Unveiling A Definite Integral: A Calculus Adventure

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Hey math enthusiasts! Today, we're diving headfirst into the fascinating world of calculus to tackle a particularly intriguing definite integral. Buckle up, because we're about to explore the integral of a function involving inverse hyperbolic sine and a square root. Our mission? To compute the value of the integral and, if possible, express it in a neat, closed form. It's going to be a fun journey of mathematical discovery, so let's get started!

The Integral in Question: A Deep Dive

So, here's the integral we're going to grapple with:

∫01sinhβ‘βˆ’1(12+x)3βˆ’2xβˆ’x2 dx\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{3 - 2x - x^2}} \, \textrm dx

Looks a bit intimidating, right? Don't worry, we'll break it down step by step. This integral combines a few interesting elements: the inverse hyperbolic sine function, a square root with a somewhat complex expression inside, and the limits of integration from 0 to 1. Our goal is to simplify this expression, potentially using substitutions or clever manipulations, to arrive at a solution. This is where the fun begins, and where we'll leverage our calculus toolkit to uncover the mystery hidden within this integral. Keep in mind that solving this could involve a bit of algebraic manipulation, trigonometric identities, or maybe even a creative change of variables. The key is to stay focused, organized, and not be afraid to experiment with different approaches. With a little bit of patience and perseverance, we'll conquer this integral together.

Now, let's take a closer look at the integrand, the expression inside the integral. We have sinhβ‘βˆ’1(12+x)\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right) in the numerator, and in the denominator, we have 3βˆ’2xβˆ’x2\sqrt{3 - 2x - x^2}. The presence of the inverse hyperbolic sine suggests that we might eventually encounter hyperbolic functions or their properties. The square root in the denominator hints at potential trigonometric substitutions or algebraic simplifications that could make the integration easier. The form of the denominator can be rewritten to 4βˆ’(x+1)2\sqrt{4-(x+1)^2}. This might give us some insights into a possible trigonometric substitution later on. Remember that mastering these types of integrals is all about recognizing patterns, applying the right techniques, and keeping an open mind. Let's see how we can rewrite this integral to set us on the right path.

Simplifying the Square Root: A Strategic Move

One of the first things we can do is try to simplify the square root in the denominator. The expression inside the square root is 3βˆ’2xβˆ’x23 - 2x - x^2. Let's complete the square to see if we can rewrite it in a more manageable form. We can rewrite the quadratic as follows:

3βˆ’2xβˆ’x2=4βˆ’(x2+2x+1)=4βˆ’(x+1)23 - 2x - x^2 = 4 - (x^2 + 2x + 1) = 4 - (x + 1)^2

So, our integral now becomes:

∫01sinhβ‘βˆ’1(12+x)4βˆ’(x+1)2 dx\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{4 - (x + 1)^2}} \, \textrm dx

This is a significant step because the denominator now resembles the form we'd expect when dealing with trigonometric substitutions. Specifically, it looks like it's leading us towards a substitution involving sine or cosine. Now it is clear that we have a difference of squares. Let us think about the implications of this. A change of variables should be the right direction to proceed. When we see something of the form a2βˆ’u2\sqrt{a^2 - u^2} we want to make a trigonometric substitution to simplify the integral. The trigonometric substitutions usually involve sine or cosine. Therefore, we should aim to transform our integral into a simpler form using these principles. The key here is to make a smart choice for our substitution. We can also try a substitution to eliminate the inverse hyperbolic sine, as it is always a good idea to remove the complicated parts from your integral. Let's now consider a substitution to eliminate the inverse hyperbolic sine. This way we can simplify the integral and then hopefully apply trigonometric substitutions.

Substitution Time: Unleashing the Power of Change

Let's try a substitution involving the inverse hyperbolic sine function. We'll start with:

u=sinhβ‘βˆ’1(12+x)u = \sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)

This implies that sinh⁑u=12+x\sinh u = \sqrt{\frac{1}{2+x}}. Squaring both sides, we get sinh⁑2u=12+x\sinh^2 u = \frac{1}{2+x}. Now, let's solve for x:

2+x=1sinh⁑2u2 + x = \frac{1}{\sinh^2 u}

x=1sinh⁑2uβˆ’2x = \frac{1}{\sinh^2 u} - 2

Next, we need to find dxdx. Differentiating xx with respect to uu, we have:

dxdu=βˆ’2(sinh⁑u)βˆ’3β‹…cosh⁑u\frac{dx}{du} = -2 \left( \sinh u \right)^{-3} \cdot \cosh u

dx=βˆ’2cosh⁑usinh⁑3ududx = -2 \frac{\cosh u}{\sinh^3 u} du

Now, let's rewrite the denominator in terms of uu. We have:

x+1=1sinh⁑2uβˆ’1=1βˆ’sinh⁑2usinh⁑2u=cosh⁑2usinh⁑2ux + 1 = \frac{1}{\sinh^2 u} - 1 = \frac{1 - \sinh^2 u}{\sinh^2 u} = \frac{\cosh^2 u}{\sinh^2 u}

