Prove the following!!!
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Answered by
0
This is an old favorite of mine.
Define
I=∫
+∞
−∞
e−x2dx
Then
I2=(∫
+∞
−∞
e−x2dx)(∫
+∞
−∞
e−y2dy)
I2=∫
+∞
−∞
∫
+∞
−∞
e−(x2+y2)dxdy
Now change to polar coordinates
I2=∫
+2π
0
∫
+∞
0
e−r2rdrdθ
The θ integral just gives 2π, while the r integral succumbs to the substitution u=r2
I2=2π∫
+∞
0
e−udu/2=π
So
I=
√
π
and your integral is half this by symmetry
I have always wondered if somebody found it this way, or did it first using complex variables and noticed this would work.
Answered by
4
Answer:
hi
Step-by-step explanation:
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