ENERGY CONSERVATIVE SOLUTIONS TO A NONLINEAR WAVE SYSTEM OF NEMATIC LIQUID CRYSTALS
|
|
- Tyler Phillips
- 6 years ago
- Views:
Transcription
1 ENERGY CONSERVATIVE SOLUTIONS TO A NONLINEAR WAVE SYSTEM OF NEMATIC LIQUID CRYSTALS GENG CHEN, PING ZHANG, AND YUXI ZHENG Abstract. We establish the global existence of solutions to the Cauchy problem for a system of hyperbolic partial differential equations in one space dimension modeling a type of nematic liquid crystals that has equal splay and twist coefficients. Our results have no restrictions on the angles of the director, as we use the director in its natural three-component form, rather than the two-component form of spherical angles.. Introduction In this paper, we consider the global existence of energy conservative weak solutions to the following one-dimensional wave system of liquid crystals tt n x c 2 x n ) = n t 2 + 2c 2 γ) n x 2) n,.) tt n 2 x c 2 x n 2 ) = n t 2 + 2c 2 α) n x 2) n 2, tt n 3 x c 2 x n 3 ) = n t 2 + 2c 2 α) n x 2) n 3, together with initial data.2) n i t=0 = n i0 H, n i ) t t=0 = n i L 2, i =, 2, 3, where c depends on n with c 2 = α + γ α)n 2, α > 0, γ > 0, and n = n, n 2, n 3 ) with.3) n =. Subscripts t or x represent partial derivatives with respect to t or x, and tt = t t. We firstly mention briefly the origin of this system. The mean orientation of the long molecules in a nematic liquid crystal is described by a director field of unit vectors, n S 2, the unit sphere. Associated with the director field n, there is the well-known Oseen-Franck potential energy density W given by.) W n, n) = 2 α n)2 + 2 β n n)2 + 2 γ n n) 2. The positive constants α, β, and γ are elastic constants of the liquid crystal, corresponding to splay, twist, and bend, respectively. For the special case α = β = γ, the potential energy density reduces to W n, n) = 2 α n 2, which is the potential energy density used in harmonic maps into S 2. There are many studies on the constrained elliptic system of equations for n derived through variational principles from the potential.), and on the parabolic flow associated with it, see [2, 5, 6, 8, 9, 7 and references therein. In the regime in which inertia effects dominate viscosity, however, the propagation of the orientation waves in the director field may then be modelled by the least action principle [0, ) { } δ.5) δn 2 tn t n W n, n) dx dt = 0, n n =. R Date: March 9, 202.
2 2 G. CHEN, P. ZHANG, AND Y. ZHENG In the special case α = β = γ, this variational principle.5) yields the equation for harmonic wave maps from +3)-dimensional Minkowski space into S 2, see [,, 2 for example. One may also check [3,, 5, 6 for wave maps in dimension + 2). For planar deformations depending on a single space variable x, i.e, the director field has the special form n = cos ux, t)e x + sin ux, t)e y, where the dependent variable u R measures the angle of the director field to the x- direction, and e x and e y are the coordinate vectors in the x and y directions, respectively, one finds that the variational principle.5) yields.6) u tt c c u x ) x = 0 with the wave speed c given specifically by.7) c 2 u) = γ cos 2 u + α sin 2 u. If we let n be arbitrary in S 2 while maintaining dependence on a single space variable x, i.e.,.8) n = cos u, sin u cos v, sin u sin v) where u, v) are both functions of x, t), we find that the Lagrangian density of.5) is.9) 2 tn t n W