<?xml version="1.0" encoding="UTF-8"?>
<?xmlspysps C:\Program Files\Altova\AUTHENTIC\sps\template\TeachEngineering\lesson.sps?>
<lesson xmlns="http://www.teachengineering.org" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.teachengineering.org C:\PROGRA~1\Altova\AUTHENTIC\sps\template\TeachEngineering\lesson.xsd" xml:lang="en-US" version="1.0">
	<title>Get Me Off This Planet</title>
	<header>
		<text_section>
			<text_block format="text">
				<text_element><image url="../cub_images/cub_mars_lesson04_image1.jpg" description="A photo of a rocket taking off." horizontal_alignment="right" rights="Microsoft Corporation 1983-2001."/></text_element>
			</text_block>
		</text_section>
	</header>
	<grade realm="k12" target="8" lowerbound="6" upperbound="8"/>
	<lesson_number rank="4" total="6"/>
	<time total="50" unit="minutes"/>
	<summary>The purpose of this lesson is to teach students how a spacecraft gets from the surface of the Earth to Mars. Students first investigate rockets and how they are able to get us into space. Finally, the nature of an orbit is discussed as well as how orbits enable us to get from planet to planet &#x2014; specifically from Earth to Mars.</summary>
	<engineering_connection>
		<text_section>
			<text_block format="text">
				<text_element>Aeronautical engineers play an important role in the design of rockets for space exploration. These engineers must have a thorough understanding of Newton's third law of motion &#x2014; or else the rockets would not leave the Earth's surface! Engineers are also experts in the concepts of thrust and specific impulse, so they are able to design efficient rockets. Engineers also lead the research that has resulted in the three primary rocket types used in space applications: chemical rockets, electrical rockets and cold gas rockets.</text_element>
			</text_block>
		</text_section>
	</engineering_connection>
	<engineering_category_TYPE category="Category1_Relating_Science_Concept_to_Engineering"/>
	<keywords>
		<keyword>launch</keyword>
		<keyword>laws of motion</keyword>
		<keyword>Mars</keyword>
		<keyword>Newton</keyword>
		<keyword>orbit</keyword>
		<keyword>planet</keyword>
		<keyword>rocket</keyword>
		<keyword>solar system</keyword>
		<keyword>space</keyword>
	</keywords>
	<edu_standards>
		<edu_standard identifier="S11417BA"/>
		<edu_standard identifier="S11425BD"/>
		<edu_standard identifier="S11425C1"/>
		<edu_standard identifier="S1142658"/>
		<edu_standard identifier="S11426CF"/>
	</edu_standards>
	<learning_objectives>
		<text_section>
			<text_block format="text">
				<text_element>After this lesson, students should be able to:</text_element>
			</text_block>
			<text_block format="unordered">
				<text_element>Describe how a rocket must overcome the forces of gravity and drag in order to get out of the atmosphere.</text_element>
				<text_element>Explain that thrust is the force created by a rocket.</text_element>
				<text_element>Describe how an orbit is the balance of gravity and an object&apos;s tendency to follow a straight path.</text_element>
				<text_element>Explain some challenges that engineers face in getting a rocket to Mars.  </text_element>
			</text_block>
		</text_section>
	</learning_objectives>
	<introduction>
		<text_section>
			<text_block format="text">
				<text_element>How does a rocket physically get from the Earth to Mars? (Expect students to indicate that it takes a very large rocket to get there.) Why do you need such a large rocket? (Expect answers such as: We need to overcome gravity, Mars is a far away, when we go to Mars, we have to take a lot of supplies and equipment, and maybe even, we have to overcome gravity and the drag of our atmosphere.) </text_element>
				<text_element>So, as soon as we leave the atmosphere, are we free to travel to Mars?  Not quite yet, we are still in the grip of Earth&apos;s gravity even though the astronauts feel weightless. There is a misconception that once you leave the Earth&apos;s atmosphere, there is no gravity. The truth is that there is gravity acting on a person in orbit around the Earth - but they do not feel it. A comparison can be made to a sky diver. Do you think a sky diver feels the effects of gravity? The answer is no, a sky diver cannot feel gravity. S/he can feel the air rushing by and see the ground coming up but s/he cannot actually feel gravity. This feeling is called <italic>weightlessness</italic>, and it does not mean that gravity is not there. It is as if both the astronaut and spacecraft are perpetually falling, but never actually get any closer to the surface of the Earth. </text_element>
