If two (spherical) asteroids are in contact and are attracted with a force of 1 Newton, how much more or less force would they experience if they both had been twice as large (assuming the same density)? - PowerPoint PPT Presentation

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If two (spherical) asteroids are in contact and are attracted with a force of 1 Newton, how much more or less force would they experience if they both had been twice as large (assuming the same density)?

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Title: If two (spherical) asteroids are in contact and are attracted with a force of 1 Newton, how much more or less force would they experience if they both had been twice as large (assuming the same density)?


1
If two (spherical) asteroids are in contact and
are attracted with a force of 1 Newton, how much
more or less force would they experience if they
both had been twice as large (assuming the same
density)?
Physics 1710Warm-up Quiz

0
  1. The same
  2. Twice as much (2x)
  3. Half as much (1/2x)
  4. 4 x
  5. 8 x
  6. 16 x

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20
21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40
2
Physics 1710Chapter 12 Apps Gravity
0
  • Solution

F G M1 M2 /r2 M1 M2 4p/3 ?R3 R r F G
(4p/3 ?R3)2 /R2 F?R4 F2/F1 (R2/R1)4 24 16
3
Physics 1710Chapter 13 Apps Gravity
0
  • 1' Lecture
  • Fg - rG Mm/d 2
  • G 6.673 x 10 11 N m2 /kg2 2/3 x 10 10 N m2
    /kg2
  • The gravitational force constant g is equal to
    g G M/(Rh) 2, M and R are the mass and radius
    of the planet.
  • The gravitation field is the force divided by the
    mass.
  • The gravitation potential energy for a point mass
    is proportional to the product of the masses and
    inversely proportional to the distance between
    their centers.

4
Physics 1710Chapter 13 Apps Gravity
0
  • 1' Lecture (contd.)
  • Keplers Laws
  • The orbits of the planets are ellipses.
  • The areal velocity of a planet is constant.
  • The cube of the radius r 3 of a planets orbit
  • is proportional to the square of the period T 2.

5
Which best corresponds to the actual shape of a
planets orbit?
Physics 1710Chapter 13 Apps Gravity

0
  1. None of the above.

81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100
101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120
6
Physics 1710Chapter 12 Apps Gravity
0
  • Solution

Keplers First Law The orbits of the planets are
ellipses. r ro /1e cos ? e eccentricity
Planet e ? 0.2056? 0.0068? 0.0934? 0.0483
? 0.0560? 0.0461? 0.0097? 0.2482

ro
ro/(1e)
ro/(1-e)
ro
7
Physics 1710Chapter 12 Apps Gravity
0
  • History

Keplers First Law The orbits of the planets are
ellipses. What is the significance?
Repudiation of Aristotle
F is inverse square law
8
Physics 1710Chapter 13 Apps Gravity
0
  • Isaac Newtons
  • Universal Law of GravitationF - G M m/ d 2

d moon
9
Physics 1710Chapter 13 Apps Gravity
0
  • Keplers Laws
  • The orbits are ellipses.
  • The areal velocity is a constant.
  • T 2 ? r 3 implies F ? 1/ r 2, only.

10
Physics 1710Chapter 12 Apps Gravity
0
  • Comment

Keplers Second Law The areal velocity is
constant. ½ r2 ? constant.
Why? mr2 ? L constant. L is conserved if no
torque, i.e. F is central force.

11
Physics 1710Chapter 13 Apps Gravity
0
  • Keplers Laws
  • The orbits are ellipses. (Contrary to Aristotle
    and Ptolemy.)
  • A central force F ? 1/ r 2 or r 2
  • The areal velocity is a constant.
  • Angular momentum is conserved
  • ½ v r ?t constant implies that
  • rmv L constant.
  • T 2 ? r 3 implies F ? 1/ r 2, only.

?
r3
T 2
12
Physics 1710Chapter 12 Apps Gravity
0
  • How did Newton figure out UL of G?
  • Fact a moon circling a planet has an
    acceleration of a v 2 /r
  • Fact a F/m.
  • Fact Kepler had found that the square of the
    period T was proportional to the cube of the
    radius of the orbit r
  • T 2 k r 3 .
  • Thus
  • v 2p r / T

13
Physics 1710Chapter 12 Apps Gravity
0
  • And
  • T 2 (2pr) 2 /(F r /m) k r 3
  • Thus
  • F (2p) 2 m/(k r 2 )
  • An inverse square law, with k 1/ (2p) 2G
    M
  • F G Mm/ r 2 ,
  • But what value is G?