n, n) = [ u 2 2 t c 2 u)u 2 x + 2 a2 u) [ vt 2 c 2 2u)vx 2 where.0) c 2 u) = γ cos 2 u + α sin 2 u, c 2 2u) = γ cos 2 u + β sin 2 u, a 2 u) = sin 2 u. The Euler-Lagrange equations are { utt c u)c u)u x ) x = aa vt 2 c 2 2 v2 x) a 2 c 2 c 2 v2 x,.) a 2 v t ) t c 2 2 a2 v x ) x = 0. See Alì and Hunter [ for more details on the derivation of the above system. Under the additional assumption that c u) 0, Zhang and Zheng established the global existence of energy dissipative weak solutions to.6) in [8, 9. Without any additional assumption, Bressan and Zheng established the global existence of energy conservative weak solutions to.6) in [3. In [20, 2, Zhang and Zheng solved the global existence of energy conservative solutions to.) under the un-physical assumption that au) a min > 0 and c 2 < c for [2). The goal of this paper is to get rid of this assumption in [20. Indeed.5) can be equivalently reformulated as { δ δn 2 tn t n W n, x n) + λ } 2 n 2 ) dx dt = 0, R 2 which gives rise to the Euler-Langrage equations.2) tt n i + ni W n, x n) x [ xn i W n, x n) = λn i, for i =, 2, 3. Using n =, multiplying.2) with n i, and summing them up for i from to 3, we obtain 3 {.3) λ = t n i 2 [ + n i ni W n, x n) n i x xni W n, x n) }. i= It is easy to calculate that.2) has the following energy conservation law: [.) t 2 n t 2 + W n, x n) [ 3 x t n i xni W n, x n) = 0. i=
3 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 3 On the other hand, we use.) in the one-dimensional case to obtain.5) W n, x n) = α 2 xn ) 2 + β 2 [ x n 2 ) 2 + x n 3 ) γ β)n2 n x 2, from which and.3), we infer.6) λ = n t 2 + β + 2γ β)n 2 ) nx 2 + β α)n 2 xn. Combining.2),.5) and.6), we have.7) tt n x [ c 2 x n = { nt 2 + 2c 2 2 γ) n x 2 + 2α β) x n ) 2} n with Similarly, we have.8) c 2 def = α + γ α)n 2 and c 2 2 = β + γ β)n 2. tt n 2 x [ c 2 2 x n 2 = { nt 2 + 2c 2 2 β) n x 2 + β α)n xx n } n2, tt n 3 x [ c 2 2 x n 3 = { nt 2 + 2c 2 2 β) n x 2 + β α)n xx n } n3. In particular, taking α = β in.7) and.8) leads to.). When α = β, the two speeds are equal, so we let.9) c 2 = c 2 = c 2 2 = α + γ α)n 2, and it follows that.20) 0 < min{α, γ} c 2 max{α, γ} < ; max{ c } <, for any n. The energy equation.) becomes.2) 2 [ t nt 2 + c 2 n x 2 [ x c 2 n t n x = 0, where the energy density W in.5) becomes.22) W n, x n) = 2 c2 x n 2. We consider in this paper the global existence of energy-conservative weak solutions of.).3) to its initial value problem with data.2). Since some smooth initial data for equation.6) is known to form singularity later in time, it is easy to see that the same is true for system.) and.). Thus we shall give up classical solutions and consider weak solutions instead. Definition. Weak solution). The vector function nt, x), defined for all t, x) R R, is a weak solution to the Cauchy problem.).3) if it satisfies i): In the t-x plane, the functions n, n 2, n 3 ) are locally Hölder continuous with exponent /2. This solution t n, n 2, n 3 )t, ) is continuously differentiable as a map with values in L p loc, for all p < 2. Moreover, it is Lipschitz continuous with.23) respect to w.r.t.) the L 2 distance, i.e. n i t, ) n i s, ) L 2 L t s, i = 3, for all t, s R. ii): The functions n, n 2, n 3 ) take on the initial conditions in.2) pointwise, while their temporal derivatives hold in L p loc for p [, 2[. iii): The equations.) hold in distributional sense for test functions φ Cc R R).
