Why Does a Heavy Spring Extend Differently Under Its Own Weight?

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The discussion revolves around calculating the extension of a spring under its own weight, where a spring of mass M and spring constant k is suspended from a ceiling. The initial calculation yields an extension of Mg/2k, while the book states the answer is Mg/3k. The approach involves considering an element of the spring and calculating the tension and extension based on its position. The discrepancy in answers raises questions about the correctness of the book's solution. The conversation highlights the importance of careful analysis in physics problems involving variable tension in non-uniform systems.
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A spring of mass M is suspended from the ceiling of a room. Find the extension in the spring due to its own weight if it has a spring constant of value k.

I am getting answer as \frac{Mg}{2k}, but the answer given in back of the book is \frac{Mg}{3k}. What I did was :

Let the natural (in un-stretched position) length of the spring be L. Let us consider an element of length dx at a distance x from the bottom of the spring. Then the spring constant of this small spring is k_x = \frac{L}{dx} k. Tension in this spring is T_x= \frac{x}{L} Mg (due to the weight of the spring below it, neglecting the weight of this small spring). Therefore, the extension in this small spring, dl = \frac{T_x}{k_x} = \frac{Mg}{k L^{2}} x dx. Therefore total extension, l = \frac{Mg}{k L^{2}} \int_{0}^{L} x dx = \frac{Mg}{2k}.

So, where I am wrong; or is the answer in the book wrong ?
 
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I'd say that you are correct. What book are you using?
 
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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