				<text_element>So, once a rocket has taken us out of the Earth&apos;s atmosphere, we enter into an <italic>orbit </italic>around the Earth. What is an orbit? (Listen to student suggestions. ) An orbit is a regular, repeating path that one object in space takes around another one. What is the shape of most orbits? (Listen to their answers; most will suggest the shape of a circle.) It is elliptical. An ellipse is essentially an oval. While a circle is a special kind of ellipse, engineers and scientists use the term ellipse to describe orbits around Earth and other bodies such as the Sun. So, if a spacecraft is in orbit around Earth, how does it get to Mars? (Listen to student answers.) Well, it uses another rocket. If the rocket moves the craft fast enough, it can overcome the Earth&apos;s gravity and start heading for Mars. Elliptical orbits also help to move a rocket between planets. However, many other factors must be taken into consideration when traveling between planets. Today we are going to talk about the basics of traveling from Earth to Mars.</text_element>
			</text_block>
		</text_section>
	</introduction>
	<lesson_background>
		<text_section name="Getting off Earth - Launch">
			<text_block format="text">
				<text_element>The first step on the trip to Mars is the <italic> aunch</italic>. Launch is the act of getting a spacecraft off the surface of the Earth and into an orbit around it. It takes a lot of energy to reach an orbit above Earth. Consider that just to jump a couple feet off the ground takes all the energy we can muster. To get a thousand kilogram spacecraft off the ground takes an incredible amount of energy. Not only do we have to overcome Earth&apos;s gravity, but also the drag of the atmosphere. To figure out how much velocity we need to get into an orbit around Earth, we use the following equation:</text_element>
				<text_element alignment="center"><image url="../cub_images/cub_mars_lesson04_equation01.jpg" description="Equation" horizontal_alignment="center"/></text_element>
				<text_element>where, ∆ means change and <italic> V</italic> means velocity. </text_element>
				<text_element>So ∆V<subscript>Launch</subscript> is the total change in velocity needed to launch a spacecraft into an orbit around Earth. ∆V is the final velocity minus the initial velocity. Since the velocity of the spacecraft is initially zero while it is on the ground, ∆V is simply the final velocity. ∆V<subscript>burnout</subscript> is the leftover velocity that we need to maintain and orbit around Earth. We will talk about this velocity a little later. ∆V<subscript>gravity</subscript> is the change in velocity needed to overcome the gravity of Earth. ∆V<subscript>drag</subscript> is the change in velocity required to overcome drag.</text_element>
				<text_element>To achieve the required ∆V, engineers at NASA use huge rockets. The actual size and mass of the rocket, which engineers call the <italic>launch vehicle</italic>, dwarfs the actual spacecraft, which is referred to as the <italic> payload</italic>.  For a typical mission into Low Earth Orbit (LEO) the mass of the launch vehicle and the fuel is roughly 40 times the mass of the actual payload.</text_element>
				<text_element>So, how does a rocket create the ∆V we need? (Answer: Rockets take advantage of what is described in Newton&apos;s third law of motion.) Newton&apos;s third law states that for every action there is an equal and opposite reaction. If you were to stand on a skateboard and push against a wall you would move in the opposite direction. This is an example of Newton&apos;s third law. Cars use tires to push backwards against the road, which causes them to move in the opposite direction. True, rockets do not actually push against the air, but the movement of a rocket is still described by Newton&apos;s third law of motion. A rocket works by creating super hot gasses and &quot;throwing&quot; them backwards very quickly.  This &quot;throwing&quot; of the air is the <italic>action</italic>. The <italic>reaction </italic>is that the rocket moves in the opposite direction, forwards. </text_element>
				<text_element>We use two basic numbers to characterize rockets. The first of is the<italic> thrust </italic>&#x2014; the force that pushes the rocket into orbit. We calculate the amount of thrust a rocket produces by using the following equation:</text_element>
				<text_element alignment="center"><image url="../cub_images/cub_mars_lesson04_equation02.jpg" description="Equation" horizontal_alignment="center"/></text_element>
				<text_element>where the thrust force (F) is equal to the mass flow rate (m) multiplied by the exhaust velocity (V<subscript>e</subscript>). The mass flow rate is how fast mass is coming out of the rocket. The mass is the exhaust gas that comes from the burning fuel. Mass flow rate is measured in kilograms per second (kg/s).  The exhaust velocity is a measure of how fast the hot gas leaves the rocket nozzle.</text_element>