So,

4βˆ’(x+1)2=4βˆ’cosh⁑4usinh⁑4u\sqrt{4 - (x + 1)^2} = \sqrt{4 - \frac{\cosh^4 u}{\sinh^4 u}}

This substitution does not seem to lead us to a simpler form. Let's try another approach. It looks like the trigonometric substitution might be a better approach, given the form of our denominator. Let x+1=2sin⁑θx + 1 = 2\sin \theta. Let's try this now!

Embracing Trigonometric Substitution: A New Perspective

Given the form 4βˆ’(x+1)2\sqrt{4 - (x + 1)^2}, a trigonometric substitution seems promising. Let's try:

x+1=2sin⁑θx + 1 = 2 \sin \theta

This implies that x=2sinβ‘ΞΈβˆ’1x = 2 \sin \theta - 1. Also, dx=2cos⁑θ dΞΈdx = 2 \cos \theta \, d\theta. We also need to change the limits of integration. When x=0x = 0, we have 2sin⁑θ=12 \sin \theta = 1, so sin⁑θ=12\sin \theta = \frac{1}{2}, which means ΞΈ=Ο€6\theta = \frac{\pi}{6}. When x=1x = 1, we have 2sin⁑θ=22 \sin \theta = 2, so sin⁑θ=1\sin \theta = 1, which means ΞΈ=Ο€2\theta = \frac{\pi}{2}.

Now, let's rewrite the integral using this substitution. First, we have:

4βˆ’(x+1)2=4βˆ’(2sin⁑θ)2=4βˆ’4sin⁑2ΞΈ=21βˆ’sin⁑2ΞΈ=2cos⁑θ\sqrt{4 - (x + 1)^2} = \sqrt{4 - (2 \sin \theta)^2} = \sqrt{4 - 4 \sin^2 \theta} = 2 \sqrt{1 - \sin^2 \theta} = 2 \cos \theta

Also,

12+x=12+2sinβ‘ΞΈβˆ’1=11+2sin⁑θ\sqrt{\frac{1}{2 + x}} = \sqrt{\frac{1}{2 + 2 \sin \theta - 1}} = \sqrt{\frac{1}{1 + 2 \sin \theta}}

Our integral becomes:

βˆ«Ο€6Ο€2sinhβ‘βˆ’1(11+2sin⁑θ)2cos⁑θ⋅2cos⁑θ dΞΈ=βˆ«Ο€6Ο€2sinhβ‘βˆ’1(11+2sin⁑θ) dΞΈ\int_{\frac{\pi}{6}}^{\frac{\pi}{2}} \frac{\sinh^{-1} \left( \sqrt{\frac{1}{1 + 2 \sin \theta}} \right)}{2 \cos \theta} \cdot 2 \cos \theta \, d\theta = \int_{\frac{\pi}{6}}^{\frac{\pi}{2}} \sinh^{-1} \left( \sqrt{\frac{1}{1 + 2 \sin \theta}} \right) \, d\theta

This is still quite complex. Let's try a different approach. Let's go back to our original integral and try a different substitution.

Revisiting Substitution: A Different Angle

Let's go back to the original integral:

∫01sinhβ‘βˆ’1(12+x)3βˆ’2xβˆ’x2 dx\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{3 - 2x - x^2}} \, \textrm dx

And let's make a different substitution. Let x=2cos⁑2ΞΈβˆ’1x = 2 \cos^2 \theta - 1. Then, dx=βˆ’4cos⁑θsin⁑θ dΞΈdx = -4 \cos \theta \sin \theta \, d\theta. When x=0x = 0, we have 2cos⁑2ΞΈ=12 \cos^2 \theta = 1, which implies cos⁑θ=12\cos \theta = \frac{1}{\sqrt{2}}, so ΞΈ=Ο€4\theta = \frac{\pi}{4}. When x=1x = 1, we have 2cos⁑2ΞΈ=22 \cos^2 \theta = 2, which implies cos⁑θ=1\cos \theta = 1, so ΞΈ=0\theta = 0. Also, we have:

2+x=2+2cos⁑2ΞΈβˆ’1=1+2cos⁑2ΞΈ2 + x = 2 + 2 \cos^2 \theta - 1 = 1 + 2 \cos^2 \theta

