How Do I Solve This Limit Using Factoring X Out?

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To solve the limit \(\lim_{x\rightarrow 0}\frac{\sqrt[4]{1+x^2}-1}{x}\), factoring out \(x\) leads to an indeterminate form of \(\infty - \infty\). The correct approach involves setting \(a=\sqrt[4]{1+x^{2}}\) and \(b=1\), and finding the polynomial \(P(a,b)\) that satisfies \((a-b)P(a,b)=a^{4}-b^{4}\). This can be achieved through polynomial division of \(a^{4}-b^{4}\) by \(a-b\). Finally, multiplying the fraction by \(\frac{P(a,b)}{P(a,b)}\) allows for the limit to be evaluated, confirming that the answer is 0.
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I Have No Clue How To Start This One. I Tried Applying The Same Kind Of Strategy As In https://www.physicsforums.com/showthread.php?t=51562 But No Luck. Please Give Me A Hint.

\lim_{x\rightarrow 0}\frac{\sqrt[4]{1+x^2}-1}{x}

Factoring X Out Gives A \infty - \infty Undeterminate Form. The answer is 0.
 
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Set:
a=\sqrt[4]{1+x^{2}}, b=1^{\frac{1}{4}}=1
Find the polynomial in a, b P(a,b) which satisfies:
(a-b)P(a,b)=a^{4}-b^{4}
In order to find P(a,b), use polynomial division on:
(a^{4}-b^{4}):(a-b)

In order then to evaluate the limit, multiply your fraction with:
1=\frac{P(a,b)}{P(a,b)}
 
Simply amazing!

And I realize this method is the same as the one which have been advised to me for the other limit problem, but generalized. Thanks arildno !
 
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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