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Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

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Page 1: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Lecture L04 - ASTC25

Physics of TidesTides in the solar system

Roche limit of tidal disruption

Page 2: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption
Page 3: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Damped oscillator as a model equation of tidal wave

braking

Natural frequency of oscillations = sqrt( spring constant)

Deformation (vertical, relative to sphere)

Frequency of forcing = spin frequency = angular speed of planet

forcingFree oscil.

Page 4: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

?

Page 5: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption
Page 6: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Net torque = 0, stable resonance

Page 7: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption
Page 8: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

c

Phobos

Phobos has only ~1 Gyr more to live…

before a crash onto Mars

Page 9: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Io

Europa

Ganimede

Callisto

Page 10: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption
Page 11: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Tidal flexing and heating of Io causesthe most activevolcanism in theSolar System

Page 12: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Roche limit: tidal forces destroy bodies which come too close to a source of gravitation through differential acceleration

Consider an orbiting mass of fluid held together by gravity. Far from the Roche limit the mass is practically spherical. The body is deformed by tidal forces

Within the Roche limit the mass' own gravity (self-gravity) can no longer withstand the tidal forces, and the body disintegrates.

Particles closer to the primary orbit move more quickly than particles farther away, as represented by the red arrows.

The varying orbital speed of the material eventually causes it to form a ring.

http://www.answers.com/topic/roche-limit#wp-Fluid_satellites

Page 13: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

1992

1994

Jupiter disrupted tidally comet Shoemaker-Levy 9 (SL9)

Page 14: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Roche limit:

Fluid limit: tides destroy a body bound byself-gravity withinthat minimumdistance r_R

Solid/rocky limit:the same but with additional binding(electromagnetic) forces of materialstrength

Q: which limit is larger?

First step in the computation is the estimation of the differential torque

Édouard Roche

(1820–1883)

Page 15: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Roche limit

calculation

Page 16: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Comet Shoemaker-Levi SL-9 (1994) disintegrated after approach to Jupiter, and so do the sun-grazing comets.

Roche limit

[pron.: rowsh]

Page 17: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

~2.2 R_p

satellites generally outside the rings

Roche limit for fluid satellite (~1849):

Roche limit for rocky satellite: 1.4

Page 18: Lecture L04 - ASTC25 Physics of Tides Tides in the solar system Roche limit of tidal disruption

Jup

iter

Sat

urn

Ura

nu

s

Nep

tun

e

R_p

2R_p

3R_p

=satellite

rings

0

Roche limit is somewherenear 2 R_p: satellitesdestroyed if closer to their planets.

Ring systems drawn to scale of their planets,

but not to relative scale.