querent

Spam yourself with math PhD qualifying-exam questions.

Showing 251โ€“260 of 816
Stanford Practice, 20 Applied mathematics, Gagliardo-Nirenberg inequality, parabolic PDE, L^infinity decay

(i) Find a unique pair of numbers ๐›ผ๐‘›>0 and ๐›ฝ๐‘›>0 such that an inequality of the form

โˆซโ„๐‘›|๐‘ข(๐‘ฅ)|2d๐‘ฅโ‰ค๐ถ๐‘›(โˆซโ„๐‘›|โˆ‡๐‘ข(๐‘ฅ)|2d๐‘ฅ)๐›ผ๐‘›(โˆซโ„๐‘›|๐‘ข(๐‘ฅ)|d๐‘ฅ)๐›ฝ๐‘›

holds for all ๐‘ขโˆˆ๐’ฎ๏ธ€(โ„๐‘›).

(ii) Show that this inequality does hold.

(iii) Use that inequality to show that a smooth rapidly decaying solution to a parabolic equation of the form

๐œ•๐‘ข๐œ•๐‘ก=โˆ‡โ‹…(๐‘Ž(๐‘ฅ)โˆ‡๐‘ข),๐‘ก>0,๐‘ฅโˆˆโ„๐‘›,

satisfies an estimate of the form

โ€–๐‘ข(๐‘ก,โ‹…)โ€–๐ฟโˆžโ‰ค๐ถ[๐‘Ž]๐‘ก๐‘›/2,

with a constant ๐ถ[๐‘Ž] that depends only on the ellipticity constant ฮ› of the matrix ๐‘Ž(๐‘ฅ). In other words, for all ๐‘ฅโˆˆโ„๐‘› and ๐œ‰โˆˆโ„๐‘› we have

ฮ›โˆ’1|๐œ‰|2โ‰ค(๐‘Ž(๐‘ฅ)๐œ‰โ‹…๐œ‰)โ‰คฮ›|๐œ‰|2.
Stanford Practice, 21 Applied mathematics, viscous Burgers' equation, smoothing effect, Oleinik inequality

Consider the solutions to the viscous Burgers' equation

๐œ•๐‘ข๐œ•๐‘ก+๐‘ข๐œ•๐‘ข๐œ•๐‘ฅ=๐œˆ๐œ•2๐‘ข๐œ•๐‘ฅ2,

in dimension one, with some ๐œˆ>0.

(i) Show that if ๐‘ข(0,๐‘ฅ)=๐‘ข0(๐‘ฅ) is continuously differentiable, then ๐‘ข(๐‘ก,๐‘ฅ) is infinitely differentiable for all ๐‘ก>0.

(ii) Show that for all ๐‘ก>0, ๐‘ฅโˆˆโ„ and ๐‘ฆ>0 we have

๐‘ข(๐‘ก,๐‘ฅ+๐‘ฆ)โˆ’๐‘ข(๐‘ก,๐‘ฅ)๐‘ฆโ‰ค1๐‘ก.
Stanford Practice, 22 Applied mathematics, interpolation inequalities, transition layers

Show that there is a constant ๐ถ>0 so that for any smooth function ๐‘ข(๐‘ฅ) such that ๐‘ข(๐‘ฅ)โ†’1 as ๐‘ฅโ†’โˆ’โˆž and ๐‘ข(๐‘ฅ)โ†’0 as ๐‘ฅโ†’+โˆž, we have

(โˆซโ„|๐‘ข๐‘ฅ|2d๐‘ฅ)(โˆซโ„๐‘ข(1โˆ’๐‘ข)d๐‘ฅ)โ‰ฅ๐ถ.
Stanford Practice, 23 Applied mathematics, Euler-Lagrange equations, calculus of variations