4 G. CHEN, P. ZHANG, AND Y. ZHENG Our conclusions are as follows. Theorem. Existence). The problem.).3) has a global weak solution defined for all t, x) [0, ) R. We shall use the method of energy-dependent coordinates, used in papers [3 and related Camassa-Holm equation, to dilate the singularity in building the solution. Our constructive procedure yields solutions which depend continuously on the initial data. Moreover, the energy.2) Et) := 2 [ n t 2 + c 2 n x 2 dx remains uniformly bounded by its initial level:.25) E 0 := 2 [ n x) 2 + c 2 n 0 x)) n 0 x)) x 2 dx. More precisely, we have Theorem.2 Continuous dependence). A family of weak solutions to the Cauchy problem.).3) can be constructed with the additional properties: For every t R we have.26) Et) E 0. Moreover, let a sequence of initial conditions satisfy k n i0 ) x n i0 ) L x 2 0, k ni n L i 2 0, i = 3, and n k 0 n 0 uniformly on compact sets, as k. Then we have the convergence of the corresponding solutions n k n, uniformly on bounded subsets of the t-x plane. It appears in.26) that the total energy of our solutions may decrease in time. Yet, we emphasize that our solutions are conservative, in the following sense. Theorem.3 Conservation of energy). There exists a continuous family {µ t ; t R} of positive Radon measures on the real line with the following properties. i): At every time t, we have µ t R) = E 0. ii): For each t, the absolutely continuous part of µ t has density 2 nt 2 + c 2 n x 2) w.r.t. Lebesgue measure. iii): For almost every t R, the singular part of µ t is concentrated on the set where n = 0 or ±, when α γ. In other words, the total energy represented by the measure µ is conserved in time. Occasionally, some of this energy is concentrated on a set of measure zero. At those times τ when this happens, µ τ has a non-trivial singular part and Eτ) < E 0. Condition iii) places some restrictions on the set of such times τ. The paper is organized as follows. In Section 2 we introduce a new set of independent and dependent variables, and derive some identities valid for smooth solutions. We formulate a set of equations in the new variables which is equivalent to.). Remarkably, in the new variables all singularities disappear: Smooth initial data lead to globally smooth solutions. In Section 3, we prove the existence of the solutions in the energy coordinates. In Sections 7, we present proofs to Theorems..3.
5 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 5 2. New formulation in energy-dependent coordinates 2.. Energy-dependent coordinates. We denote 2.) R = R, R 2, R 3 ) def = n t + cn x, S = S, S 2, S 3 ) def = n t cn x. Then.) can be reformulated as: t R c x R = c 2 { c 2 γ) R 2 + S 2 ) 23c 2 γ) R S } n 2.2) + c 2c R S )R, t S + c x S = c 2 { c 2 γ) R 2 + S 2 ) 23c 2 γ) R S } n c 2c R S )S, t R 2 c x R 2 = c 2 { c 2 α) R 2 + S 2 ) 23c 2 α) R S } n 2 + c 2c R 2 S 2 )R, t S 2 + c x S 2 = c 2 { c 2 α) R 2 + S 2 ) 23c 2 α) R S } n 2 c 2c R 2 S 2 )S, t R 3 c x R 3 = c 2 { c 2 α) R 2 + S 2 ) 23c 2 α) R S } n 3 + c 2c R 3 S 3 )R, t S 3 + c x S 3 = c 2 { c 2 α) R 2 + S 2 ) 23c 2 α) R S } n 3 n x = R S 2c or n t = R+ S 2. c 2c R 3 S 3 )S, Similar to.), system 2.2) has the following form of energy conservation law: 2.3) t R 2 + S 2) [ x cn ) R 2 S 2 ) = 0. We define the forward and backward characteristics as follows { d ds x± s, t, x) = ±cn s, x ± s, t, x))), 2.) x ± s=t = x. Then we define the coordinate transformation: X def = This implies x 0,t,x) 0 [ + R 2 0, y) dy, and Y def = 0 x + 0,t,x) 2.5) X t cx x = 0, Y t + cy x = 0. Furthermore, for any smooth function f, we obtain by using 2.5) that [ + S 2 0, y) dy. 2.6) f t + cf x = X t + cx x )f X = 2cX x f X f t cf x = Y t cy x )f Y = 2cY x f Y.