				<text_element>The other number we use to characterize rockets is the<italic> specific impulse</italic> (I<subscript>sp</subscript>) &#x2014; a measure of the energy content of a propellant and how efficiently it is converted into thrust. Basically, the specific impulse tells us how much &quot;bang for the buck&quot; we get out a certain type of rocket. To calculate the specific impulse, we divide the thrust by the weight flow rate:</text_element>
				<text_element alignment="center"><image url="../cub_images/cub_mars_lesson04_equation03.jpg" description="Equation" horizontal_alignment="center"/></text_element>
				<text_element>The weight flow rate is the mass flow rate (m) multiplied by the gravitational acceleration of Earth (g = 9.81 m/s<superscript>2</superscript>). The specific impulse has units of seconds. The I<subscript>sp</subscript> measures how much thrust we are getting for how much fuel weight we are using. A higher I<subscript>sp</subscript> means that we are getting more thrust for less fuel, and it is more efficient system.</text_element>
				<text_element>Three different kinds of rockets are currently used in space applications: chemical, electrical and cold gas. <italic>Chemical rockets</italic> are the most common typein use today, and include liquid fuel rockets, solid fuel rockets and a hybrid of the two. Chemical rockets rely on chemical combustion that creates a super-heated, high-pressure gas. This high-pressure gas can only escape through the nozzle. According to Newton&apos;s third law of motion, this gas leaving the rocket at a very high velocity is the action, while the rocket moving in the opposite direction is the opposite reaction. </text_element>
				<text_element><image url="../cub_images/cub_mars_lesson04_figure1.jpg" description="A drawing shows two tanks inside a rocket that hold the fuel and the oxidizer. A pump that moves the fuel and oxidizer into the combustion chamber where the fuel burns. The hot gasses then escape out the back end of the rocket through the nozzle." horizontal_alignment="center" rights="NASA http://spaceplace.jpl.nasa.gov/en/kids/ (edited by Geoff Hill, University of Colorado, 2004)" caption="Figure 1. Diagram of a liquid fuel rocket."/></text_element>
				<text_element>Liquid fuels are stored in large tanks and are pumped into a combustion chamber where they ignite before leaving the rocket through the nozzle. Figure 1 shows a diagram of a liquid fuel rocket. Liquid fuel systems are complicated since they require several tanks, complex valves and intricate piping, but they create a lot of thrust, have a high Isp, and can be throttled and restarted if needed. The space shuttles main engines use a liquid fuel that is a mixture of liquid oxygen and liquid hydrogen. Figure 2 shows the liquid fuel tank and the liquid fuel main engine on the space shuttle.</text_element>
				<text_element><image url="../cub_images/cub_mars_lesson04_figure2.jpg" description="Photo of the space shuttle during launch, showing the two white solid rocket boosters, three main engines, and red liquid fuel tank." horizontal_alignment="left" rights="http://nvo.gsfc.nasa.gov/astrodata/epohst-satellite.html (edited by Geoff Hill, University of Colorado, 2004)" caption="Figure 2. The space shuttle&apos;s rockets."/></text_element>
				<text_element>Solid fuel rockets can be described as a tube, filled with a solid fuel, capped at one end and with a nozzle at the other end. The solid fuel is highly flammable and works in the same way the liquid fuel system works. As the fuel burns, a hot and high-pressure gas comes out of the nozzle creating thrust. Solid fuel systems are very simple, cheap and reliable, but they cannot be turned off once they start and they are not as efficient as liquid fuels. An example of a solid fuel system is the Solid Rocket Boosters (SRB) on the space shuttle (see Figure 2). They are the two white rockets strapped to the side of the vehicle and are used to help get the space shuttle off the ground. Once the fuel inside the boosters is exhausted, they are released from the shuttle and dropped into the ocean. Bottle rockets and model rockets are both considered solid fuel rockets.</text_element>
