Dirac delta function (DE problem) solved

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The discussion revolves around solving a deflection problem for a uniform beam subjected to a concentrated load using the Laplace transform. The key equation derived is EI(d^4y/dx^4) = w_0δ(x - L/2), with boundary conditions specified for deflection and its derivatives at the beam's ends. The solution for deflection y(x) is expressed as a combination of terms involving the load w_0, the beam's length L, and constants c_1 and c_2. The constants are determined through boundary conditions, leading to the final expression for y(x). The thread concludes with a positive acknowledgment of the solution's simplicity.
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NOTE: I actually found the correct answer while I was typing this :rolleyes: and since I already had it typed, I figured i would post anyway. mods you can do with it as you please or leave it for reference. thanks

Here's the problem:



A uniform beam of length L carries a concentrated load w_{0} at x=\frac{1}2{L}. The beam is embedded at its left end and is free at its right end. Use the Laplace transform to determine the deflection y(x) from EI\frac{d^4y}{dx^4}=w_{0}\delta(x-\frac{L}2) where y(0)=0, y'(0)=0, y''(L)=0, y'''(L)=0.




Here is what I did: let y''(0)=c_{1}, y'''(0)=c_{2}

EI(s^4Y(s)-s^3y(0)-s^2y'(0)-sy''(0)-y'''(0))=w_0e^{\frac{-LS}2

s^4Y(s)-sc_1-c_2=\frac{w_0}{EI}e^\frac{-LS}2

Y(s)=\frac{w_0}{EIs^4}e^{\frac{-LS}2}+\frac{c_1}{s^3}+\frac{c_2}{s^4}

y(x)=\frac{w_0}{6EI}(x-\frac{L}2)^3U(x-\frac{L}2)+\frac{c_1x^2}2+\frac{c_2x^3}6

y'(x)=\frac{w_0}{2EI}(x-\frac{L}2)^2U(x-\frac{L}2)+c_1x+\frac{c_2x^2}2

y''(x)=\frac{w_0}{EI}(x-\frac{L}2)U(x-\frac{L}2)+c_1+c_2x

y'''(x)=\frac{w_0}{EI}U(x-\frac{L}2)+c_2



y''(L)=\frac{Lw_0}{2EI}+c_1+c_2L=0

y'''(L)=\frac{w_0}{EI}+c_2=0

c_2=\frac{-w_0}{EI}

c_1=\frac{Lw_0}{2EI}

y(x)=\frac{w_0}{6EI}(x-\frac{L}2)^3U(x-\frac{L}2)+\frac{Lw_0x^2}{4EI}-\frac{w_0x^3}{6EI}
 
Last edited:
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Glad to hear you got it solved. We love the easy ones :smile:
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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