Arc length problem with a thorny integration

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SUMMARY

The discussion centers on calculating the arc length of a particle's path defined by the parametric equations \(\gamma(t) = \left(\frac{t^2}{2}, t, \ln(2t)\right)\) for \(t\) in the interval \([1, 4]\). The speed differential is derived as \(ds = \sqrt{t^2 + 1 + \frac{1}{t^2}} dt\), leading to the arc length formula \(\ell = \int_1^4 \sqrt{t^2 + 1 + \frac{1}{t^2}} dt\). The discussion highlights the challenge of evaluating this integral, with attempts at trigonometric substitutions and the use of Wolfram's online integrator yielding complex results. A key insight is recognizing that \(t^2 + 1 + \frac{1}{t^2}\) can be rewritten as \((t + \frac{1}{t})^2 - 1\), which simplifies the integration process.

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Homework Statement



So, the question gives a particle traveling over a path [itex]\gamma[/itex], and I need the arc length.

Homework Equations



The path is [itex]\gamma(t) : [1,4] \to ℝ^3, t \mapsto (t^2/2, t, ln(2t))[/itex].

We want the arc length over [itex]1 \le t \le 4[/itex].

The Attempt at a Solution



First, the speed differential: [itex]ds = \left\| \gamma'(t) \right\| dt = \sqrt{t^2 + 1 + 1 /t^2} dt[/itex]

Now, the arc length. [itex]\ell = \int_\gamma ds = \int_1^4 \sqrt{t^2 + 1 + 1 /t^2}dt[/itex].

But that's where the fun ends. I've tried a bunch of trig substitutions (e.g. [itex]t=\tan u[/itex]), to no avail.

I also tried Wolfram online integrator, which returned a mess of symbols -- this problem should have a (reasonably) simple analytic solution.

Any ideas, anyone? I'd really appreciate any help!
 
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Didn't you notice that [itex]t^2+ 1+ 1/t^2= t^2+ 2+ 1/t^2- 1= (t+ 1/t)^2- 1[/itex]?
 
HallsofIvy said:
Didn't you notice that [itex]t^2+ 1+ 1/t^2= t^2+ 2+ 1/t^2- 1= (t+ 1/t)^2- 1[/itex]?

I had, but didn't realize it would help. I'll play around and see what I can come up with. :)

Thankyou for the quick response!
 

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