				<text_element>Electrical rockets use electricity to accelerate particles that are directed out the back end of the spacecraft, thus creating thrust. The rockets generally use charged atoms called ions that have a positive or negative charge associated with them. An electrical source, such as solar cells, or a nuclear reactor is used to charge plates in the engine with different charges so that the ions are pushed and pulled out of the spacecraft. The downside to electrical rockets is that they cannot create much thrust. If you hold one sheet of paper in your hand, the force with which the paper pushes on your hand due to its weight is roughly equal to the thrust of an electrical rocket. The plus side to electric rockets is that they are very efficient and have a high Isp. Since the thrust of an electrical rocket is so small, it is impossible to launch a rocket into space; but, once a spacecraft is in an orbit around Earth, an electrical rocket can be used to escape the Earth&apos;s gravity and head to different places around our solar system. The small thrust means it takes a long time for the craft to build up sufficient escape velocity, but the high efficiency of the system means less fuel is needed to achieve the desired velocity. The first use of electrical rockets in space was onboard Deep Space 1, which launched onboard a conventional liquid fuel rocket on October 24, 1998. Once it was in orbit, it started its own engine and eventually reached the Comet Borrelly in September of 2001.</text_element>
				<text_element>Cold gas rockets use pressurized gas that is not ignited. This is usually a nonflammable gas such as nitrogen or helium. A balloon that is filled and then released is an example of a cold gas system. The pressurized gas can only escape out the nozzle, and as it does, it creates thrust. Cold gas systems have very low thrusts and are very inefficient (low I<subscript>sp</subscript>), but they are very simple and cheap. They are often used on spacecraft to make very small velocity changes where large rockets are overkill. The rocket packs that astronauts use when they are outside the space shuttle or international space station use cold gas rockets.</text_element>
				<text_element>Table 1 shows the different types of rockets and the typical thrusts and specific impulses for each system.</text_element>
				<text_element alignment="center"><image url="../cub_images/cub_mars_lesson04_table1.jpg" description="A table lists maximum specific impulses and maximum thrust for liquid, solid, electric and cold gas rocket types." horizontal_alignment="center" caption="Table 1. Rockets, Thrusts and Specific Impulses."/></text_element>
			</text_block>
		</text_section>
		<text_section name="Orbits">
			<text_block format="text">
				<text_element>Once a launch vehicle has taken the spacecraft out of the Earth&apos;s atmosphere, it now must enter into an <italic>orbit</italic>. An orbit is a circular or elliptical path around a celestial body (sun, star, planet, asteroid, etc.) on which an object such as a spacecraft follows. One common misconception is that no gravity exists on the space shuttle and international space station. In fact, gravity <italic>is </italic>acting on a person in orbit around the Earth, but s/he does not feel it like we feel it on Earth, because no ground exists to push back on a person in space. So, why doesn&apos;t a spacecraft just fall back to Earth once the rockets shut off? This is because the velocity of the spacecraft wants to move it past the Earth, while gravity pulls it back. These two actions cancel out to form an orbit.  An orbit can be explained by Newton&apos;s first law of motion, which tells us that an object in motion stays in motion unless a force acts against it. This means that an object will move in a straight line unless a force pushes it in a different direction. For any object to change the direction in which it is moving, a force force must act upon it. For example, when you are on a bike and want to turn (change directions), your tire must apply a force to the ground. This force is called friction; without friction, it would be like biking on perfectly smooth ice. If you tried to turn, there would be no frictional force; you would keep moving in a straight line as Newton&apos;s first law describes. Just like your bike, a spacecraft will not turn unless a force acts on it. The force that acts on objects &#x2014; ultimately causing them to orbit a planet or a star &#x2014; is gravity. An orbit is just a balance between the velocity of an object and gravity.  </text_element>
				<text_element><image url="../cub_images/cub_mars_lesson04_figure3.jpg" description="Two drawings: (left) The path of a spacecraft if the gravity of Earth had no affect on it. The spacecraft continues in a straight line past Earth and beyond. (right) The same spacecraft under the influence of gravity; gravity bends the path of the spacecraft into a curved orbit. around the planet" horizontal_alignment="left" rights="2004 Geoff Hill, University of Colorado Boulder" caption="Figure 3. How an orbit works."/></text_element>
