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. Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

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Page 1: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

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Mr. K. NASA/GRC/LTP Edited: Ruth Petersen

Part 4

Pathfinder’s Path I

Page 2: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Preliminary Activities(Use the URL’s provided on Slide 21 to complete

the preliminary activities.)

1.Who were Tycho Brahe and Johannes Kepler? What did they contribute to

modern astronomy and space exploration?

2. Write down Kepler’s three laws of planetary motion. Why are these

laws significant today?

3. What role did Mars play in the discovery of Kepler’s law of

planetary orbits?

Page 3: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

4. Why is Mars significant today?

5. In your algebra class, discuss the conic sections. Write the equation for an ellipse with its center at the origin.

6. What role do the conic sections play in planetary and spacecraft orbits?

Page 4: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Tycho Brahe (1546 - 1607)

Page 5: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Uraniborg - Tycho’s Famous Observatory

Page 6: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Johannes Kepler (1571 - 1630)

Three Laws of Planetary Motion

Every planet travels in an ellipse with the sun at one focus.

The radius vector from the sun to the planet sweeps equal areas in equal times.

The square of the planet’s period is proportional to the cube of its mean distance from the sun.

Page 7: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Kepler’s study of Mars’ orbit lead him to the discovery that planetary orbits

were ellipses.

Actually, we know now that orbits can be any conic section, depending on the

total energy involved.

Page 8: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Circle Ellipse Parabola Hyperbola

The Conic Sections

Page 9: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

(a,0)

(-a,0)

(0,-b)

(0,b)

x

yThe Ellipse

s1s2

P = any point on the ellipse

p

f2f1

f1 & f2 = specific points on the x-

axis

S1 + S2 = Constant

Page 10: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Kepler’s First law: Elliptical Orbits

Sun

Planet

rRadius Vector

vVelocity Vector

The sun is located at one of the two foci of the ellipse.

Page 11: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

“Vis Viva”

v

r

Conservation of Energy: ½mv2 - GMm/r = K

M

m

v = {2(K + GMm/r)/m }1/2

Page 12: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

“Vis Viva” (Continued)

M

v

r

m

Faster

Slower

As r increases, v decreases & vice versa.

How are v and r related?

Page 13: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Pathfinder’s Path:

Departure: December 1996

Page 14: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Pathfinder’s Path:

Arrival: July 1997

Departure: December 1996

Page 15: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Circle Ellipse Parabola Hyperbola

The Conic Sections - Revisited

Closed orbits:

Planets, moons, asteroids, spacecraft.

Open orbits:

Some comets

Parabolic velocity = escape velocity

Page 16: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Follow-Up Activities

1. Earth orbits the sun at a mean distance of 1.5 X 108 km. It completes

one orbit every year. Compute its orbital velocity in km. sec.

2. The Pathfinder required a greater velocity than Earth orbital velocity to achieve its transfer orbit. Why? Since additional velocity costs NASA money

for fuel, can you explain why we launched the spacecraft eastward?

(Hint: When viewed from celestial north, the Earth and planets orbit the sun counter-clockwise.)

Page 17: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

3. The equation for an ellipse with its center at the origin is

(x/a)2 + (x/b)2 = 1

Under what mathematical condition does the ellipse become a circle? (Check

with your algebra teacher if necessary.)

4. Plot the ellipse choosing different values of a and b. (a < b; a = b; a > b).

What do you observe?

5. In the Vis-Viva equation for velocity, how does the velocity vary

around a CIRCULAR orbit?

Page 18: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

6. Extra Credit:The ellipse is defined as a locus of points p such that for

two points, f1 and f2 (the foci), the sum of the distances from f1 and f2 to p is a constant. Use this definition and your knowledge of algebra to show that the

equation of an ellipse follows: i.e., that

(x/a)2 + (y/b)2 = 1

where a and b are the x and y intercepts respectively.

Page 19: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

x

y

(a,0)

(-a,0)

(0,b)

(0,-b)

(f ,0) (f,0)

s1s2

P(x,y)

Solution to #6: The Setup

Page 20: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Solution to #6: The Algebra

Given: s1 + s2 = k (f - x)2 + y2 = s1

2 … (eq. i) (f + x)2 + y2 = s2

2 … (eq. ii)1.) Let (x,y) = (a,o). This gives k = 2a, and

s1 = 2a - s2

2.) Let (x,y) = (0,b). This gives s1 = s2 = (f2+b2)1/2, and f2 = a2 - b2

3.) Result 2.) eq. ii givess2 = a + (x/a)(a2 - b2)1/2

4.) Result 2.) and 3.) eq. ii gives(x/a)2 + (y/b)2 = 1Be careful: The algebra gets messy!

From geometry:

Page 21: Mr. K. NASA/GRC/LTP Edited: Ruth Petersen Part 4 Pathfinder’s Path I

Johannes Kepler:csep10.phys.utk.edu/astr161/lect/history/

kepler.html www.vma.bme.hu/mathhist/Mathematicians/

Kepler.html

Tycho Brahe:http://www-groups.dcs.st-andrews.ac.uk/

~history/Mathematicians/Brahe.html

Hohmannn Transfer Orbits:http://www.jpl.nasa.gov/basics/bsf-

toc.htm