The structure of a football goal is shown in the figure below. The bending motion of the structure can be represented by a flexible cantilever beam with tip mass M¡ as shown in the figure. The tip mass M, represents the mass of the horizontal crossbar which is assumed to be rigid in this motion. A single vertical straight beam having mass of MH, shown in the figure below, is the equivalent model for the two symmetrical vertical posts. A soccer ball of mass M, hits the horizontal crossbar with the velocity of Vp. x(t) м, VINGLI SOLAR The response of the horizontal crossbar, mass M, is shown by x(t) in the figure. The vertical beam has a circular cross section of radius r, Young's modulus E and length L. For numerical calculations, use M, = 23.2130 kg, MH = 28.6617 kg. M, = 0.5497 kg, Vý = 8.8974 m/s, L= 2.7757 m, E = 133.5685 GPa andr= 0.0437 m. For circular cross- section I = Tr/4.Considering zero damping and the numerical data given above, obtain the maximum amplitude of response x(t) after it was hit by soccer ball Mp.

Elements Of Electromagnetics
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The structure of a football goal is shown in the figure below. The bending motion of the
structure can be represented by a flexible cantilever beam with tip mass M¡ as shown
in the figure. The tip mass M, represents the mass of the horizontal crossbar which is
assumed to be rigid in this motion. A single vertical straight beam having mass of MH,
shown in the figure below, is the equivalent model for the two symmetrical vertical
posts. A soccer ball of mass M, hits the horizontal crossbar with the velocity of Vp.
x(t)
м,
VINGLI SOLAR
The response of the horizontal crossbar, mass M, is shown by x(t) in the figure. The
vertical beam has a circular cross section of radius r, Young's modulus E and length L.
For numerical calculations, use M, = 23.2130 kg, MH = 28.6617 kg. M, = 0.5497 kg, Vý
= 8.8974 m/s, L= 2.7757 m, E = 133.5685 GPa andr= 0.0437 m. For circular cross-
section I = Tr/4.Considering zero damping and the numerical data given above,
obtain the maximum amplitude of response x(t) after it was hit by soccer ball Mp.
Transcribed Image Text:The structure of a football goal is shown in the figure below. The bending motion of the structure can be represented by a flexible cantilever beam with tip mass M¡ as shown in the figure. The tip mass M, represents the mass of the horizontal crossbar which is assumed to be rigid in this motion. A single vertical straight beam having mass of MH, shown in the figure below, is the equivalent model for the two symmetrical vertical posts. A soccer ball of mass M, hits the horizontal crossbar with the velocity of Vp. x(t) м, VINGLI SOLAR The response of the horizontal crossbar, mass M, is shown by x(t) in the figure. The vertical beam has a circular cross section of radius r, Young's modulus E and length L. For numerical calculations, use M, = 23.2130 kg, MH = 28.6617 kg. M, = 0.5497 kg, Vý = 8.8974 m/s, L= 2.7757 m, E = 133.5685 GPa andr= 0.0437 m. For circular cross- section I = Tr/4.Considering zero damping and the numerical data given above, obtain the maximum amplitude of response x(t) after it was hit by soccer ball Mp.
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