				<text_element>Figure 3 shows how gravity affects the path of a spacecraft. The diagram on the left shows the path of a spacecraft if there was no gravity. In this case, the spacecraft would continue along in a straight line. The diagram on the right shows the path of a spacecraft under the influence of gravity. Gravity is pulling the spacecraft towards the center of the Earth, while the velocity of the spacecraft makes the spacecraft want to keep going past the Earth. The balance of these two opposing actions is known as an orbit. For a low Earth orbit (LEO), which has an altitude between 600 and 2000 kilometers above the Earth&apos;s surface, the spacecraft must have a velocity of about 8 kilometers per second. That means that it can go all the way around the Earth in 90 minutes. So, what happens if the spacecraft is not moving (that is, it has no velocity)? If there is no velocity, then the only force acting on the spacecraft is gravity. This means that a spacecraft would fall to Earth just as a stone falls to the ground when you drop it. So, what happens if the spacecraft is moving much faster than the 8 km/s needed to maintain a LEO? In that case, the gravity will not be able to hold the spacecraft as close to the Earth, and the spacecraft will either move into an orbit that is further away from the Earth, or if it is moving fast enough it will overcome the Earth&apos;s gravity entirely.  This is called the <italic>escape velocity</italic>, and it is the minimum velocity needed to escape the Earth&apos;s gravity. </text_element>
				<text_element>Sir Isaac Newton performed a famous mind experiment to demonstrate how an orbit works that involves shooting cannons off the top of a mountain. See a demonstration of the cannon ball orbit on the NASA website at <link url="http://spaceplace.nasa.gov/en/kids/orbits1.shtml" type="internet">http://spaceplace.nasa.gov/en/kids/orbits1.shtml</link>. </text_element>
			</text_block>
		</text_section>
		<text_section name="Getting to Mars">
			<text_block format="text">
				<text_element>Now that our spacecraft has left Earth&apos;s gravity, our mission is to arrive at Mars. We have left the influence of Earth&apos;s gravity, but we are not free of gravity altogether. Since we are now orbiting around the Sun, we are now under the influence of the Sun&apos;s gravity.   </text_element>
				<text_element>Thus far, we have talked about circular orbits &#x2014; the simplest kind of orbit. However, most orbits are actually ellipses, a stretched circle. Ellipses are often called ovals. Figure 4 shows a diagram of an elliptical orbit. </text_element>
				<text_element alignment="center"><image url="../cub_images/cub_mars_lesson04_figure5.jpg" description="A drawing of an elliptical orbit showing the foci, periapsis and apoapsis." horizontal_alignment="center" rights="2004 Geoff Hill, University of Colorado Boulder" caption="Figure 4. An elliptical orbit." width="400"/></text_element>
				<text_element>Two foci (each one called a focus) define an ellipse: the <italic>periapsis</italic>, which is the point on the elliptical orbit that is closest to the planet or sun; and the <italic>apoapis</italic>, the point furthest from the planet or sun. You may have also heard these points called <italic>perigee </italic>and <italic>apogee</italic>. These are the periapsis and apoapsis for an elliptical orbit around Earth, respectively.  In an elliptical orbit, the Earth (or other massive body) is located at one of the two foci. Elliptical orbits enable movement between planets. Using the Sun as one of the foci, and the Earth as the periapsis, the spacecraft will actually be closer to the Sun when it is at the periapsis. When the spacecraft is at the apoapsis, it will be further away from the sun.  This is useful for traveling to planets further from the Sun such as Mars. Figure 5 shows how half an elliptical orbit can be used to get from Earth to Mars.</text_element>
				<text_element alignment="center"><image url="../cub_images/cub_mars_lesson04_figure6.jpg" description="A drawing of an elliptical transfer orbit from Earth to Mars. On the ellipse, Earth is the periapsis, Mars is the apoapsis and the Sun is one of the foci." horizontal_alignment="right" rights="2004 Geoff Hill, University of Colorado Boulder " caption="Figure 5. An elliptical transfer orbit from the Earth to Mars."/></text_element>
				<text_element>In addition to great engineering and excellent calculations by scientists, it takes good timing to reach Mars. Since the Earth and Mars are both moving, it is like standing on a moving platform and trying to shoot a basketball into a hoop that is moving as well. To make things worse, since it takes about 6 months for a spacecraft to go from the Earth to Mars, scientists and engineers have to anticipate where Mars is going to be when the spacecraft gets there. If we try to shoot a spacecraft right at Mars, by the time it actually gets there, the great Red Planet will be long gone. Once we get to Mars, we must slow down so that we are in an orbit around our destination. From our orbit, we can take photographs of Mars, take scientific readings, or even land on the planet. </text_element>