6 6 G. CHEN, P. ZHANG, AND Y. ZHENG Introduce 2.7) p def = + R 2 X x and q def = + S 2 Y x. Then By 2.2), we have t p c x p = 2X x ) [ R t R cn ) x R) X x ) 2 [ t X x c x X x + R 2 ). R tr cn ) xr) { = c 2 c 2 α) R 2 + S 2 ) 23c 2 α) R S } R n + α γ R 2 c 2 + S 2 2R S ) R n + c 2c R R 2 R S). Using n = and c = γ α)n c, so that R n = 0, we further obtain 2.8) R t R cn ) x R) = c c R R 2 S 2 ), which together with 2.5) applied gives t p c x p = c p 2c + R [ R + S 2 ) + S + R 2 ), 2 from which, and ), we infer 2.9) Similarly, p Y = 2c Y x ) p t cp x ) = c c 2 pq R + R 2 + S + S 2 ). t q + c x q = 2 Y x ) [ S t S + cn ) x S) while again thanks to 2.2), we have +Y x ) 2 t Y x + c x Y x ) + S 2 ), S ts cn ) xs) { = c 2 c 2 α) R 2 + S 2 ) 23c 2 α) R S } S n + α γ R 2 c 2 + S 2 2R S ) S n + c 2c S S 2 R S), which along with the fact that S n = 0 leads to 2.0) S t S cn ) x S) = c c S R 2 S 2 ), from which and 2.5), we infer t q + c x q = c q 2c + S [R + S 2 ) S + R 2 ). 2
7 Then applying ) gives rise to 2.) Now we introduce 2.2) Then ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 7 l = l, l 2, l 3 ) def = h def = q X = q t + cq x ) 2cX x = c c 2 pq R + R S ) 2 + S. 2 + R, h def 2 2 = R + R, m = m, m 2, m 3 ) def = 2 + S 2. t l c x l = + R 2 ) t R c x R ) which together with 2.2) and 2.8) imply S + S 2, and 2 + R 2 ) 2 R [ R t R cn ) x R), t l c x l = + R 2 ) [ c 2 γ c 2 R 2 + S 2 ) 3c2 γ R 2c 2 S n + c 2c + R 2 ) 2 [ R R + S 2 ) S + R 2 ). Then thanks to ), we obtain Y l = q [ c 2 8c 3 γ)h + h 2 2h h 2 ) 23c 2 γ) l m n 2.3) + c c 2 l ql m ). Similarly thanks to 2.2), we have t m + c x m = + S 2 ) t S + c x S ) which together with 2.2) and 2.0) ensure that 2 + S 2 ) 2 S [ S t S + cn ) x S), t m + c x m = + S 2 ) [ c 2 γ c 2 R 2 + S 2 ) 3c2 γ R 2c 2 S n c 2c + S 2 ) 2 [ S R + S 2 ) S + R 2 ), from which and ), we infer X m = p [ c 2 8c 3 γ)h + h 2 2h h 2 ) 23c 2 γ) l m n 2.) c c 2 m pl m ).
8 8 G. CHEN, P. ZHANG, AND Y. ZHENG Following the same line, we deduce from 2.2) and 2.8) that t l 2 c x l 2 = + R 2 ) [ c 2 α c 2 R 2 + S 2 ) 3c2 α R 2c 2 S n 2 + c 2c + R 2 ) 2 [ R R2 + S 2 ) S 2 + R 2 ), and t l 3 c x l 3 = + R 2 ) [ c 2 α c 2 R 2 + S 2 ) 3c2 α R 2c 2 S n 3 + c 2c + R 2 ) 2 [ R R3 + S 2 ) S 3 + R 2 ), which together with ) ensure that 2.5) Y l 2 = q [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 + c c 2 l ql 2 m 2 ) and Y l 3 = q [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 3 + c c 2 l ql 3 m 3 ). While we deduce from 2.2) and 2.0) that and t m 2 + c x m 2 = + S 2 ) [ c 2 α c 2 R 2 + S 2 ) 3c2 α R 2c 2 S n 2 c 2c + S 2 ) 2 [ S R2 + S 2 ) S 2 + R 2 ), t m 3 + c x m 3 = + S 2 ) [ c 2 α c 2 R 2 + S 2 ) 3c2 α R 2c 2 S n 3 c 2c + S 2 ) 2 [ S R3 + S 2 ) S 3 + R 2 ), which together with ) imply that 2.6) X m 2 = p [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 c c 2 m pl 2 m 2 ) and X m 3 = p [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 3 c c 2 m pl 3 m 3 ).
