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Activity 3: Trip to the Sun - The Curvature of the Earth Page 1 of 1  
 

 
 
The Trip to the Sun demonstrates that, due to its curvature, the Earth falls away below you on your journey. The curvature of the Earth can be noticed by watching a ship sail beyond the horizon. The ship sinks below until only the highest parts of the ship can be seen. From the top of a tall building you can see much further. Clint Brookhart, in his book called Go Figure, Using Math to Answer Everyday Imponderables (1998, Contemporary Books) gives an approximate formula for determining the distance to the horizon for different heights above the ground. The formula is said to be accurate to about 0.5%, and to work for altitudes of up to 180,000 feet. The formula is given as:

Distance D (in miles) =1.225 (h)1/2 where h is the height above the ground in feet.

For example, a person at the seashore whose eyes are 4 feet above the ground can see an ocean horizon about two and a half miles away. From the top floor of the John Hancock Building in Chicago, which is 1,440 feet above the local ground, one can see 46.5 miles. And for an airplane flying at 40,000 feet, the horizon would be 245 miles in each direction. Notice that the formula makes sense as it predicts the horizon to be zero distance away for a height of zero feet. That means that an ant with its eye to the ground has a horizon that is very near, and about zero.

The formula above doesn't take into a small optical effect caused by the fact that air gets less dense with altitude and can bend the light slightly. This means that the different layers of air you see through act like a lens and bend the light from beyond the horizon over the horizon into your view. So you can actually see a bit further than the formula above would predict. A revised formula more accurately describes the distance to the horizon, taking into account the refraction or bending of light. It is attributed to noted geographer Arthur Strahler and means you can see about 8% farther than the geometry would indicate: D = 1.317 (h)1/2

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