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REALLY hard integral?

Seriously.

y^2 = 4x

Find the arc length of this curve for y within [0,2]

I tried so many approaches... I know the formula, but I've gotten to integral[0,2](sqrt((1/4)+y^2)), and I've already tried trig substitution. I got 1.161695941, but that's apparently not right, according to my online homework system...

Update:

Just in case anyone needs it, and they probably will, I've figured out the indefinite integral of sec^3(theta) before, and it is:

(1/2)[sec(theta)tan(theta)+ln|sec(theta)+tan(theta)|]+C

Update 2:

That cut off...

(1/2)[sec(theta)tan(theta)]

+

(1/2)ln|sec(theta)+tan(theta)|+C

Update 3:

Never mind, I got the answer by developing a calculator program to solve integrals like this, and the answer (only in decimal form, since it's a TI-83) is 2.295587149. Now I just need to know how to do it...

Scratch that, I figured it out.

Update 4:

In that case, I might as well write out how I did the problem! :D

Arc Length = integral[0,2](sqrt(1+(y^2/4)))

= integral[0,2]((1/2)*sqrt(4+y^2))),

y = 2tan(theta)

dy = 2sec^2(theta)dtheta

sqrt(4+y^2) = 2sec(theta)

= (1/2)*integral[0,2](2sec(theta)

*2sec^2(theta)dtheta)

= 2*integral[0,2](sec^3(theta)dtheta)

Haha, now this is hard...

= 2((1/2)[sec(theta)tan(theta)]+

(1/2)ln|sec(theta)+tan(theta)|)

= {[sec(theta)tan(theta)]+

ln|sec(theta)+tan(theta)|}

eval @ [0,2]

And from there, that's the answer. :D Wow, it's so epic it's cutting off without linebreaks.

3 Answers

Relevance
  • 9 years ago
    Favorite Answer

    s = ∫ ds = ∫[0,2] √(1 + (dx/dy)²) dy = ∫[0,2] √(1 + (y/2)²) dy

    u = y/2 ⇒ u(0) = 0, u(2) = 1

    du = dy/2

    2 ∫[0,1] √(1 + u²) du

    And I'm betting you can take it from there. It's always best to get rid of fractions whenever possible. They're your friends, but sometimes you just want to be alone.

  • Nick
    Lv 6
    9 years ago

    LOOK AGAIN, I JUST EDITED MY ANSWER, MADE A STUPID CALCULATION ERROR.

    Have you tried substituting hyperbolic sine:

    ds = (1 + (dx/dy)^2)^(1/2) dy (1)

    dx/dy = y/2

    ds = (1 + (y/2)^2)^(1/2) dy (2)

    y/2 = sinh(u) => dy/du = 2cosh(u):

    ds = (1 + sinh^2(u))^(1/2) 2cosh(u) du

    use the hyperbolic identity cosh^2(u) - sinh^2(u) = 1 to give:

    ds = 2cosh^2(u) du

    also there is another hyperbolic identity 2cosh^2(u) = cosh(2u) + 1:

    ds = (cosh(2u) + 1) du

    The limits are found since u = arsinh(y/2) = ln((y/2) + ((y/2)^2 + 1)^(1/2)), so for y=0 u=0 and for y=2 u=ln(1 + (2)^(1/2)) = 0.881.

    Int(ds) = [(1/2)sinh(2u) + u]_0^0.881

    arc length = Ds = 2.294

    All the identities and information of hyperbolic functions is here:

    http://en.wikipedia.org/wiki/Hyperbolic_function

  • y^2 = 4x

    2y * dy = 4 * dx

    dy/dx = 2/y

    (dy/dx)^2 = 4/y^2

    (dy/dx)^2 = 4/(4x)

    (dy/dx)^2 = 1/x

    sqrt(1 + (dy/dx)^2) * dx =>

    sqrt(1 + (1/x)) * dx =>

    sqrt(1 + x) * dx / sqrt(x)

    x = tan(t)^2

    dx = 2 * tan(t) * sec(t)^2 * dt

    sqrt(1 + tan(t)^2) * 2 * tan(t) * sec(t)^2 * dt / sqrt(tan(t)^2) =>

    sqrt(sec(t)^2) * 2 * tan(t) * sec(t)^2 * dt / tan(t) =>

    sec(t) * 2 * sec(t)^2 * dt =>

    2 * sec(t)^3 * dt

    Integrate

    2 * (1/2) * (sec(t) * tan(t) + ln|sec(t) + tan(t)|) + C =>

    sec(t) * tan(t) + ln|sec(t) + tan(t)|

    x = tan(t)^2

    0 = tan(t)^2

    tan(t) = 0

    sec(t) = sqrt(1 + tan(t)^2) = 1

    2 = tan(t)^2

    tan(t) = sqrt(2)

    sec(t) = sqrt(1 + tan(t)^2) = sqrt(1 + 2) = sqrt(3)

    sec(t) * tan(t) + ln|sec(t) + tan(t)|

    (sqrt(3) * sqrt(2) + ln|sqrt(3) + sqrt(2)|) - (1 * 0 + ln|1 + 0|) =>

    sqrt(6) + ln|sqrt(2) + sqrt(3)| - 0 =>

    sqrt(6) + ln|sqrt(2) + sqrt(3)| =>

    3.5957055775637669420976777303799

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