A uniform spring whose unstretched length .

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SUMMARY

A uniform spring with an unstretched length L and spring constant k is divided into two segments of lengths L1 and L2, where L1 = nL2. The resulting spring constants are k1 = (n+1)k/n and k2 = (n+1)k. The derivation utilizes the formula for springs in series, 1/k = 1/k1 + 1/k2, and the relationship between the lengths and spring constants of the segments. Understanding the force equation F = kΔx is crucial for this analysis.

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Estrex
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A uniform spring whose unstretched length...

A uniform spring whose unstretched length is L has a spring constant k. the spring is cut into two pieces of unstretched lengths L1 and L2, with L1 = nL2. What are the corresponding spring constants k1 and k2 in terms of n and k?

The answer is k1 = (n+1)k/n and k2 = (n+1)k. I have no idea how they got that. I tried setting up the force equation F = kL and solving for k, k = F/L, but the substitution never worked out.
 
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Hi Estrex! Welcome to PF! :smile:

Instead of cutting the spring, just mark it where the cut should be, and remember that the reaction force across the mark will be the same in each direction, and will be the same as the force at the ends. (why? :wink:)
 
Estrex said:
I tried setting up the force equation F = kL and solving for k, k = F/L, but the substitution never worked out.
Stop right there. The restoring force generated in a string is given by F = kΔx, where Δx is the length by which the string is compressed or elongated. F does not depend on L at all.
Well now consider the original spring to be split up into two strings of spring constants k1 and k2, which are connected in series and consider what tiny-tim said. That's pretty much all you need to do here!
 
Ok, I figured it out. I just forgot the formula for springs in series, 1/k = 1/k1 + 1/k2.
Since L1 = nL2, k2 = nk1. 1/k = 1/k1 + 1/nk1. 1/k = n+1/nk1. k = nk1/n+1. k1 = k(n+1)/n. Solving for k2, 1/k = n/k2 + 1/k2. 1/k = n+1/k2. k = k2/n+1. k2 = k(n+1).
 
good job... if u forget something, u can always derive it... works for me most of the time...
 
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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