Quadratic Drag Force: Solving Differently

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The discussion centers on the confusion surrounding the different approaches to solving two similar problems involving quadratic drag force. The first problem utilizes the equation of motion during ascent, leading to the relationship between velocity and position, while the second problem focuses on velocity as a function of time. The key distinction lies in the first question's requirement to express speed as a function of position, which simplifies the solution process. The use of the chain rule, specifically ##\frac{dv}{dt}=\frac{dv}{dy}\frac{dy}{dt}##, is highlighted as a crucial technique that aids in solving the first problem effectively. Understanding these differences clarifies why the two problems yield different forms of answers despite their similarities.
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Homework Statement
There are two questions in my book that are almost the same but have two different answers.

The first question:
A particle is projected vertically upward in a constant gravitational field with an initial speed of ##v0##. Show that if there is a retarding force proportional to the square of the speed, the speed of the particle when it returns to its initial position is where $$\frac{v_ov_T}{\sqrt{v_o^2+v_T^2}}$$ ##v_T## is the terminal speed.

Second question:
A baseball is thrown vertically up with speed v o and is subject to a quadratic drag with magnitude ##f (v) = cv^2## . Write down the equation of motion for the upward journey (measuring ##y## vertically up).
Relevant Equations
##F=ma##
But the answers to these two questions confuses me.

For the first question the answer goes like: $$m\ddot y = -mkv^2-mg$$ $$\therefore \ddot y = v\frac{dv}{dy}$$ $$\therefore v\frac{dv}{dy}= -kv^2-g$$

but for the answer to the second question we have: $$m\dot v = mg - cv^2.$$

Both questions are very similar but with different answers. Why is the first question solving it using ##\frac{dv}{dy}\frac{dy}{dt}## instead of just ##\dot v##?
 
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The first equation for the first question is the equation of motion during ascent, and it matches the answer to the second question. But the first question requires you to go further.
It is not in general possible, or at least not easy, to solve drag equations to get position as a function of time. But in the first problem you do not need speed or position as a function of time, but speed as a function of position. Using ##\frac{dv}{dt}=\frac{dv}{dy}\frac{dy}{dt}## makes it a lot easier.
 
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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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