			</text_block>
		</text_section>
	</lesson_background>
	<vocabulary>
		<definition word="apoapsis">The point in an orbit farthest from the center of attraction (that is, the planet or sun). </definition>
		<definition word="chemical rocket">A rocket that relies on a chemical combustion to create a super-heated, high-pressure gas that is used for thrust.</definition>
		<definition word="cold gas rocket">A rocket that uses escaping pressurized gas as a source of thrust.</definition>
		<definition word="electrical rocket">A rocket that creates thrust by using electricity to accelerate charged particles, which are directed out the back of the vehicle.</definition>
		<definition word="ellipse">A closed curve resembling a flattened circle. Most orbits are in the shape of an ellipse.</definition>
		<definition word="escape velocity">The minimum velocity needed to escape from the gravitational pull of a celestial body (Earth, Sun, etc). </definition>
		<definition word="foci">Two points on an ellipse in which the sum of the distances to the foci from any point on the ellipse is a constant.</definition>
		<definition word="orbit">The path of a planet, moon, spacecraft, or any other object in space as it revolves around another object, such as the sun.</definition>
		<definition word="periapsis">That point in an orbit closest to the center of attraction (that is, the planet or sun). </definition>
		<definition word="specific impulse">A measure of rocket efficiency that is equal to the thrust of the rocket per weight of the fuel.</definition>
		<definition word="thrust">The forward reaction to the rearward movement of exhaust from a rocket engine.</definition>
		<definition word="universal gravitational constant">The constant that relates the gravity of two objects depending on their masses and the distance between them.</definition>
	</vocabulary>
	<child_documents>
		<link url="../../activities/cub_mars/cub_mars_lesson04_activity1.xml" type="activity" description="Students use water balloons and a length of string to understand how gravity and the speed of an orbiting body balance to form an orbit. They also see that when the velocity exceeds the escape velocity, the object will escape the gravity of the sun or planet that it is orbiting around.">The Great Gravity Escape</link>
	</child_documents>
	<lesson_closure>
		<text_section>
			<text_block format="text">
				<text_element>In this lesson, the students should learn what it takes to get a spacecraft from the launch pad to Mars. We learned that rockets use the behavior described in Newton&apos;s third law of motion to propel upward/forward. We covered the basics of orbits and learned that an orbit is where the velocity of the spacecraft and the gravity balance to form an elliptical path. Finally, we talked about elliptical orbits and how elliptical orbits can be used to help us to travel from Earth to Mars.</text_element>
			</text_block>
		</text_section>
	</lesson_closure>
	<summary_assessment>
		<text_section name="Pre-Lesson Assessment">
			<text_block format="text">
				<text_element><italic>Discussion Questions:</italic> Solicit, integrate and summarize student responses.</text_element>
			</text_block>
			<text_block format="unordered">
				<text_element>What does it take for us to get to Mars? What does it take to get a spacecraft off the ground?</text_element>
				<text_element> What do you know about rockets? How do they work? Can you name any rockets? (Answer: US space shuttles: Saturn, Atlas, Titan, Delta, Ariane, Pegasus, etc.) </text_element>
				<text_element>Once a spacecraft is out of the Earth&apos;s atmosphere, it goes into an orbit. What is an orbit? (Answer: An orbit is a curved path on which a planet, star, spacecraft, etc. moves around another object or celestial body.)</text_element>
			</text_block>
			<text_block format="text">
				<text_element><italic>Voting:</italic> Ask a true/false question and have students vote by holding thumbs up for true and thumbs down for false. Count the votes and write the totals on the board. Give the right answer.</text_element>
			</text_block>
			<text_block format="unordered">
				<text_element>Is gravity acting on the space shuttle and its crew? (Answer: Gravity is acting on them and creates the centripetal force that keeps the space shuttle from flying in a straight line off into space. They do not feel it because the inertia of their orbit is perfectly balanced with the centripetal force from gravity.)</text_element>
			</text_block>
		</text_section>
		<text_section name="Post-Introduction Assessment">
			<text_block format="text">