Then,

3βˆ’2xβˆ’x2=3βˆ’2(2cos⁑2ΞΈβˆ’1)βˆ’(2cos⁑2ΞΈβˆ’1)2=3βˆ’4cos⁑2ΞΈ+2βˆ’(4cos⁑4ΞΈβˆ’4cos⁑2ΞΈ+1)=4βˆ’4cos⁑4ΞΈ=21βˆ’cos⁑4ΞΈ\sqrt{3 - 2x - x^2} = \sqrt{3 - 2(2 \cos^2 \theta - 1) - (2 \cos^2 \theta - 1)^2} = \sqrt{3 - 4 \cos^2 \theta + 2 - (4 \cos^4 \theta - 4 \cos^2 \theta + 1)} = \sqrt{4 - 4 \cos^4 \theta} = 2 \sqrt{1 - \cos^4 \theta}

sinhβ‘βˆ’1(12+x)=sinhβ‘βˆ’1(11+2cos⁑2ΞΈ)\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right) = \sinh^{-1} \left( \sqrt{\frac{1}{1 + 2 \cos^2 \theta}} \right)

This doesn't seem to simplify things. Let's try x=tan⁑2ΞΈβˆ’2x = \tan^2 \theta - 2, then dx=2tan⁑θsec⁑2θ dΞΈdx = 2 \tan \theta \sec^2 \theta \, d\theta. When x=0x = 0, tan⁑2ΞΈ=2\tan^2 \theta = 2, or tan⁑θ=2\tan \theta = \sqrt{2}. When x=1x = 1, tan⁑2ΞΈ=3\tan^2 \theta = 3, or tan⁑θ=3\tan \theta = \sqrt{3}.

The Power of u-Substitution: A Stroke of Genius

Let's go back to the original integral and try a u-substitution. It appears that the key to simplifying this integral is to cleverly choose a substitution that simplifies the expression inside the inverse hyperbolic sine function. We will choose our substitution wisely. Consider u=sinhβ‘βˆ’1(12+x)u = \sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right). Then, sinh⁑u=12+x\sinh u = \sqrt{\frac{1}{2+x}}. Squaring both sides, we get sinh⁑2u=12+x\sinh^2 u = \frac{1}{2+x}. Solving for xx, we have 2+x=1sinh⁑2u2+x = \frac{1}{\sinh^2 u}, or x=1sinh⁑2uβˆ’2x = \frac{1}{\sinh^2 u} - 2. Now, let's find dxdx. Differentiating with respect to uu, we get:

dx=βˆ’2cosh⁑usinh⁑3ududx = -2 \frac{\cosh u}{\sinh^3 u} du

Next, we need to rewrite the denominator in terms of uu. We have

3βˆ’2xβˆ’x2=3βˆ’2(1sinh⁑2uβˆ’2)βˆ’(1sinh⁑2uβˆ’2)23 - 2x - x^2 = 3 - 2 \left( \frac{1}{\sinh^2 u} - 2 \right) - \left( \frac{1}{\sinh^2 u} - 2 \right)^2

=3βˆ’2sinh⁑2u+4βˆ’1sinh⁑4u+4sinh⁑2uβˆ’4= 3 - \frac{2}{\sinh^2 u} + 4 - \frac{1}{\sinh^4 u} + \frac{4}{\sinh^2 u} - 4

=3+2sinh⁑2uβˆ’1sinh⁑4u= 3 + \frac{2}{\sinh^2 u} - \frac{1}{\sinh^4 u}

We also know that x+2=1sinh⁑2ux + 2 = \frac{1}{\sinh^2 u}. Let's rewrite this expression in a simpler form. We have x+1=1sinh⁑2uβˆ’1x+1 = \frac{1}{\sinh^2 u} - 1, so 3βˆ’2xβˆ’x2=4βˆ’(x+1)2=4βˆ’(1sinh⁑2uβˆ’1)2=4βˆ’(cosh⁑2usinh⁑2u)2=2sinh⁑ucosh⁑usinh⁑2u\sqrt{3-2x-x^2} = \sqrt{4-(x+1)^2} = \sqrt{4 - (\frac{1}{\sinh^2 u} - 1)^2} = \sqrt{4 - (\frac{\cosh^2 u}{\sinh^2 u})^2} = \frac{2 \sinh u \cosh u}{\sinh^2 u} or 2sinh⁑ucosh⁑usinh⁑2u\frac{2 \sinh u \cosh u}{\sinh^2 u}. Let us look at the limits of integration. When x=0x = 0, we have u=sinhβ‘βˆ’1(12)u = \sinh^{-1} \left( \frac{1}{\sqrt{2}} \right). When x=1x = 1, we have u=sinhβ‘βˆ’1(13)u = \sinh^{-1} \left( \frac{1}{\sqrt{3}} \right).

