GO In analyzing certain geological features, it is often appropriate to assume that the pressure at some horizontal level of compensation, deep inside Earth, is the same over a large region and is equal to the pressure due on the gravitational force on the overlying material. Thus, the pressure on the level of compensation is given by the fluid pressure formula. This model requires, for one thing, that mountains have roots of continental rock extending into the denser mantle (Fig. 14-34). Consider a mountain of height H = 6.0 km on a continent of thickness T = 32 km. The continental rock has a density of 2.9g/cm 3 , and beneath this rock the mantle has a density of 3.3 g/cm 3 . Calculate the depth D of the root, ( Hint: Set the pressure at points a and b equal; the depth y of the level of compensation will cancel out.) Figure 14-34 Problem 23.
GO In analyzing certain geological features, it is often appropriate to assume that the pressure at some horizontal level of compensation, deep inside Earth, is the same over a large region and is equal to the pressure due on the gravitational force on the overlying material. Thus, the pressure on the level of compensation is given by the fluid pressure formula. This model requires, for one thing, that mountains have roots of continental rock extending into the denser mantle (Fig. 14-34). Consider a mountain of height H = 6.0 km on a continent of thickness T = 32 km. The continental rock has a density of 2.9g/cm 3 , and beneath this rock the mantle has a density of 3.3 g/cm 3 . Calculate the depth D of the root, ( Hint: Set the pressure at points a and b equal; the depth y of the level of compensation will cancel out.) Figure 14-34 Problem 23.
GO In analyzing certain geological features, it is often appropriate to assume that the pressure at some horizontal level of compensation, deep inside Earth, is the same over a large region and is equal to the pressure due on the gravitational force on the overlying material. Thus, the pressure on the level of compensation is given by the fluid pressure formula. This model requires, for one thing, that mountains have roots of continental rock extending into the denser mantle (Fig. 14-34). Consider a mountain of height H = 6.0 km on a continent of thickness T = 32 km. The continental rock has a density of 2.9g/cm3, and beneath this rock the mantle has a density of 3.3 g/cm3. Calculate the depth D of the root, (Hint: Set the pressure at points a and b equal; the depth y of the level of compensation will cancel out.)
Space botany requires a certain pressue of 1.20 space pressure units (SPU) for the growth biomes to be succesful.
If 1 SPU= 3 earth atm, what value should my tool that reads out in torr be for everything to be good?
Hint: there are 3 units you should be working with.
(III) The Earth is not a uniform sphere, but has regions of
varying density. Consider a simple model of the Earth
divided into three regions-inner core, outer core, and man-
tle. Each region is taken to have a unique constant density
(the average density of that region in the real Earth):
Region
Radius (km)
Density (kg/m³)
Inner Core
0-1220
13,000
Outer Core
1220–3480
11,100
Mantle
3480–6380
4400
(a) Use this model to predict the average density of the
entire Earth. (b) If the radius of the Earth is 6380 km
and its mass is 5.98 × 1024 kg, determine the actual average
density of the Earth and compare it (as a percent difference)
with the one you determined in (a).
In the Challenger Deep of the Marianas Trench, the depth of seawater is 10.9 km and the pressure is 1.16×108Pa (about 1.15×103atm). (a) If a cubic meter of water is taken from the surface to this depth, what is the change in its volume? (Normal atmospheric pressure is about 1.0×105Pa. Assume that k for seawater is the same as the freshwater value given in Table) (b) What is the density of seawater at this depth? (At the surface, seawater has a density of 1.03×103kg/m)"
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