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University of Utah Advanced Electromagnetics Green’s Function Dr. Sai Ananthanarayanan University of Utah Department of Electrical and Computer Engineering www.ece.utah.edu/~psai 1
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2 Green’s Function
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3 T is the uniform tensile force of the string The string is stationary at the ends, the displacement satisfies the boundary condition
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4 Green’s Function Lets first assume that the load applied to the string is concentrated at a point x=x’ Once G(x,x’) is found the displacement u(x) can be obtained by convolving the load F(x) with the green’s function
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5 Green’s Function Away from the load at x=x’ the differential equation reduces to the homogeneous form: which has solution of the form
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6 Green’s Function Applying the boundary condition A 1 and A 2 are to be determined
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7 Green’s Function At x=x’ the displacement of the string must be continuous And hence Green’s function must be continuous at x=x’
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8 Green’s Function Substituting
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9 Green’s Function
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11 Solution
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13 Closed Form Solution The homogeneous differential equation reduces to:
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14 Closed Form Solution Wronskian:
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15 Series Form Solution
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16 Series Form Solution The amplitude B is such that
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17 Series Form Solution
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18 Series Form Solution
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19 2D Green’s Function Static Fields
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20 2D Green’s Function Static Fields
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21 Closed Form Solution Representing the Green’s function by normalized single function Fourier series of sine functions that satisfy the BC: Substituting into the equation below
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22 Closed Form Solution And applying
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23 Closed Form Solution For Homogeneous case with solutions
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