2/7/2012 9:15:58 PM
2/7/2012 9:16:00 PM
2/7/2012 9:16:29 PM
2/7/2012 9:17:09 PM
2/7/2012 9:17:19 PM
2/7/2012 9:18:02 PM
2/7/2012 9:20:29 PM
2/7/2012 9:21:20 PM
2/7/2012 9:21:27 PM
2/7/2012 9:22:06 PM
2/7/2012 9:28:20 PM
2/7/2012 9:33:06 PM
2/7/2012 9:34:07 PM
2/7/2012 9:35:28 PM
2/7/2012 9:35:55 PM
sup keeler?
2/7/2012 9:36:29 PM
2/7/2012 9:36:32 PM
2/7/2012 9:37:07 PM
2/7/2012 9:37:20 PM
2/7/2012 9:38:38 PM
2/7/2012 9:39:01 PM
2/7/2012 9:39:10 PM
2/7/2012 9:39:22 PM
2/7/2012 9:41:02 PM
2/7/2012 9:41:29 PM
2/7/2012 9:41:44 PM
2/7/2012 9:42:44 PM
2/7/2012 9:43:10 PM
2/7/2012 9:43:44 PM
2/7/2012 9:44:58 PM
2/7/2012 9:45:06 PM
mistergreen, you mad?
2/7/2012 9:47:37 PM
2/7/2012 9:48:19 PM
2/7/2012 9:49:30 PM
2/7/2012 9:49:45 PM
2/7/2012 9:55:11 PM
2/7/2012 9:56:16 PM
BUBBLE BOB
2/7/2012 9:56:30 PM
Before my long spiel, I should mention that the part on your work after you started using u' and du' is wrong: The antiderivative of e^f(E), where f(E) is some arbitrary function of E, is not generally (1/f'(E))e^f(E), even though it is true that the antiderivative of f'(E)e^f(E) is e^f(E).First consider the transformation E=x^2/2.29; then the limits remain the same, 1.036E=(518/1145)x^2, sinh(sqrt(2.29E))=sinh(x), and 0.453E dE=(453/1145)x^2 dx.Then the integral becomes the integral from 0 to +infinity of (453/1145)x^2*e^(-(518/1145)x^2)*sinh(x) dx.--------Begin Failed Solution Attempt--------Then in integration by parts, let u=sinh(x) and dv=(453/1145)x^2*e^(-(518/1145)x^2) dx.Then du=cosh(x), and to find v, do another integration by parts, letting U=x and dV=(453/1145)x*e^(-(518/1145)x^2) dx.Then dU=dx and V=-(453/1036)e^(-(518/1145)x^2).Therefore, v=-(453/1036)x*e^(-(518/1145)x^2)+(453/1036)Int(e^(-(518/1145)t^2) dt,0,x).Then our original integral is lim(uv,x->+inf)-(uv)(0)-Int(v du,0,+inf), so keeping in mind that u=(1/2)e^x-(1/2)e^-x......hmm, I see a problem, it looks like one of the terms will go off to infinity!Notice that one term will be sinh(x)*(453/1036)Int(e^(-(518/1145)t^2) dt,0,x), in the limit as x->+inf; by the relationship at the top, the right factor becomes a finite positive number, but the left factor becomes infinite.This must mean that I have a problem with my method, because as you can imagine, sinh(k*sqrt(E)) for constant k grows asymptotically as quickly as e^sqrt(E), which is more slowly than e^(-1.036E) reaches 0; then their product reaches 0 as quickly as e^-E, which is faster than E grows, in fact so quickly that the whole integrand also reaches 0 in exponential time, so the integral should be finite.--------End Failed Solution Attempt--------Let's go back to the step where u=sinh(x) and dv=(453/1145)x^2*e^(-(518/1145)x^2) dx; instead let's try u=x*sinh(x) and dv=(453/1145)x*e^(-(518/1145)x^2) dx.Then du=sinh(x)+x*cosh(x) dx and v=-(453/1036)e^(-(518/1145)x^2).Then the antiderivative is -(453/1036)x*sinh(x)e^(-(518/1145)x^2)+(453/1036)int(sinh(t)e^(-(518/1145)t^2)+t*cosh(t)e^(-(518/1145)t^2),0,x).Now for the first term in that "int"-egral...letting U=e^(-(518/1145)t^2) and dV=sinh(t) dt, dU=-(1036/1145)t*e^(-(518/1145)t^2) dt and V=cosh(t), so the antiderivative becomes cosh(x)e^(-(518/1145)x^2)+(1036/1145)int(t*cosh(t)e^(-(518/1145)t^2) dt,0,x).Now for the second term in that same "int"-egral...letting w=cosh(t) and dz=t*e^(-(518/1145)t^2) dt, dw=sinh(t) dt and z=-(1145/1036)e^(-(518/1145)t^2), so the antiderivative becomes -(1145/1036)cosh(x)e^(-(518/1145)x^2)+(1145/1036)int(sinh(t)e^(-(518/1145)t^2) dt,0,x).If we denote 1036/1145 by k, then the second sentence means "so the antiderivative becomes -(1/k)cosh(x)e^(-(k/2)t^2)+(1/k)int(sinh(t)e^(-(k/2)t^2) dt,0,x)" and the first sentence means "so the antiderivative becomes cosh(x)e^(-(k/2)x^2)+k*int(t*cosh(t)e^(-(k/2)t^2) dt,0,x)" (to make it all cleaner).Now there is one more integration by parts to do; if W=cosh(t) and dZ=t*e^(-(k/2)t^2) dt, then dW=sinh(t) dt and Z=-(1/k)e^(-(k/2)t^2), so that integral becomes -(1/k)cosh(x)e^(-(k/2)x^2)+(1/k)int(sinh(t)e^(-(k/2)t^2) dt,0,x).Substituting back, some terms cancel out in "the first sentence" to yield just the innermost integral, int(sinh(t)e^(-(k/2)t^2) dt,0,x); then adding that to "the second sentence" yields the entire expression in that "int"-egral that I referred to earlier: -(1/k)cosh(x)e^(-(k/2)t^2)+(1+1/k)int(sinh(t)e^(-(k/2)t^2) dt,0,x).Now wrapping up all the integrations by parts and back-substitutions so far, the antiderivative is-(453/1036)x*sinh(x)e^(-(k/2)x^2)-(1/k)cosh(x)e^(-(k/2)t^2)+(1+1/k)int(sinh(t)e^(-(k/2)t^2) dt,0,x); this last unresolved integral does not appear amenable to integration by parts, and I don't quite know how to attack it, but when you evaluate the limit as x->+inf, that becomes finite. As for the two terms outside the integral, a similar asymptotic analysis shows that they go to 0 as x approaches 0 or +inf, so really what you're left with is (1+1/k)int(sinh(x)e^(-(k/2)x^2) dx,0,+inf), whatever that is.I'm Krallum and I approved this message.
2/7/2012 10:19:58 PM
2/8/2012 12:02:26 AM
2/8/2012 12:06:03 AM
Good jam Greenie
2/8/2012 12:06:53 AM
what's up guise
2/8/2012 12:09:41 AM
Just got done jammin wit some kewl peeps
2/8/2012 12:10:56 AM
2/8/2012 12:11:16 AM
2/8/2012 12:11:48 AM
2/8/2012 12:11:59 AM
2/8/2012 12:12:38 AM
2/8/2012 12:12:42 AM