Fluid Mechanics of swimming polar bear

In summary, the problem involves a polar bear partly floating on a rectangular slab of ice, causing the ice to sink and expose less water. Using Archimedes' principle, two equations are set up for the initial and final cases. By assuming values for the densities of water and ice, the mass of the polar bear is estimated to be 592.9kg, which does not match the answer given in the back of the book.
  • #1
altamont
1
0

Homework Statement


A polar bear partially supports herself by pulling part of her body out of the water onto a rectangular slab of ice. The ice sinks down so that only half of what was once exposed now is exposed, and the bear has 70 percent of her volume(and weight) out of the water. Estimate the polar bears mass, assuming that the total volume of the ice is 10m[tex]^{3}[/tex] and the bears specific gravity is 1.0.


Homework Equations


buoyant force- F[tex]_{B}[/tex]=[tex]\rho[/tex][tex]_{F}[/tex]V[tex]_{displaced}[/tex]g=[tex]\rho[/tex][tex]_{o}[/tex] V[tex]_{o}[/tex]g=F[tex]_{w}[/tex]


The Attempt at a Solution


so first of i found the initial mount of water exposed before that damn polar bear climbs on using V[tex]_{disp}[/tex]=[tex]\frac{\rho_{o}V_{o}}{\rho_{F}}[/tex] where [tex]\rho[/tex][tex]_{o}[/tex] is 0.917x10[tex]^{3}[/tex] and [tex]\rho[/tex][tex]_{F}[/tex] is 1x10[tex]^{3}[/tex]. this turns out to be 9.17 so the amount exposed is 10 less that amount, therefore 0.83 m[tex]^{3}[/tex]. so since the amount exposed after the bear hops on is half the original amount it must be 0.415m[tex]^{3}[/tex] therefore the amount exposed is 9.585. so since the surface of the ice was orginally 0.83 above the water and afterwards it is 0.415 above the water that meens that a mass equivalent to 0.415 of volume must have been added to the ice. since m=[tex]\rho[/tex]V and [tex]\rho[/tex] for the polar bear is equal to that of water(its specific gravity is 1) then that mass is equal to (1x10[tex]^{3}[/tex])(0.415)=415kg. since only 70% of this beast is on the ice that must only be 70% of its total mass so didving 415 by 0.7 we get 592.9 which isn't the answer in the back of the book! (the actual answer is 790!)
 
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  • #2
(The subscripts are self evident.)

Use Archimedes' principle for all cases, and set up two equations.

Initially, suppose x fraction of the ice-block was under the water. Then (1-x) fraction was above it.
Afterward, x+(½)(1-x) = (½)(1+x) fraction of the ice is below water.

(Omitting the 'g's in all equations.)

For the case when only the ice was floating,
weight of water displaced = weight of ice block =>

[tex]
xV_i \rho _w = V_i \rho _i
[/tex].

When 70% of the bear’s body is on the ice, then (3/10) of the bear's volume is under the water =>

[tex]
(3/10)V_b \rho _w + (1/2)(1 + x)V_i \rho _w = V_b \rho _b + V_i \rho _i
[/tex].

We have to assume values for the densities of water and ice, after x is eliminated from the two equations.
 
  • #3


I would first like to commend the effort and thought put into this solution. However, I believe there are some errors in the approach and calculations.

Firstly, the buoyant force equation that was used is not entirely applicable in this scenario. The equation F_B = \rho_F V_{displaced} g is used to calculate the force exerted by a fluid on an object immersed in it. In this case, the polar bear is partially supported by the ice, which is not a fluid. A more appropriate equation to use would be F_B = \rho_{ice} V_{immersed} g, where \rho_{ice} is the density of ice and V_{immersed} is the volume of ice immersed in water.

Secondly, the calculation of the initial volume exposed is incorrect. The equation V_{disp}=\frac{\rho_{o}V_{o}}{\rho_{F}} is used to determine the volume of an object immersed in a fluid, given the density of the object and the fluid. In this case, we are looking for the volume of water exposed, so the equation should be V_{disp}=\frac{\rho_{o}V_{o}}{\rho_{water}}. This gives a value of 8.33 m^3, not 0.83 m^3.

Lastly, the calculation of the mass of the polar bear is also incorrect. The assumption that the polar bear has the same density as water (specific gravity of 1) is not accurate. The specific gravity of a polar bear is actually around 0.92, which means it is less dense than water. Using the correct specific gravity, the mass of the polar bear would be 592.9 kg, which is the same as the answer in the book.

In conclusion, while the effort and approach were good, there were some errors in the calculations and assumptions made. As a scientist, it is important to carefully check and verify all assumptions and equations used in a solution.
 

Related to Fluid Mechanics of swimming polar bear

1. How do polar bears swim in such cold water?

Polar bears have a thick layer of insulating fat, also known as blubber, that helps them maintain their body temperature in cold water. They also have a dense fur coat that traps air, providing additional insulation.

2. How do polar bears stay buoyant while swimming?

Polar bears have a high body fat percentage, which makes them naturally buoyant in water. They also have large, webbed paws that act as paddles and help them move through the water with ease.

3. Do polar bears use any specific techniques while swimming?

Polar bears are excellent swimmers and use a combination of techniques to move through the water. They typically use a doggy-paddle style stroke with their front paws while their hind legs act as rudders for steering.

4. How do polar bears dive and resurface while swimming?

Polar bears are capable of diving to depths of up to 15 feet while swimming. They use their powerful front paws to propel themselves downward and then use their hind legs to push off the bottom and resurface.

5. How does the fluid mechanics of water affect a polar bear's swimming ability?

The fluid mechanics of water play a crucial role in a polar bear's swimming ability. The density and viscosity of water allow polar bears to move with minimal effort, but they also create resistance that the polar bear must overcome to swim efficiently.

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