9 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 9 On the other hand, it follows from 2.8) and 2.2) that t h c x h = 2 + R 2 ) 2[ R t R cn ) x R) Then we obtain by using ) that = c 2c + R 2 ) 2 R R 2 S 2 ). 2.7) Y h = c c 2 ql h h 2 ). Similar calculations together with 2.0) yield t h 2 + c x h 2 = c 2c + S 2 ) 2 S R 2 S 2 ), which together with ) imply that 2.8) X h 2 = c c 2 pm h 2 h ). Finally we observe from 2.6) and 2.2) that 2.9) Y n = t n c x n) = 2cX x X n = 2c Y x ) tn + c x n) = q 2c m, p 2c l. In summary, we obtain Y l = q 8c 3 [ c 2 γ)h + h 2 2h h 2 ) 23c 2 γ) l m n 2.20) + c c 2 l ql m ), X m = p 8c 3 [ c 2 γ)h + h 2 2h h 2 ) 23c 2 γ) l m n Y l 2 = c c 2 m pl m ), q 8c 3 [ c 2 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 + c c 2 l ql 2 m 2 ), X m 2 = p 8c 3 [ c 2 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 Y l 3 = c c 2 m pl 2 m 2 ), q 8c 3 [ c 2 α)h + h 2 2h h 2 ) 23c 2 α) l m n 3 + c c 2 l ql 3 m 3 ), X m 3 = p 8c 3 [ c 2 α)h + h 2 2h h 2 ) 23c 2 α) l m n 3 c c 2 m pl 3 m 3 ), Y n = q 2c m, or Xn = p 2c l) Y h = c c 2 ql h h 2 ), X h 2 = c c 2 m ph 2 h ), p Y = c c 2 pql m ), q X = c c 2 pql m ).
10 0 G. CHEN, P. ZHANG, AND Y. ZHENG 2.2. Consistency of variables of 2.20). The various variables introduced for 2.20) are consistent, following from the proposition below. Proposition 2.. For smooth enough data, there hold the following conservative quantities: 2.2) l nx, Y ) = m nx, Y ) = 0, nx, Y ) = and lx, Y ) 2 + h 2 X, Y ) = h X, Y ), mx, Y ) 2 + h 2 2X, Y ) = h 2 X, Y ), X, Y, as long as l nx, ϕx)) = m nx, ϕx)) = 0, nx, ϕx)) = and lx, ϕx)) 2 + h 2 X, ϕx)) = h X, ϕx)), mx, ϕx)) 2 + h 2 2X, ϕx)) = h 2 X, ϕx)), X. Here the function ϕ represents the initial curve, see 3.2) from the next section. Proof. We first deduce from 2.20) that [ Y l 2 + h 2 q [ h = c 2 c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m l n + α γ)n c 3 q[ h + h 2 2h h 2 ) 2 l m l + c c 2 ql [ 2 l 2 l m) + 2h h h 2 ) h h 2 ), from which and the fact that c = γ α)n c, we deduce that [ Y l 2 + h 2 q [ h = c 2 c 3 α)h + h 2 2h h 2 ) 2.22) 23c 2 α) l m c l n + 2c 2 ql [ l 2 + h 2 h. Similarly it follows from 2.20) that Y [ l n = Y l n + l Y n = q [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 ) q + 8c 3 h + h 2 2h h 2 ) [ c 2 α) + α γ)n 2 q c 3 l m [ 3c 2 α + α γ)n 2 q + c 2 ql [ l n m n + q 2c l m, which along with the fact that c 2 = α + γ α)n 2 leads to Y [ l n = q [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 ) 2.23) + c c 2 ql [ l n m n.