				<text_element><italic>Discussion Question:</italic> Ask the students and discuss as a class:</text_element>
			</text_block>
			<text_block format="unordered">
				<text_element>Why does it take so much energy to get to Mars? (Possible answers: We have to overcome the gravity of Earth; we have to overcome the drag of Earth&apos;s atmosphere; we have to get enough speed to get to Mars in a reasonable time; and/or we have to slow down once we get to Mars so we do not just fly past the planet.)</text_element>
			</text_block>
		</text_section>
		<text_section name="Lesson Summary Assessment">
			<text_block format="text">
				<text_element><italic>Numbered Heads:</italic> Divide the class into teams of three to five students each. Have students on each team pick numbers so each has a different number. Ask the students a question and give them a short time frame for solving it (~1 minute). The members of each team should work together on the question until everyone on the team knows the answer. Call a number at random. Students with that number should raise their hands to answer the question. If not all the students with that number raise their hands, give the teams more time to work on the question. Example questions:</text_element>
			</text_block>
			<text_block format="unordered">
				<text_element>Which of Newton&apos;s laws of motion states that for every action there is an equal and opposite reaction? (Answer: Newton&apos;s third law of motion.)</text_element>
				<text_element>What must a rocket overcome in order to reach orbit? (Answer: Gravity and drag.)</text_element>
				<text_element>What is the force created by a rocket called? (Answer: Thrust.)</text_element>
				<text_element>What do we call the measurement of a rocket&apos;s efficiency? (Answer: Specific impulse.)</text_element>
				<text_element>What happens if a spacecraft in orbit slows down too much? (Answer: If the spacecraft slows down a little it moves into a lower orbit  &#x2014; closer to Earth; if the craft slows down too much it will not be able to maintain an orbit and will crash &#x2014; if they did not mean to slow down &#x2014; or land &#x2014; if they did mean to slow down.)</text_element>
				<text_element> What happens if a spacecraft in orbit reaches the escape velocity? (Answer: The spacecraft will overcome the Earth&apos;s gravity.)</text_element>
				<text_element>What do we call the point on an elliptical orbit that is furthest from the planet/Sun? (Answer: Apoapsis.)</text_element>
				<text_element>What do we call the point on an elliptical orbit that is closest to the planet/Sun? (Answer: Periapsis.)  </text_element>
			</text_block>
		</text_section>
	</summary_assessment>
	<extensions>
		<text_section>
			<text_block format="text">
				<text_element>Besides circular and elliptical orbits, there are also parabolic and hyperbolic orbits. Have students research these types of orbits to determine what is special about them and how they are used.</text_element>
			</text_block>
		</text_section>
	</extensions>
	<references>
		<reference>
			<reference_biblio>National Aeronautics and Space Administration, Mars Exploration Program, </reference_biblio>
			<link url="http://mars.jpl.nasa.gov" type="internet" description="accessed October 4, 2005.">http://mars.jpl.nasa.gov</link>
		</reference>
		<reference>
			<reference_biblio>National Aeronautics and Space Administration, Space Place </reference_biblio>
			<link url="http://spaceplace.nasa.gov/en/kids/orbits1.shtml" type="internet" description="accessed October 4, 2005.">http://spaceplace.nasa.gov/en/kids/orbits1.shtml</link>
		</reference>
		<reference>
			<reference_biblio>Wertz, James R. and Larson, Wiley J. <italic> Space Mission Analysis and Design, 3rd Edition,</italic> Space Technology Library, Volume 8, New York, NY: Springer Publishing Company, 1999.</reference_biblio>
		</reference>
	</references>
	<owner name="Integrated Teaching and Learning Program" organization="College of Engineering, University of Colorado at Boulder"/>
	<contributors>
		<contributor name="Geoffrey Hill"/>
		<contributor name="Daria Kotys-Schwartz"/>
		<contributor name="Chris Yakacki"/>
		<contributor name="Janet Yowell"/>
		<contributor name="Malinda Schaefer Zarske"/>
	</contributors>
	<copyright owner="Regents of the University of Colorado." year="2004" desc="The contents of this digital library curriculum were developed under a grant from the Fund for the Improvement of Postsecondary Education (FIPSE), U.S. Department of Education and National Science Foundation GK-12 grant no. 0330326. However, these contents do not necessarily represent the policies of the Department of Education or National Science Foundation, and you should not assume endorsement by the federal government."/>
</lesson>

