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Lesson2e Lava Tubes and Density

Lesson2e

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Lesson2e . Lava Tubes and Density. Lava tubes. Lava pouring out of Lava Tube. Collapsed Lava Tube on Earth . Lava flows in channels also. Lunar Rille (means “groove”). Topographical map of Mars. Olympus Mons. Lava Tubes on Mars – Pavonis Mons. - PowerPoint PPT Presentation

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Page 1: Lesson2e

Lesson2e

Lava Tubes and Density

Page 2: Lesson2e

Lava tubes

Page 3: Lesson2e

Lava pouring out of Lava Tube

Page 4: Lesson2e

Collapsed Lava Tube on Earth

Page 5: Lesson2e

Lava flows in channels

also

Page 6: Lesson2e

Lunar Rille (means “groove”)

Page 7: Lesson2e
Page 8: Lesson2e
Page 9: Lesson2e

Topographical map of Mars

Olympus Mons

Page 10: Lesson2e

Lava Tubes on Mars – Pavonis Mons

Page 11: Lesson2e

SolidifiedLava flow

at the base of

Olympus Mons

Page 12: Lesson2e

Which surface do you think

might be older,

Surface A or

Surface B?

“A”

“B”

Flat Plain at bottom of slope

Page 13: Lesson2e

Which surface do you think

might be older?A or B?

A

B

Page 14: Lesson2e

• Surface A is likely to be older. We can see a number of impact craters in surface A. But surface B seems to be missing craters.

• The area in the image is about the same for both regions.

• We must assume that lava has covered up any craters that might have been present in surface B. This makes B younger than A.

Page 15: Lesson2e

A very big question to answer

• We see that the Moon and Mars have both had active volcanism.

• When a planet is still very hot inside various tectonic processes occur that allows the heat to escape the interior. We say the planet is geologically active.

• When a planet cools to the point that tectonism stops, we say the planet is geologically dead.

• If we don’t see tectonic processes occurring at the moment, what do we have to do in order to determine when a planet was geologically active?

Page 16: Lesson2e

• We need to determine the age of the features we see.

• Radiometric data of lava would be the best but we can not currently travel to Mars and return rock samples. Or the other planets or moons.

• An important tool to use is crater density on the surface. The greater the density of craters the older the surface must be.

Page 17: Lesson2e

Density -- an important parameter

• There are two types of densities we will use in this class.

• Mass density (mass/volume) and Number density (number/volume).

• A density doesn’t have to be a volume density.• It can be an area density. (kg/m2)• And it doesn’t have to be mass.

Page 18: Lesson2e

Population Density

• Alaska has a population of 686,000 people• It has an area of 663,000 square miles.

• That is roughly 1 person/square mile.

• What does this tell us about the lives of Alaskans?

Page 19: Lesson2e

• Not much. It only tells us there is a lot of room for people to expand into.

• This is an average density. In fact most Alaskans live near or in cities where the population density is much higher.

Page 20: Lesson2e

White blood cell counts.

• When a doctor checks your white blood cell counts for an infection, they draw some blood and then use a very small volume of blood to count the number of white cells.

• This is a number of white blood cells/volume.• This density tells them if you have an infection

or not.• What assumptions is built into this analysis?

Page 21: Lesson2e

Let’s compute the mass density of the Earth.

• Earth mass = 5.97 x 1024 kg.• Earth radius = 6.96 x 106 m.• Density = mass/volume• The Earth is approximately a sphere.• So all we need is the volume equation for a

sphere.

Page 22: Lesson2e

A volume is 3-D

R

LL

L

V = L x L x L = L3 V = 4πR3/3

Page 23: Lesson2e

• The surface area of a sphere is: 4πR2

• The surface area of a cube is: 6L2

• The volume of a sphere is (4/3)πR3

• The volume of a cube is L3

Page 24: Lesson2e

Let’s compute the mass density of the Earth.

• Earth mass: M = 5.97 x 1024 kg.• Earth radius: R = 6.96 x 106 m.• Density = mass/volume = M/V• The Earth is approximately a sphere.• So all we need is the volume equation for a

sphere.• V = (4/3) π R3

Page 25: Lesson2e

• V = (4/3)π(6.96 x 106 m)3

• Dearth = (5.97 x 1024 kg)/(1.09 x 1021 m3)

• Dearth = 5,477 kg/m3

• Dearth = 5.48 g/cm3

We can test this by comparing to rocks we find on the surface.

Page 26: Lesson2e

This is easy to do.

• Weigh the rock to find its mass.• Find the volume of the rock by the amount of

water it displaces.

Page 27: Lesson2e

Result

• The average density of rocks on the surface of the Earth is Drock = 3 g/cm3

• The density we calculated for the Earth was

This is very different. How can we explain this?

Dearth = 5.48 g/cm3

Page 28: Lesson2e

• The density we calculated for the Earth was the average density. It doesn’t mean that the density is the same everywhere inside.

• Here is what we have:• Average density of Earth is 5.48 g/cm3

• Average density of surface rocks is 3 g/cm3

• Inside the Earth there must be something that is much more dense than the surface rock in order to increase the average.

Page 29: Lesson2e

• Research on the composition of meteorites shows that many are composed of high fractions of iron.

• The Earth and the other planets are built up from the accumulation of meteors and asteroids.

• The planets should have a lot of iron.• The density of iron is about 8 gm/cm3

• You can see that mixing iron densities with rock densities will give us something closer to the average.

Page 30: Lesson2e

• The iron has to be in the interior of the Earth and not much on the surface.

• In fact, the core of the Earth is mostly iron.

• Why is the majority of Earth’s iron in the core?

Page 31: Lesson2e

Differentiation

• When the Earth was forming it was suffering many impacts from meteors and asteroids.

• These impacts heated the Earth so that it was completely molten.

• When it was in liquid form, it was possible for the dense elements (like iron) to sink, and the least dense elements (like silicon) to rise.

• This is why the surface rocks are low density.

Page 32: Lesson2e

Compressed vs. Uncompressed

The average density we have been discussing is the Earth’s compressed density. It depends on the material in the Earth and how much that material is compressed by the Earth’s gravity.

If we want to know what planets are made of, we do not want to take into account the force of gravity. This is the uncompressed density. It only depends on the material in the planet.

Page 34: Lesson2e

• Let’s see what we can deduce about the four Galilean moons, Io, Europa, Ganymede, and Callisto.

Page 35: Lesson2e

Io – Density = 3.6 gm/cm3

Page 36: Lesson2e

Europa – Density = 3.0 g/cm3

Page 37: Lesson2e

Ganymede – Density = 1.9 g/cm3

Page 38: Lesson2e

Callisto – Density = 1.8 g.cm3

Page 39: Lesson2e

Other evidence

• Surface of Europa, Ganymede and Callisto is composed of water ice. (Density = 1 g/cm3)

• What can you conclude about the Galilean moons?

Page 40: Lesson2e

Io Europa

GanymedeCallisto