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10/10/2013PHY 113 C Fall 2013-- Lecture 131 PHY 113 C General Physics I 11 AM - 12:15 PM MWF Olin 101 Plan for Lecture 13: Chapter 13 – Fundamental gravitational force law and planetary motion 1.Gravitational force law; relationship with g near Earth’s surface 2.Orbital motion of planets, satellites, etc. 3.Energy associated with gravitation and planetary motion

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10/10/2013 PHY 113 C Fall 2013-- Lecture 132

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10/10/2013PHY 113 C Fall 2013-- Lecture 133 Question from Webassign Assignment #11

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10/10/2013PHY 113 C Fall 2013-- Lecture 134 X 11 33 22

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10/10/2013PHY 113 C Fall 2013-- Lecture 135 X 11 33 22

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10/10/2013PHY 113 C Fall 2013-- Lecture 136 Question from Webassign Assignment #11 X

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10/10/2013PHY 113 C Fall 2013-- Lecture 137 Question from Webassign Assignment #11 iclicker question: A. K i =K f ? B. K i =K f ?

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10/10/2013PHY 113 C Fall 2013-- Lecture 138 Universal law of gravitation Newton (with help from Galileo, Kepler, etc.) 1687

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10/10/2013PHY 113 C Fall 2013-- Lecture 139 Newton’s law of gravitation: m 2 attracts m 1 according to: x y m1m1 m2m2 r2r2 r1r1 r2r1r2r1 G=6.67 x 10 -11 N m 2 /kg 2

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F 12 10/10/2013PHY 113 C Fall 2013-- Lecture 1310 Vector nature of Gravitational law: m1m1 m2m2 m3m3 x y d d F 13

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10/10/2013PHY 113 C Fall 2013-- Lecture 1311 Gravitational force of the Earth RERE m Note: Earth’s gravity acts as a point mass located at the Earth’s center.

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10/10/2013PHY 113 C Fall 2013-- Lecture 1312 Question: Suppose you are flying in an airplane at an altitude of 35000ft~11km above the Earth’s surface. What is the acceleration due to Earth’s gravity? a/g = 0.997

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10/10/2013PHY 113 C Fall 2013-- Lecture 1313 Attraction of moon to the Earth: Acceleration of moon toward the Earth: F = M M a a = 1.99x20 20 N/7.36x10 22 kg =0.0027 m/s 2 R EM

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10/10/2013PHY 113 C Fall 2013-- Lecture 1314

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10/10/2013PHY 113 C Fall 2013-- Lecture 1315 Gravity on the surface of the moon Gravity on the surface of mars

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10/10/2013PHY 113 C Fall 2013-- Lecture 1316 iclicker question: In estimating the gravitational acceleration near the surfaces of the Earth, Moon, or Mars, we used the full mass of the planet or moon, ignoring the shape of its distribution. This is a reasonable approximation because: A.The special form of the gravitational force law makes this mathematically correct. B.Most of the mass of the planets/moon is actually concentrated near the center of the planet/moon. C.It is a very crude approximation.

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10/10/2013PHY 113 C Fall 2013-- Lecture 1317 Stable circular orbit of two gravitationally attracted objects (such as the moon and the Earth) R EM F a v

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10/10/2013PHY 113 C Fall 2013-- Lecture 1318 iclicker question: In the previous discussion, we saw how the moon orbits the Earth in a stable circular orbit because of the radial gravitational attraction of the moon and Newton’s second law: F=ma, where a is the centripetal acceleration of the moon in its circular orbit. Is this the same mechanism which stabilizes airplane travel? Assume that a typical cruising altitude of an airplane is 11 km above the Earth’s surface and that the Earth’s radius is 6370 km. (a) Yes (b) No

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10/10/2013PHY 113 C Fall 2013-- Lecture 1319 Stable (??) circular orbit of two gravitationally attracted objects (such as the airplane and the Earth) R Ea F a v

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10/10/2013PHY 113 C Fall 2013-- Lecture 1320 Newton’s law of gravitation: Earth’s gravity: Stable circular orbits of gravitational attracted objects: RERE m R EM F a v M Summary:

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10/10/2013PHY 113 C Fall 2013-- Lecture 1321 More details If we examine the circular orbit more carefully, we find that the correct analysis is that the stable circular orbit of two gravitationally attracted masses is about their center of mass. m1m1 R2R2 R1R1 m2m2

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10/10/2013PHY 113 C Fall 2013-- Lecture 1322 m1m1 R2R2 R1R1 m2m2 Radial forces on m 1 : T 2 ?