Find the Euler-Lagrange equations for the functional

๐ผ[๐‘ข]=โˆซฮฉ๐น(๐‘ฅ,โˆ‡๐‘ข(๐‘ฅ))d๐‘ฅ,

with two different functionals

๐น1(๐‘ฅ,๐‘)=12(๐ด(๐‘ฅ)๐‘โ‹…๐‘),๐‘ฅโˆˆฮฉ,๐‘โˆˆโ„๐‘›,

and

๐น2(๐‘ฅ,๐‘)=12det(๐ด(๐‘ฅ))(๐ด(๐‘ฅ)๐‘โ‹…๐‘).
Stanford Practice, 24 Applied mathematics, distributions, weak derivatives

Show that if a distribution ๐œ‘โˆˆ๐’Ÿ๏ธ€โ€ฒ(โ„) satisfies ๐œ‘โ€ฒ=0 (in the sense of distributions), then ๐œ‘=๐‘, where ๐‘โˆˆโ„ is a constant.

Stanford Practice, 25 Applied mathematics, conservation laws, entropy solutions, Burgers equation

(i) Let ๐‘ข(๐‘ก,๐‘ฅ) be a smooth solution to a conservation law

๐‘ข๐‘ก+(๐‘“(๐‘ข))๐‘ฅ=0.

Assume that ๐‘“โˆˆ๐ถ2(โ„) and ๐‘“โ€ณโ‰ 0. Show that ๐‘ฃ=๐‘“โ€ฒ(๐‘ข) is a solution to the Burgers equation

๐‘ฃ๐‘ก+(๐‘ฃ2/2)๐‘ฅ=0.

(ii) Now, suppose that ๐‘ข(๐‘ก,๐‘ฅ) is not a smooth solution to this conservation law but rather an entropy solution. Is then ๐‘ฃ=๐‘“โ€ฒ(๐‘ข) an entropy solution to the Burgers equation?

Stanford Practice, 26 Applied mathematics, Lax pairs, Toda lattice, integrable systems, conserved quantities

We use the notation [๐ด,๐ต]=๐ด๐ตโˆ’๐ต๐ด for the commutator of two operators ๐ด and ๐ต.

(i) Suppose that an ๐‘›ร—๐‘› symmetric real-valued matrix ๐ฟ(๐‘ก) satisfies an ODE of the form

d๐ฟ(๐‘ก)d๐‘ก=[๐ฟ(๐‘ก),๐ด(๐‘ก)],

with some ๐‘›ร—๐‘› matrix ๐ด(๐‘ก). Show that the eigenvalues ๐œ†๐‘˜(๐‘ก) of the matrix ๐ฟ(๐‘ก) do not depend on ๐‘ก. Is the same true for the eigenvectors of ๐ฟ(๐‘ก)?

(ii) Consider a system of ๐‘ particles located at positions ๐‘ž๐‘˜(๐‘ก), ๐‘˜=1,โ€ฆ,๐‘, on the real line. Let us denote their momenta by ๐‘๐‘˜(๐‘ก), ๐‘˜=1,โ€ฆ,๐‘. The Hamiltonian governing their motion is

๐ป(๐‘,๐‘ž)=12โˆ‘๐‘˜=1๐‘|๐‘๐‘˜|2+โˆ‘๐‘˜=1๐‘โˆ’1exp(2(๐‘ž๐‘˜โˆ’๐‘ž๐‘˜+1)),

and the equations of motion are

๐‘žฬ‡๐‘˜(๐‘ก)=๐œ•๐ป(๐‘,๐‘ž)๐œ•๐‘ž๐‘˜,๐‘ฬ‡๐‘˜(๐‘ก)=โˆ’๐œ•๐ป(๐‘,๐‘ž)๐œ•๐‘๐‘˜.

Let ๐ฟ(๐‘ก) be the symmetric tri-diagonal ๐‘ร—๐‘ matrix with the diagonal entries

๐ฟ๐‘˜๐‘˜=๐‘๐‘˜,๐‘˜=1,โ€ฆ,๐‘,

and the entries just above and just below the main diagonal equal to

๐ฟ๐‘˜,๐‘˜+1=๐ฟ๐‘˜+1,๐‘˜=exp(๐‘ž๐‘˜โˆ’๐‘ž๐‘˜+1),๐‘˜=1,โ€ฆ,๐‘โˆ’1.

