How do you solve for A in a critically damped oscillator problem?

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The discussion focuses on solving for the constant A in the equation of motion for a critically damped oscillator, given the initial conditions. The condition for critical damping is established as β² = ω₀², where β = b/(2m) and ω₀ = √(k/m). The position function is derived as x(t) = (A + B*t)e^(-βt), and the initial conditions indicate that the mass starts at rest at x = 0 with an initial velocity v₀. The user struggles to determine A, believing it should represent the maximum displacement, but is confused since the mass remains at x = 0 immediately after the impulse. Clarification is provided that the impulsive force gives velocity without initial displacement, which aids in understanding the problem.
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Homework Statement


(A) A damped oscillator is described by the equation
m x′′ = −b x′− kx .
What is the condition for critical damping? Assume this condition is satisfied.
(B) For t < 0 the mass is at rest at x = 0. The mass is set in motion by a sharp impulsive force at t = 0, so that the velocity is v0 at time t = 0. Determine the position x(t) for t > 0.
(C) Suppose k/m = (2π rad/s)2 and v0=10 m/s. Plot, by hand, an accurate graph of x(t). Use graph paper. Use an appropriate range of t.


Homework Equations


For critically damped, β2 = w02
where β = b/(2m) and w0 = √(k/m)

The Attempt at a Solution


Ok, for this problem, what I did initially was find the general form of position for a critically damped oscillator, which is:
x(t) = (A + B*t)*e-β*t

and the velocity function is:
v(t) = -Aβe-βt + (Be-βt - Bβte-βt)

Using the conditions given, I found:
x(0) = A (obviously) which we don't know x(0)
B = v0 + Aβ
and x(t) can be rewritten as:
x(t) = A(e-βt + βte-βt) + v0te-βt

This is where I run into a wall. I can't seem to solve for A. I believe that x(0) should also be the max displacement since there is no driver for the impulse force, so A should be the max displacement, but this doesn't seem to get me anywhere. Any help on solving for A? I know how to do the rest other than that.
 
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A "sharp impulsive force" is defined such that it instantaneously gives the mass an initial velocity without any displacement of the mass. So the mass is still at x = 0 immediately after the impulse.
 
Ok, that makes sense. Thank you for the help.
 
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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