], {x, 0, n}]Plot[{sol[4], sol[8], sol[12], sol[16], sol[24], Cos[x]}//Evaluate, {x, 0, 3Pi}, PlotRange -> {-2, 5}]sol = AsymptoticDSolveValue[x ^ 2 y''[x] + x y'[x] + (x ^ 2 - 1 / 4)y[x] == 0, y[x], {x, 0, 24}]Plot[{(sol /. {C[1] -> 1, C[2] -> 0}), (sol /. {C[1] -> 0, C[2] -> 1})}, {x, 0, 3π}, PlotRange -> {-2, 2}]airyode = y''[x] - x y[x] == 0;sol = AsymptoticDSolveValue[airyode, y[x], {x, ∞, 3}]与 Infinity 处的 Airy 函数展开式相比较:
s1 = Series[AiryAi[x], {x, ∞, 4}]//Normals2 = Series[AiryBi[x], {x, ∞, 4}]//NormalPlot[Evaluate[{AiryAi[x], AiryBi[x], (sol /. {C[1] -> 1 / (2 Sqrt[Pi]), C[2] -> 0}), (sol /. {C[1] -> 0, C[2] -> 1 / Sqrt[Pi]}) }], {x, -3, 3}, PlotLegends -> {AiryAi[x], AiryBi[x], "sol1", "sol2"},
PlotStyle -> Thickness[0.008]]ode = 3y'[x] ^ 2 + 4x y'[x] - y[x] + x ^ 2 == 0;sol = AsymptoticDSolveValue[ode, y[x], {x, 0, 4}]//Quietode /. y -> Function[{x}, Evaluate[sol]]//Simplifyodes = {u'[t] == u[t] ^ 2 / v[t] - u[t], v'[t] == u[t] ^ 2 - v[t]};StreamPlot[{u ^ 2 / v - u, u ^ 2 - v}, {u, -2, 2}, {v, -2, 2}]sol = AsymptoticDSolveValue[{odes, u[0] == a, v[0] == b}, {u[t], v[t]}, {t, 0, 5}];sol /. {a -> 1, b -> 1}eqn = {u''[x] + u[x] + ϵ u[x] ^ 3 == 0, u[0] == 3, u'[0] == 0};psol = AsymptoticDSolveValue[eqn, u[x], x, {ϵ, 0, 1}]Plot[psol /. {ϵ -> 1 / 800}, {x, 0, 20}, PlotPoints -> 100, WorkingPrecision -> 20]dsol = DSolveValue[eqn /. {ϵ -> (1/800)}, u[x], x]Plot[dsol // Evaluate, {x, 0, 20}, PlotPoints -> 100]求对应于
的 Sturm–Liouville 问题的近似特征函数,其中
取较大值. 用较小参数
重写问题:
eqns = {ϵ y''[x] + (x + 1) ^ 2y[x] == 0, y[0] == A, y[1] == B};sol = FullSimplify[AsymptoticDSolveValue[eqns, y[x], x, {ϵ, 0, 1}], 0 < x < 1]忽略 Csc 常量因子,使用
构建特征函数:
eigfuns = Simplify[(Sqrt[2] B Sin[(x (2 + x)/2 Sqrt[ϵ])] - A Sin[((-1 + x) (3 + x)/2 Sqrt[ϵ])]/Sqrt[1 + x]) /. {B -> 1, A -> 0, ϵ -> (9/4 n^2 π^2)}, n∈ℤ && n > 0]Plot[Table[eigfuns, {n, 1, 4}]//Evaluate, {x, 0, 1}]属性和关系 (3)
sol = AsymptoticDSolveValue[{y'[x] + y[x] == 0, y[0] == 1}, y[x], {x, 0, 8}]{y'[x] + y[x], y[0] == 1} /. y -> Function[{x}, Evaluate[sol]]用 DSolveValue 求精确解:
asol = AsymptoticDSolveValue[{y'[x] - 2y[x] == 0, y[0] == 1}, y[x], {x, 0, 4}]dsol = DSolveValue[{y'[x] - 2y[x] == 0, y[0] == 1}, y[x], x]Series[%, {x, 0, 4}]//Normal用 NDSolveValue 求数值解:
asol = AsymptoticDSolveValue[{y'[x] + 2y[x] == 0, y[0] == 1}, y[x], {x, 0, 10}]Table[%, {x, 0, 1, 0.2}]dsol = NDSolveValue[{y'[x] + 2y[x] == 0, y[0] == 1}, y[x], {x, 0, 1}]Table[%, {x, 0, 1, 0.2}]可能存在的问题 (1)
AsymptoticDSolveValue[{y''[x] + y[x] == 0, y[0] == 0, y'[0] == 1}, y[x], {x, 0, 4}]AsymptoticDSolveValue[{y''[x] + a y'[x] + y[x] == 0, y[0] == b, y'[0] == 1}, y[x], {x, 0, 4}]% /. {a -> 0, b -> 0}技术笔记
-
▪
- 分数阶微积分
相关指南
-
▪
- 渐近 ▪
- 方程求解 ▪
- 微积分 ▪
- 分数阶微积分 ▪
- 符号向量、矩阵和数组
文本
Wolfram Research (2018),AsymptoticDSolveValue,Wolfram 语言函数,https://reference.wolfram.com/language/ref/AsymptoticDSolveValue.html (更新于 2026 年).
CMS
Wolfram 语言. 2018. "AsymptoticDSolveValue." Wolfram 语言与系统参考资料中心. Wolfram Research. 最新版本 2026. https://reference.wolfram.com/language/ref/AsymptoticDSolveValue.html.
APA
Wolfram 语言. (2018). AsymptoticDSolveValue. Wolfram 语言与系统参考资料中心. 追溯自 https://reference.wolfram.com/language/ref/AsymptoticDSolveValue.html 年
BibTeX
@misc{reference.wolfram_2026_asymptoticdsolvevalue, author="Wolfram Research", title="{AsymptoticDSolveValue}", year="2026", howpublished="\url{https://reference.wolfram.com/language/ref/AsymptoticDSolveValue.html}", note=[Accessed: 13-September-2026]}
BibLaTeX
@online{reference.wolfram_2026_asymptoticdsolvevalue, organization={Wolfram Research}, title={AsymptoticDSolveValue}, year={2026}, url={https://reference.wolfram.com/language/ref/AsymptoticDSolveValue.html}, note=[Accessed: 13-September-2026]}