All other entries of ๐ฟ(๐‘ก) are equal to zero. Find a matrix ๐‘ƒ(๐‘ก) such that the system can be written as

d๐ฟ(๐‘ก)d๐‘ก=๐ฟ(๐‘ก)๐‘ƒ(๐‘ก)โˆ’๐‘ƒ(๐‘ก)๐ฟ(๐‘ก).

(iii) It follows from part (ii) of this problem that Tr(๐ฟ๐‘˜(๐‘ก)) does not depend on time for all ๐‘˜โ‰ฅ1. Compute these conserved quantities explicitly in terms of ๐‘๐‘— and ๐‘ž๐‘— for ๐‘˜=1, ๐‘˜=2 and ๐‘˜=3.

Stanford Practice, 27 Applied mathematics, Lax pairs, KdV equation, integrable systems

Consider the following dispersive regularization of the Burgers equation:

๐‘ข๐‘ก+๐‘ข๐‘ข๐‘ฅ+๐œ€๐‘ข๐‘ฅ๐‘ฅ๐‘ฅ=0.

Find a third order in ๐œ•๐‘ฅ differential operator ๐ด(๐‘ก) of the form

๐ด(๐‘ก)=๐‘Ž3(๐‘ก,๐‘ฅ)๐œ•๐‘ฅ3+๐‘Ž2(๐‘ก,๐‘ฅ)๐œ•๐‘ฅ2+๐‘Ž1(๐‘ก,๐‘ฅ)๐œ•๐‘ฅ+๐‘Ž0(๐‘ก,๐‘ฅ),

and an operator

๐ฟ(๐‘ก)=๐‘š1๐œ•๐‘ฅ2+๐‘š2๐‘ข(๐‘ก,๐‘ฅ),

with the coefficients ๐‘Ž๐‘—(๐‘ก,๐‘ฅ), ๐‘—=0,1,2,3 that depend on ๐‘ข(๐‘ก,๐‘ฅ), and fixed ๐‘š1,2โˆˆโ„, so that this equation can be written as

๐œ•๐ฟ(๐‘ก)๐œ•๐‘ก=[๐ฟ(๐‘ก),๐ด(๐‘ก)].
Stanford Practice, 28 Applied mathematics, Brownian motion, exit times, harmonic functions

Fix 0<๐‘Ÿ<๐‘… and let ๐œ(๐‘ฅ;๐œ”) be the time it takes for the standard Brownian motion ๐ต(๐‘ก;๐‘ฅ) starting at the point ๐‘ฅโˆˆ(๐‘Ÿ,๐‘…) to exit the interval [๐‘Ÿ,๐‘…].

(i) Find โ„™(๐ต(๐œ(๐‘ฅ;๐œ”))=๐‘Ÿ).

(ii) Find ๐‘ข(๐‘ก,๐‘ฅ)=โ„™(๐œ(๐‘ฅ;๐œ”)>๐‘ก), for a given ๐‘ก>0.

(iii) What is ๐”ผ(๐œ(๐‘ฅ;๐œ”))?

Stanford Practice, 29 Applied mathematics, Brownian motion, martingales

Let ๐ต๐‘ก be the standard Brownian motion.

(i) Find all ๐‘Žโˆˆโ„ and ๐‘โˆˆโ„ such that

๐‘€๐‘ก=๐‘’๐‘Ž๐‘ก+๐‘๐ต๐‘ก

is a martingale.

(ii) For which ๐‘šโˆˆโ„• does there exist a deterministic function ๐‘”๐‘š(๐‘ก) such that ๐ฟ๐‘š(๐‘ก)=๐ต๐‘ก๐‘šโˆ’๐‘”๐‘š(๐‘ก) is a martingale?

Questions per page