Setting up a differential equation (buoyancy)

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Homework Help Overview

The discussion revolves around setting up a differential equation related to the buoyancy of a spherical object submerged in water. The problem involves analyzing the forces acting on the object as it sinks, including buoyant force, gravitational force, and resistive force, while considering the object's mass and density.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the setup of the differential equation using Newton's second law and question the choice of variables for depth representation. There is a focus on ensuring clarity in variable usage and the need for appropriate initial conditions.

Discussion Status

Some participants have provided guidance on the necessity of two initial conditions for the second-order differential equation. The original poster has made adjustments to the equation based on feedback and is considering assumptions about initial conditions.

Contextual Notes

There is a discussion about the potential confusion arising from using the same variable for both the depth of the pool and the variable representing the object's position. The problem does not explicitly state initial conditions regarding the object's motion, leading to assumptions being made by participants.

24karatbear
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Homework Statement


When an object is submersed in a liquid, it experiences a buoyant force equal to the weight of the liquid displaced by the object. As an object moves through a liquid, there is a resistive force which is directly proportional to the density of the liquid, the cross sectional area A of the object (perpendicular to the direction of motion) and the square of the speed v of the object. A spherical object of mass m and density λ > 1000 begins to sink in a pool of water of depth D. Set up the differential equation with initial condition for the depth of the object below the surface of the water. Use 1000 kilograms per cubic meter as the density of water.

Homework Equations


N/A

The Attempt at a Solution


I am choosing the downward direction (y-direction) to be positive. The object starts at the origin and descends to a depth D. We consider three forces, all in the y-direction: the weight of the spherical object, the buoyant force (= weight of the water displaced by the sphere), and the resistive force. I use Newton's 2nd law:
ΣFy = may = mobject(d2D/dt2) = Fobject - Fbuoyant - Fresistive = mobjectg - (1000 kg/m3)(4*πr3/3)g - kλπr2(dD/dt)2, (where k is just a constant of proportionality) and my initial condition would be D(0) = 0

Would this be correct?

edit: Added g for the buoyant force.
 
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Using D as the depth of the pool and as the vertical coordinate can be confusing. Since you have already mentioned the forces acting on the sphere are in the y direction, why not use y as the general depth coordinate?
 
SteamKing said:
Using D as the depth of the pool and as the vertical coordinate can be confusing. Since you have already mentioned the forces acting on the sphere are in the y direction, why not use y as the general depth coordinate?

Oh, I was trying to be consistent with the variables given in the problem. Would it be incorrect to use D as I used it above?
 
Like I said, it can get confusing using D as the depth of the bottom of the pool (a constant) and D as a variable quantity (the distance as measured from the surface of the pool). It's better to use an arbitrary variable to represent the position of the sphere w.r.t. the surface of the pool (x, y, or, z, for example)
 
SteamKing said:
Like I said, it can get confusing using D as the depth of the bottom of the pool (a constant) and D as a variable quantity (the distance as measured from the surface of the pool). It's better to use an arbitrary variable to represent the position of the sphere w.r.t. the surface of the pool (x, y, or, z, for example)

Ah okay, I got it! I'll switch it out then.

Here's what I get after cleaning the equation up:

mobjg - (1000)(4*πr3/3)g - kλπr2(dy/dt)2 - mobj(d2y/dt2) = 0
--> (d2y/dt2) - g + (1000)(4*πr3/3)g/mobj + kλπr2(dy/dt)2/mobj = 0 (divided everything by -mobj)
--> (d2y/dt2) + kπr2λ(dy/dt)2/mobj + g[(1000)(4*πr3/3)/mobj -1] = 0, Initial condition: y(0) = 0

Am I on the right track?
 
You're getting warmer. Since this is a second order equation, you'll need two separate initial conditions to determine a unique solution. You have specified the initial starting position of the sphere. Can you think of another condition to specify?
 
SteamKing said:
You're getting warmer. Since this is a second order equation, you'll need two separate initial conditions to determine a unique solution. You have specified the initial starting position of the sphere. Can you think of another condition to specify?

Oh, right! I am guessing that I'll need y'(0) = 0? The problem doesn't say that it starts at rest, but I suppose I can assume that it does for the 2nd condition (feel free to correct me if I'm wrong).
 
That would be a reasonable initial condition.
 
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