Complex Form of the Fourier Series. a. Using the Euler formula e i θ = cos θ + i sin θ , i = − 1 , prove that cos n x = e i n x + e − i n x 2 and sin n x = e i n x − e − i n x 2 i . b. Show that the Fourier series f ( x ) ∼ a 0 2 + ∑ n = 1 ∞ { a n cos n x + b n sin n x } = c 0 + ∑ n = 1 ∞ { c n e i n x + c − n e − i n x } , where c 0 = a 0 2 , c n = a n − i b n 2 , c − n = a n + i b n 2 . c. Finally, use the results of part (b) to show that f ( x ) ∼ ∑ n = − ∞ ∞ c n e i n x , − π < x < π where c n = 1 2 π ∫ − π π f ( x ) e − i n x d x .
Complex Form of the Fourier Series. a. Using the Euler formula e i θ = cos θ + i sin θ , i = − 1 , prove that cos n x = e i n x + e − i n x 2 and sin n x = e i n x − e − i n x 2 i . b. Show that the Fourier series f ( x ) ∼ a 0 2 + ∑ n = 1 ∞ { a n cos n x + b n sin n x } = c 0 + ∑ n = 1 ∞ { c n e i n x + c − n e − i n x } , where c 0 = a 0 2 , c n = a n − i b n 2 , c − n = a n + i b n 2 . c. Finally, use the results of part (b) to show that f ( x ) ∼ ∑ n = − ∞ ∞ c n e i n x , − π < x < π where c n = 1 2 π ∫ − π π f ( x ) e − i n x d x .
Solution Summary: The author explains how the functions mathrmcosnx=einx+
Show that the Laplace equation in Cartesian coordinates:
J²u
J²u
+
= 0
მx2 Jy2
can be reduced to the following form in cylindrical polar coordinates:
湯(
ди
1 8²u
+
Or 7,2 მ)2
= 0.
Draw the following graph on the interval
πT
5π
< x <
x≤
2
2
y = 2 cos(3(x-77)) +3
6+
5
4-
3
2
1
/2 -π/3 -π/6
Clear All Draw:
/6 π/3 π/2 2/3 5/6 x 7/6 4/3 3/2 5/311/6 2 13/67/3 5
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Determine the moment about the origin O of the force F4i-3j+5k that acts at a Point A. Assume that the position vector of A is (a) r =2i+3j-4k, (b) r=-8i+6j-10k, (c) r=8i-6j+5k
Chapter 10 Solutions
Fundamentals of Differential Equations and Boundary Value Problems
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