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10/10/2013PHY 113 C Fall 2013-- Lecture 1323 iclicker question: What is the relationship between the periods T 1 and T 2 of the two gravitationally attracted objects rotating about their center of mass? (Assume that m 1 < m 2.) (A) T 1 =T 2 (B) T 1 T 2 m1m1 R2R2 R1R1 m2m2

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10/10/2013PHY 113 C Fall 2013-- Lecture 1324 m1m1 R2R2 R1R1 m2m2

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10/10/2013PHY 113 C Fall 2013-- Lecture 1325 iclicker questions: How is it possible that all of these relations are equal? A.Magic. B.Trick. C.Algebra.

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10/10/2013PHY 113 C Fall 2013-- Lecture 1326 m1m1 R2R2 R1R1 m2m2 For m 2 >>m 1 R 2 << R 1 : m2m2 m1m1 R1R1 Larger mass

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10/10/2013PHY 113 C Fall 2013-- Lecture 1327 What is the physical basis for stable circular orbits? 1.Newton’s second law? 2.Conservation of angular momentum? L = (const) Note: Gravitational forces exert no torque

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10/10/2013PHY 113 C Fall 2013-- Lecture 1328 m1m1 R2R2 R1R1 m2m2 v1v1 v2v2 L 1 =m 1 v 1 R 1 L 2 =m 2 v 2 R 2 L = L 1 + L 2 Question: How are the magnitudes of L 1 and L 2 related? Note: More generally, stable orbits can be elliptical.

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10/10/2013PHY 113 C Fall 2013-- Lecture 1329 Satellites orbiting earth (approximately circular orbits): R E ~ 6370 km Examples: Satellite h (km)T (hours)v (mi/h) Geosynchronous35790 ~24 6900 NOAA polar orbitor 800 ~1.716700 Hubble 600 ~1.616900 Inter. space station * 390 ~1.517200

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10/10/2013PHY 113 C Fall 2013-- Lecture 1330 Planets in our solar system – orbiting the sun PlanetMass (kg)Distance to Sun (m) Period of orbit (years) Mercury3.30x10 23 5.79x10 10 0.24 Venus4.87x10 24 1.08x10 11 0.61 Earth5.97x10 24 1.496x10 11 1.00 Mars6.42x10 23 2.28x10 11 1.88 Jupter1.90x10 27 7.78x10 11 11.85 Saturn5.68x10 26 1.43x10 12 29.43

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10/10/2013PHY 113 C Fall 2013-- Lecture 1331 m1m1 R2R2 R1R1 m2m2 v1v1 v2v2 Review: Circular orbital motion about center of mass CM

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10/10/2013PHY 113 C Fall 2013-- Lecture 1332 m1m1 R1R1 m2m2 v1v1 Review: Circular orbital motion about center of mass

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10/10/2013PHY 113 C Fall 2013-- Lecture 1333 Example: Satellite in circular Earth orbit

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10/10/2013PHY 113 C Fall 2013-- Lecture 1334 Work of gravity: riri rfrf

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10/10/2013PHY 113 C Fall 2013-- Lecture 1335 Gravitational potential energy Example:

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10/10/2013PHY 113 C Fall 2013-- Lecture 1336 h U=mgh iclicker exercise: We previously have said that the gravitational potential of an object of mass m at a height h is U=mgh. How is this related to A.No relation B.They are approximately equal C.They are exactly equal

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10/10/2013PHY 113 C Fall 2013-- Lecture 1337 h g Near the surface of the Earth U=mgh is a good approximation to the gravitation potential.

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10/10/2013PHY 113 C Fall 2013-- Lecture 1338 iclicker exercise: How much energy kinetic energy must be provided to an object of mass m=1000kg, initially on the Earth’s surface to outer space? A.This is rocket science and not a fair question. B.It is not possible to escape the Earth’s gravitational field. C.We can estimate the energy by simple conservation of energy concepts.

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10/10/2013PHY 113 C Fall 2013-- Lecture 1339 Total energy of a satellite in a circular Earth orbit

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10/10/2013PHY 113 C Fall 2013-- Lecture 1340 Total energy of a satellite in a circular Earth orbit iclicker question: Compared to the energy needed to escape the Earth’s gravitational field does it take A.more B.less energy to launch a satellite to orbit the Earth?

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10/10/2013PHY 113 C Fall 2013-- Lecture 1341

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10/10/2013PHY 113 C Fall 2013-- Lecture 1342 Energy involved with changing orbits h’

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10/10/2013PHY 113 C Fall 2013-- Lecture 1343 Stable Elliptical Orbits

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