14
Physics 1710Chapter 13 Apps Gravity
0
  • Isaac Newtons
  • Universal Law of GravitationF - G M m/ d 2

d moon
F g m g G M ? / R? 2
15
Physics 1710Chapter 12 Apps Gravity
0
  • Gravitation

g? G M?/ R?2 G M? gR? 2 (9.80 N/kg)(6.37x10
6 m) 3.99x10 14 N m 2/kg
Need to know G or M.
16
Physics 1710Chapter 13 Apps Gravity
0
  • Henry Cavendish
  • And the
  • Cavendish Experiment

M
m
d
17
Physics 1710Chapter 13 Apps Gravity
0
  • G 6.673 x 10 -11 N ?m 2 /kg 2
  • G 2/3 x 10 -10 N ?m 2 /kg 2
  • (to an accuracy of 0.1)

So, M? (3.99x10 14 N m 2/kg)/(6.673 x 10-11 N
?m 2/kg 2) 5.98 x10 24 kg
18
Physics 1710Chapter 13 Apps Gravity
0
  • What is g? on Mars? M ? 0.107 M? , R ? 0.532
    R ?

Peer Instruction Time
19
What is g? on Mars?
Physics 1710Chapter 13 Apps Gravity

0
  1. 25.9 m/sec2
  2. 9.80 m/sec2
  3. 3.70 m/sec2
  4. 1.97 m/sec2
  5. None of the above.

41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80
20
Physics 1710Chapter 13 Apps Gravity
0
  • What is g? on Mars?

g?/g? (M?/M?)(R?/R ?)2 (0.107)(1/0.532)2
0.378 g? 3.70 m/sec2
M?
M?
Peer Instruction Time
21
Physics 1710Chapter 13 Apps Gravity
0
  • Gravitational Force

F - G M m/ d 2 What is the order of magnitude
of the attraction between two people (m 100 kg)
separated by a distance of 1m?
M
m
d
22
What is the order of magnitude of the attraction
between two people (m 100 kg) separated by a
distance of 1m?
Physics 1710Chapter 13 Apps Gravity

0
  1. 9.8 N.
  2. 980. N
  3. 6.7 X 10 - 7 N
  4. 6.7 X 10 - 9 N
  5. None of the above

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20
21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40
23
Physics 1710Chapter 13 Apps Gravity
0
  • Gravitational Force

F - G M m/ d 2 F - (6.67 x10 11 N ?m 2 /kg
2)(100 kg)(100kg )/(1 m) 2 F - 6.67 x10 7 N
Equivalent weight F/g 67 ng
M
m
d
24
Physics 1710Chapter 13 Apps Gravity
  • Gravitational Potential Energy
  • U -?8R Fd r
  • U -?8R G Mm/r 2d r
  • U GMm/R
  • U 0 as r ?8

25
Physics 1710Chapter 13 Apps Gravity
  • Total Energy
  • for Gravitationally Bound Mass
  • E K U
  • E ½ m v 2 GMm/r
  • E L2/2mr 2 GMm/r
  • Bound orbit if E 0 and
  • - dE/dr ro 2 (L2/2mro) - GMm 0
  • E - GMm/2ro

26
Physics 1710Chapter 13 Apps Gravity
0
  • Total Energy
  • for Gravitationally Bound Mass
  • E K UE - GMm/2ro

E - L2 /2mr 2 lt GMm/r
ro - 2E/(GMm)
27
Physics 1710Chapter 13 Apps Gravity
  • Escape Velocity
  • If K is such that E gt 0, then
  • K ½ m v 2 GMm/ r
  • Thus at r R
  • v v 2GM/R

28
Physics 1710Chapter 13 Apps Gravity
  • Summary
  • The force of attraction between two bodies with
    mass M and m respectively is proportional to the
    product of their masses and inversely
    proportional to the distance between their
    centers squared.
  • F - G M m/ r 2
  • The proportionality constant in the Universal
    Law of Gravitation G is equal to 6.673 x 10 11 N
    m2 /kg2 .

29
Physics 1710Chapter 13 Apps Gravity
  • Summary
  • The gravitational force constant g is equal to
  • G M/(Rh) 2, R is the radius of the planet.
  • Keplers Laws
  • The orbits of the planets are ellipses.
  • The areal velocity of a planet is constant.
  • The cube of the radius of a planets orbit
  • is proportional to the square of the period.
  • The gravitation field is the force divided by
    the mass.
  • g Fg / m

30
Physics 1710Chapter 13 Apps Gravity
  • Summary
  • The gravitation potential energy for a point
    mass is proportional to the product of the masses
    and inversely proportional to the distance
    between their centers
  • U GMm / r
  • The escape velocity is the minimum speed a
    projectile must have at the surface of a planet
    to escape the gravitational field.
  • v v 2GM/R
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