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Accretion Discs - Mathematical Tripos - Past Exam, Exams of Mathematics

This is the Past Exam of Mathematical Tripos which includes Class Field Theory, Artin Map, Abelian Extension of Number Fields, Decomposition Group, Inertia Group, Factorisation of Prime Ideals, Version of Hensel’s Lemma, Hilbert Norm Residue Symbol etc. Key important points are: Accretion Discs, Keplerian Accretion Disc, Negligible Radiation Pressure, Ordinary Differential Equations, Zero Boundary Conditions, Kinematic Viscosity, Dimensionless Constant, Fractional Error

Typology: Exams

2012/2013

Uploaded on 02/27/2013

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MATHEMATICAL TRIPOS Part III
Wednesday 8 June, 2005 1.30 to 3.30
PAPER 73
ACCRETION DISCS
Attempt TWO questions.
There are THREE questions in total.
The questions carry equal weight.
STATIONERY REQUIREMENTS SPECIAL REQUIREMENTS
Cover sheet None
Treasury Tag
Script paper
You may not start to read the questions
printed on the subsequent pages until
instructed to do so by the Invigilator.
pf3

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MATHEMATICAL TRIPOS Part III

Wednesday 8 June, 2005 1.30 to 3.

PAPER 73

ACCRETION DISCS

Attempt TWO questions.

There are THREE questions in total. The questions carry equal weight.

STATIONERY REQUIREMENTS SPECIAL REQUIREMENTS

Cover sheet None Treasury Tag Script paper

You may not start to read the questions

printed on the subsequent pages until

instructed to do so by the Invigilator.

1 The vertical structure of a thin, Keplerian accretion disc with constant (Thomson) opacity and negligible radiation pressure is governed by the equations

∂p ∂z

= −ρΩ^2 z, (1) ∂F ∂z

αΩp, (2)

∂T ∂z

3 κρF 16 σT 3

p =

kρT μmmp

(i) Explain briefly the physical meaning of each equation.

(ii) Show that the problem of the vertical structure of such a disc can be reduced to a universal system of dimensionless ordinary differential equations and boundary conditions by a suitable rescaling of the variables. You may assume that the viscosity parameter α and the mean molecular weight are independent of z and that the ‘zero boundary conditions’ apply at the surfaces of the disc.

(iii) Assuming that the dimensionless system has a unique solution, deduce that the density-weighted mean kinematic viscosity of the disc is of the form

ν¯ = Cα^4 /^3 (GM )−^1 /^3

( (^) κ

σ

) 1 / 3 ( (^) μ mmp k

rΣ^2 /^3 ,

where Σ is the surface density of the disc at a distance r from the central mass M , and C is a dimensionless constant, which need not be determined.

(iv) Equations (1) and (2) involve several approximations that are valid only in the limit of a thin disc. Estimate the order of magnitude of the terms neglected in these equations, and show that the fractional error in each equation is of the order of (H/r)^2 , where H is the semithickness of the disc.

Paper 73