Let (x, y) be a point on the unit hyperbola x² - y² = 1 in the first quadrant. Define the hyperbolic sector of this point to be the region bounded by the x-axis, the unit hyperbola, and the line segment from (0, 0) to (x, y). The hyperbolic angle α may then be defined as twice the area of the hyperbolic sector. Now, note that the area of the hyperbolic sector is the area of the right triangle with vertices (0, 0), (x, 0), and (x, y) minus the area under the hyperbola from 1 to x. The top half of the hyperbola is given by y=√(x²-1). So the hyperbolic angle α is:
α = xy - 2 [1, x]∫√(t² - 1) dt
Solving the integral, we make the substitution u=arcsec (t), so that sec u = t. Then dt = sec u tan u du. Note that when t=1, u=0 and when when t=x, u=arcsec x, so we have:
α = xy - 2 [0, arcsec (x)]∫√(sec² u - 1) sec u tan u du
Simplifying this integral:
α = xy - 2 [0, arcsec (x)]∫√(tan² u) sec u tan u du
α = xy - 2 [0, arcsec (x)]∫sec u tan² u du (since tan u is positive)
Now, in order to find [0, arcsec (x)]∫sec u tan² u du, we break this off from the main problem and integrate by parts -- let v = tan u and dw = sec u tan u du. Then dv = sec² u du and w = sec u. So we have:
[0, arcsec (x)]∫sec u tan² u du = sec u tan u|[0, arcsec x] - [0, arcsec x]∫sec³ u du
[0, arcsec (x)]∫sec u tan² u du = x tan (arcsec x) - [0, arcsec x]∫sec u (1+tan² u) du
[0, arcsec (x)]∫sec u tan² u du = x √(sec² (arcsec x) - 1) - [0, arcsec x]∫sec u du - [0, arcsec x]∫sec u tan² u du
[0, arcsec (x)]∫sec u tan² u du = x √(x² - 1) - [0, arcsec x]∫sec u du - [0, arcsec x]∫sec u tan² u du
Adding [0, arcsec x]∫sec u tan² u du to both sides:
2 [0, arcsec (x)]∫sec u tan² u du = x √(x² - 1) - [0, arcsec x]∫sec u du
So substituting this into the original equation:
α = xy - x √(x² - 1) + [0, arcsec x]∫sec u du
But note that y=√(x²-1):
α = xy - xy + [0, arcsec x]∫sec u du
α = [0, arcsec x]∫sec u du
Now make the substitution v = sec u + tan u, dv = sec u tan u + sec² u du = v sec u du. Note that when u=0, v=1, and when u=arcsec x, v = x + tan (arcsec x) = x + √(sec² (arcsec x) - 1) = x + √(x² - 1). So we have:
α = [1, x + √(x² - 1)]∫1/v dv
α = ln v | [1, x + √(x² - 1)]
α = ln (x + √(x² - 1)) - ln 1
α = ln (x + √(x² - 1))
From this we may derive an expression for x in terms of the hyperbolic angle α. By exponentiating this equation, we obtain:
e^α = x + √(x² - 1)
Squaring:
e^(2α) = x² + 2x√(x² - 1) + x² - 1
e^(2α) = 2x(x + √(x² - 1)) - 1
But note that e^α = x + √(x² - 1), so we have:
e^(2α) = 2xe^α - 1
Dividing by e^α and simplifying:
e^α = 2x - e^(-α)
2x = e^α + e^(-α)
x = (e^α + e^(-α))/2
If we want a similar expression for y, we may simply note that:
y
= √(x² - 1)
= √(((e^α + e^(-α))/2)² - 1)
= √((e^(2α) + 2 + e^(-2α))/4 - 1)
= √((e^(2α) - 2 + e^(-2α))/4)
= (e^α - e^(-α))/2
So, if we define cosh α to the the x-coordinate of a point that subtends a hyperbolic angle α and sinh α to be the y-coordinate of the same, the above serves as a proof that cosh α = (e^α + e^(-α))/2 and sinh α = (e^α - e^(-α))/2.
There is also a rather interesting article on the history of the hyperbolic functions here: http://ww2.hyperbolicsliderules.com:8110/Documents/Article_12042006.doc (MS word format).
2007-12-07 02:28:16
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answer #1
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answered by Pascal 7
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The gist of the discussion out there (sorry, there are too many pages to provide all the links) is that wands help to focus the magic resident in the witch or wizard, but wandless magic is still possible, particularly for very talented people like Snape and Dumbledore. Some examples ... Apparition Assuming one's Animagus form (or Metamorphpagus) Accio (the Summoning Charm) Elves can do magic without using wands Lumos
2016-05-21 23:52:34
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answer #2
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answered by ? 3
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Im looking for a proof of the derivative of the trig functions... FROM WHICH I can derive cosh x = [ e^x + e^-x ] / 2 Can anyone help with this?
Assume cos(ix), or e^ix can be written in complex form as A(x)+iB(x), Where A and B are real value functions.
Lets find cos(ix),
Assuming cos(ix) is continuous, We have
cos(ix)=A+iB
-isin(ix)=A'+iB'
cos(ix)=A"+iB"
Equating coefficients we have A=A", B=B" => A=C1e^x+C2e^-x, B=iC3e^x+iC4e^-4
So
I. cos(ix) = C1e^x+C2e^-x+iC3e^x+iC4e^-x
II. isin(ix) = C1e^x-C2e^-x+iC3e^x-iC4e^-x
Evaluating equations 1 and II at x=0
I. cos(i0) = 1= C1+C2+iC3 + iC4
II. isin(i0) = 0 =C1 -C2+iC3 - iC4
Once again equating coefficients:
C1+C2=1, C1-C2=0 => C1=C2=1/2
C3+C4=0, C3-C4=0 => C3=C4=0
Hence cos(ix)=(e^x+e^-x)/2.
One can derive the representation of e^(ix) in polar form following the same approach as cos(ix). Here you find A=-A" and B=-B". Both solutions for A and B requires recognition of the behavior of the nth derivative of sin(x) and cos(x). You'll find A=C1cos(x)+C2sin(x) B= C3cos(x)+C4sin(x).
e^ix=C1cos(x)+C2sin(x) +iC3cos(x) + iC4sin(x)
ie^ix=-C1sin(x)+C2cos(x) -iC3sin(x) + iC4cos(x)
Applying BC's for e^ix, and ie^x at (x=0)
e^0=1=C1(1)+C2(0)+iC3(1) +iC4(0)
ie^ix=i=-C1(0)+C2 -iC3(0) + iC4(1)
Hence C1=1,C2=0, C3=0, C4=1
e^ix=cos(x)+isin(x)
2017-03-05 19:50:43
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answer #3
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answered by Democracy for all 1
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http://answers.yahoo.com/question/index;_ylt=AmhY7dqfsAoz1cVX8JXRcHQCxgt.;_ylv=3?qid=20071124172533AALL0mt
♠ noli audis ergo noli cogitas;
♣ well exp(jb) = cos(b) +j*sin(b) right?
exp(x) = exp(j*(-jx)) = cos(jx) –j*sin(jx);
exp(-x) = exp(j*jx) = cos(jx) +j*sin(jx);
♦ exp(x) + exp(-x) =2cos(jx), hence
cos(jx) =(exp(x) + exp(-x))/2,
which was named as ch(x);
2007-12-07 01:58:23
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answer #5
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answered by Anonymous
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