Ma · Mathematics

How to Find the Inverse Laplace Transform of arctan(2/s²)

Published By the 9to5Science editorial team

At a glance

  1. 1. Expand the arctangent

    Use its power series for sufficiently large s to write the transform as powers of 1/s.

  2. 2. Invert each term

    Apply the standard inverse transform of 1/s to a positive integer power.

  3. 3. Check convergence

    The resulting factorial-denominator series converges for every finite time.

  4. 4. Verify the transform

    Taking the Laplace transform term by term recovers the arctangent series.

Title: How to Find the Inverse Laplace Transform of arctan(2/s²)

Category: mathematics

The inverse Laplace transform of arctan⁡(2/s2)\arctan(2/s^2) has an elementary closed form, although it is not one of the most basic transform-table pairs. A direct method is to expand the arctangent in powers of 1/s1/s and invert each term. This gives an exact series that converges for every finite t≥0t\geq 0.

Expand the transform

The Taylor series for the arctangent is

arctan⁡x=∑n=0∞(−1)nx2n+12n+1,∣x∣<1.\arctan x=\sum_{n=0}^{\infty}\frac{(-1)^n x^{2n+1}}{2n+1},\qquad |x|<1.

Put x=2/s2x=2/s^2. For ∣s∣>2|s|>\sqrt{2}, this gives

arctan⁡(2s2)=∑n=0∞(−1)n22n+12n+11s4n+2.\arctan\left(\frac{2}{s^2}\right) =\sum_{n=0}^{\infty}\frac{(-1)^n2^{2n+1}}{2n+1}\frac{1}{s^{4n+2}}.

The condition ∣s∣>2|s|>\sqrt{2} is where this particular series expansion is valid. It is enough to identify the inverse transform, since Laplace transforms are compared in a right half-plane where they converge.

Invert term by term

Use the standard pair

L−1{1sm}(t)=tm−1(m−1)!,m=1,2,3,….\mathcal{L}^{-1}\left\{\frac{1}{s^m}\right\}(t) =\frac{t^{m-1}}{(m-1)!},\qquad m=1,2,3,\ldots.

Here m=4n+2m=4n+2, so each term contributes a multiple of t4n+1/(4n+1)!t^{4n+1}/(4n+1)!. Therefore

L−1{arctan⁡(2s2)}(t)=∑n=0∞(−1)n22n+1t4n+1(2n+1)(4n+1)!,t≥0.\boxed{ \mathcal{L}^{-1}\left\{\arctan\left(\frac{2}{s^2}\right)\right\}(t) =\sum_{n=0}^{\infty}\frac{(-1)^n2^{2n+1}t^{4n+1}}{(2n+1)(4n+1)!} },\qquad t\geq 0.

In fact, this series sums to the elementary expression

f(t)=2sin⁡(t)sinh⁡(t)t,f(t)=\frac{2\sin(t)\sinh(t)}{t},

with the continuous value f(0)=0f(0)=0. To verify it, use the identity

L{cos⁡(bt)−cos⁡(at)t}(s)=12log⁡(s2+a2s2+b2)\mathcal{L}\left\{\frac{\cos(bt)-\cos(at)}{t}\right\}(s) =\frac12\log\left(\frac{s^2+a^2}{s^2+b^2}\right)

for sufficiently large real ss. Taking a=1+ia=1+i and b=1−ib=1-i, and using cos⁡((1−i)t)−cos⁡((1+i)t)=2isin⁡(t)sinh⁡(t)\cos((1-i)t)-\cos((1+i)t)=2i\sin(t)\sinh(t), gives

L{2sin⁡(t)sinh⁡(t)t}(s)=12ilog⁡(s2+2is2−2i)=arctan⁡(2s2)\mathcal{L}\left\{\frac{2\sin(t)\sinh(t)}{t}\right\}(s) =\frac{1}{2i}\log\left(\frac{s^2+2i}{s^2-2i}\right) =\arctan\left(\frac{2}{s^2}\right)

for sufficiently large real ss. The series above is the Taylor expansion of this same function.

The first few terms are

f(t)=2t−t545+t956700−128t137⋅13!+⋯ .f(t)=2t-\frac{t^5}{45}+\frac{t^9}{56700}-\frac{128t^{13}}{7\cdot13!}+\cdots.

For example, at t=1t=1, the first three terms give

f(1)≈2−145+156700≈1.9777954.f(1)\approx 2-\frac{1}{45}+\frac{1}{56700}\approx 1.9777954.

The next term changes this approximation by only about 2.94×10−92.94\times10^{-9}.

Why the series is a valid inverse

The series for the arctangent converges when ∣2/s2∣<1|2/s^2|<1. On the other hand, the Laplace transform of each time-domain term is

L{(−1)n22n+1t4n+1(2n+1)(4n+1)!}(s)=(−1)n22n+1(2n+1)s4n+2.\mathcal{L}\left\{\frac{(-1)^n2^{2n+1}t^{4n+1}}{(2n+1)(4n+1)!}\right\}(s) =\frac{(-1)^n2^{2n+1}}{(2n+1)s^{4n+2}}.

For real s>2s>\sqrt{2}, the sum of the absolute values of these transforms converges. Thus the terms can be transformed and summed there, reproducing the arctangent power series. The time-domain series also converges for every finite tt: the factorial (4n+1)!(4n+1)! in its denominator grows faster than the powers in its numerator. These facts verify the transform and yield the stated inverse.

The formula uses the usual principal arctangent on positive real ss. For complex ss, branch choices matter; the power-series argument establishes the transform in a right half-plane, which is the relevant setting for the unilateral Laplace transform.

Common mistakes

  • Using the wrong arctangent series. The powers are x2n+1x^{2n+1}, so substituting 2/s22/s^2 produces powers s−(4n+2)s^{-(4n+2)}, not s−(2n+1)s^{-(2n+1)}.
  • Forgetting the factorial. The inverse of 1/s4n+21/s^{4n+2} is t4n+1/(4n+1)!t^{4n+1}/(4n+1)!.
  • Treating the power series as valid for every ss. The arctangent expansion requires ∣s∣>2|s|>\sqrt{2}. This restriction applies to that expansion, not to the time-domain series, which converges for all finite tt.
  • Expecting a basic transform-table pair. The answer does have the elementary form 2sin⁡(t)sinh⁡(t)/t2\sin(t)\sinh(t)/t, though deriving it from a table may require a logarithmic cosine-difference identity; the series gives a direct alternative.

If you need a numerical value, truncate the series after enough terms for the desired accuracy. For small or moderate tt, the factorials make the terms decrease quickly; for large tt, use more terms and check convergence rather than assuming the first few terms suffice.

References

  1. Erwin Kreyszig, Advanced Engineering Mathematics

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