Banked Race Track Physics Problem: Max and Min Speeds without Friction

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On a banked race track with radii of 111 m and 163 m, the smallest speed for cars to move without friction is calculated to be 0 m/s, occurring when the track is flat. The largest speed, theoretically, is infinity, which arises when the track is at a steep angle of 90 degrees. The angle θ can be determined using the height of the outer wall and the difference in radii, leading to the equation tanθ = (r2 - r1)/18. While the calculations suggest no upper limit to speed in a frictionless scenario, practical conditions will always impose some friction, resulting in a lower maximum speed. Thus, while theoretical values are established, real-world factors will affect actual performance on the track.
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On a banked race track, the smallest circular path on which cars can move has a radius r1 = 111 m, while the largest has a radius r2 = 163 m. The height of the outer wall is 18 m.

(a) Find the smallest speed at which cars can move on this track without relying on friction.

(b) Find the largest speed at which cars can move on this track without relying on friction.

I think that I'm supposed to use this equation:
v= Square root of (r)(g)tan theta, but I don't know how to find theta?
 
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you can make a triangle out of the info given. Assuming the base of the track is on the x-z plane, you can create a triangle by taking a cross section pointing radially inward from the circle pointing in the positive y direction. Anyway that's not relevant just trying to give you a reference point. The two legs of the triangle would be (163-111) on the bottom and 18 going up. From this you can find an incline (theta) and you're solving for V.
 


Yes, you are correct that the equation v = √(r*g*tanθ) can be used to solve this problem. To find θ, we can use the fact that the height of the outer wall (18 m) is equal to the difference in height between the two circular paths (r2 - r1). So, we can set up the following equation:

tanθ = (r2 - r1)/18

(a) To find the smallest speed, we want to find the minimum value of θ. This occurs when the track is completely flat (θ = 0). So, we can plug in θ = 0 into the equation and solve for v:

v = √(r1*g*tan0) = √(r1*g*0) = 0

Therefore, the smallest speed at which cars can move on this track without relying on friction is 0 m/s.

(b) To find the largest speed, we want to find the maximum value of θ. This occurs when the track is at its steepest angle. So, we can plug in the maximum value of θ (90 degrees or π/2 radians) into the equation and solve for v:

v = √(r2*g*tan(π/2)) = √(r2*g*∞) = ∞

Therefore, the largest speed at which cars can move on this track without relying on friction is infinity. This means that there is no limit to the speed of the cars on this track as long as there is no friction. However, in reality, there will always be some amount of friction present, so the actual maximum speed will be less than infinity.
 
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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