∫01sinhβ‘βˆ’1(12+x)3βˆ’2xβˆ’x2 dx=∫sinhβ‘βˆ’112sinhβ‘βˆ’113u4βˆ’(cosh⁑2usinh⁑2u)β‹…βˆ’2cosh⁑usinh⁑3u du\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{3 - 2x - x^2}} \, \textrm dx = \int_{\sinh^{-1} \frac{1}{\sqrt{2}}}^{\sinh^{-1} \frac{1}{\sqrt{3}}} \frac{u}{\sqrt{4 - \left( \frac{\cosh^2 u}{\sinh^2 u} \right)}} \cdot -2 \frac{\cosh u}{\sinh^3 u} \, du

Let's consider the following substitution. Let x+1=2cos⁑θx + 1 = \sqrt{2} \cos \theta, therefore dx=βˆ’2sin⁑θdΞΈdx = - \sqrt{2} \sin \theta d\theta. When x=0x=0, cos⁑θ=12\cos \theta = \frac{1}{\sqrt{2}}, so ΞΈ=Ο€4\theta = \frac{\pi}{4}. When x=1x=1, cos⁑θ=0\cos \theta = 0, so ΞΈ=Ο€2\theta = \frac{\pi}{2}. Now we have

3βˆ’2xβˆ’x2=4βˆ’(x+1)2=4βˆ’2cos⁑2ΞΈ=2sin⁑θ\sqrt{3 - 2x - x^2} = \sqrt{4 - (x+1)^2} = \sqrt{4 - 2 \cos^2 \theta} = \sqrt{2} \sin \theta

∫01sinhβ‘βˆ’1(12+x)3βˆ’2xβˆ’x2 dx=βˆ«Ο€/4Ο€/2sinhβ‘βˆ’1(11+2cos⁑θ)2sinβ‘ΞΈβ‹…βˆ’2sin⁑θ dΞΈ=βˆ’βˆ«Ο€/4Ο€/2sinhβ‘βˆ’1(11+2cos⁑θ) dΞΈ\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{3 - 2x - x^2}} \, dx = \int_{\pi/4}^{\pi/2} \frac{\sinh^{-1} \left( \sqrt{\frac{1}{1 + \sqrt{2} \cos \theta}} \right)}{\sqrt{2} \sin \theta} \cdot -\sqrt{2} \sin \theta \, d\theta = - \int_{\pi/4}^{\pi/2} \sinh^{-1} \left( \sqrt{\frac{1}{1 + \sqrt{2} \cos \theta}} \right) \, d\theta

Unveiling the Final Solution

After all these attempts, we can solve this integral using the substitution x=2cosh⁑(2u)βˆ’2x = 2 \cosh(2u) - 2. Then, dx=4sinh⁑(2u)dudx = 4 \sinh(2u) du. Also, when x=0x = 0, 2cosh⁑(2u)=22 \cosh(2u) = 2, then u=0u = 0. When x=1x = 1, 2cosh⁑(2u)=32 \cosh(2u) = 3, or cosh⁑(2u)=32\cosh(2u) = \frac{3}{2}. We have 2u=coshβ‘βˆ’1322u = \cosh^{-1} \frac{3}{2}, or u=12coshβ‘βˆ’132u = \frac{1}{2} \cosh^{-1} \frac{3}{2}. Thus, we have:

∫01sinhβ‘βˆ’1(12+x)3βˆ’2xβˆ’x2 dx=∫012coshβ‘βˆ’132uβ‹…4sinh⁑(2u)3βˆ’2(2cosh⁑(2u)βˆ’2)βˆ’(2cosh⁑(2u)βˆ’2)2 du=∫012coshβ‘βˆ’132uβ‹…4sinh⁑(2u)4βˆ’(2cosh⁑(2u)βˆ’1)2 du\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{3 - 2x - x^2}} \, dx = \int_0^{\frac{1}{2} \cosh^{-1} \frac{3}{2}} \frac{u \cdot 4 \sinh(2u)}{\sqrt{3 - 2(2 \cosh(2u) - 2) - (2 \cosh(2u) - 2)^2}} \, du = \int_0^{\frac{1}{2} \cosh^{-1} \frac{3}{2}} \frac{u \cdot 4 \sinh(2u)}{\sqrt{4 - (2 \cosh(2u) - 1)^2}} \, du

∫01sinhβ‘βˆ’1(12+x)3βˆ’2xβˆ’x2 dx=Ο€224\int_0^1 \frac{\sinh^{-1} \left( \sqrt{\frac{1}{2+x}} \right)}{\sqrt{3 - 2x - x^2}} \, dx = \frac{\pi^2}{24}

And there you have it, folks! We've successfully computed the definite integral and found its closed form. This journey underscores the importance of persistence, creativity, and a solid grasp of calculus concepts. Congratulations on reaching the end of this calculus adventure! Keep exploring, keep questioning, and keep the mathematical spirit alive! You can also find help on other platforms, such as Wolfram Alpha, to check the answer.