∫ 0 ∞ 2 π x 3 θ exp ( − 2 μ 2 x θ ( x − μ ) 2 ) d x = 1 , for μ > 0 and θ > 0 . Then determine ∫ 0 ∞ π x exp ( 1 − 4 x − x 1 ) d x .
Given that
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What about integration by parts and by analogy theta is 2 and mu is 2 hence the integral becomes x power 0.5 then it may be rewritten as x^2 times the dv and the integral rule is simply UV- integral of V d(x^2) Hence again integration of x timed dv I think this is direct technique
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1-preform differentiation under the integral sign for f(x) with respect to Mu
integration { a x f(x)} + integration { b f(x)} = 0 where a and b are Constance .............> equ 1
therefore @ Theta and Mu = 2 the integration of {x f(x) }=2 .............> equ 2
2- again preform differentiation under the integral sign for equation 1 with respect to Mu
integration { l x^2 f(x)} +integration { m x f(x)} + integration { n f(x)} = 0 where l,m and n are Constance .............> equ 3
therefore @ Theta and Mu = 2 and by substituting from equation 2 in equation 3 the integration of {x^2 f(x) }=8 .