11 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS On the other hand, observe that Y n = 2c m is consistent with Xn = again thanks to 2.20), one has on the one hand X [ Y n = c 8c 3 pql + m ) m + q 2c X m, and on the other hand Y [ X n = c 8c 3 pql + m ) l + p 2c Y l, q p 2c l. Indeed which along with the l equations and m equations of 2.20) shows that X [ Y n = Y [ X n. So we can also use the equation X n = p 2c l, from which and the m equation of 2.20), we obtain X [ m n = X m n + m X l = p [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 ) p [ + c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m + α γ [ 8c 3 pn2 h + h 2 2h h 2 ) 2 l m + c c 2 pm [ m n l n + p 2c l m, which gives rise to Y [ m n = p [ c 2 8c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m n 2 ) 2.2) c c 2 pm [ l n m n. Next it is easy to observe that 2.25) Y [ n 2 = q m n. 2c Finally, to control the evolution of m 2 + h 2 2 h 2, we obtain by applying 2.20) that [ X m 2 + h 2 p [ 2 h 2 = c 2 c 3 α)h + h 2 2h h 2 ) 23c 2 α) l m m n + α γ c 3 p[ h + h 2 2h h 2 ) 2 l m m n + c 2c 2 pm [ m 2 l m) + h 2 2 )h 2 h ), which simplifies to [ X m 2 + h 2 p [ 2 h 2 = c 2 c 3 α)h + h 2 2h h 2 ) 2.26) 23c 2 α) l m m n + c 2c 3 pm [ m 2 + h 2 2 h 2. Summing up 2.22) to 2.26) gives rise to 2.2). This completes the proof of the proposition.
12 2 G. CHEN, P. ZHANG, AND Y. ZHENG 3. Solutions in the energy coordinates Using 2.6) by letting f = t or x, we obtain the equations 3.) t X = ph 2c, t Y = qh 2 2c, x X = ph 2, x Y = qh 2 2. Only one of the two equations of t X and t Y is needed for recovering t, and the two equations are consistent since t XY = t Y X. The same is true for x. The initial line t = 0 in the x, t) plane is transformed to a parametric curve 3.2) γ : Y = ϕx) in the X, Y ) plane, where Y = ϕx) if and only if there is an x such that X = x 0 [ + R 2 0, y) dy, 3.3) Y = 0 x [ + S 2 0, y) dy. We point out that the curve is non-characteristic. We introduce 3.) E 0 := [ R 2 0, y) + S 2 0, y) dy <. It equals to the number in.25). The two functions X = Xx), Y = Y x) from 3.3) are well-defined and absolutely continuous, provided that.2) is satisfied. Clearly, X is strictly increasing while Y is strictly decreasing. Therefore, the map X ϕx) is continuous and strictly decreasing. From 3.) it follows 3.5) X + ϕx) E 0. As t, x) ranges over the domain [0, ) R, the corresponding variables X, Y ) range over the set 3.6) Ω + := { X, Y ) ; Y ϕx) }. Along the curve γ := { X, Y ) ; Y = ϕx) } R 2 parametrized by x Xx), Y x) ), we can thus assign the boundary data l, m, h, h 2, p, q, n) L defined by their definition evaluated at the initial data.2), i.e., 3.7) where n = n 0 x), p =, q =, l = R0, x) h, m = S0, x) h2, h = h 2 = R0, x) = n x) + cn 0 x))n 0x), + R 2 0, x), and + S 2 0, x). S0, x) = n x) cn 0 x))n 0x). We consider solutions to the boundary value problem 2.20)3.7).3). Theorem 3.. The problem 2.20)3.7).2).3) has a unique global solution defined for all X, Y ) R 2.
13 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 3 Sketch of Proof. In the following, we shall construct the solution on the domain Ω + where Y ϕx). On the complementary set Ω where Y < ϕx), the solution can be constructed similarly. Observing that all equations in 2.20) have a locally Lipschitz continuous right hand side, the construction of a local solution as fixed point of a suitable integral transformation is straightforward. To make sure that this solution is actually defined on the whole domain Ω +, one must establish a priori bounds, showing that the solution remains bounded on bounded sets. By 2.2), we have 3.8) h h ) 0, h 2 h 2 ) 0. Thus h, h 2 are bounded between zero and one, and both l and m are uniformly bounded. By the p and q equations in 2.20), we have 3.9) p Y + q X = 0 which implies that X ϕ Y ) px, Y )dx + Y ϕx) qx, Y )dy = X ϕ Y ) + Y ϕx) where ϕ denotes the inverse of ϕ, following an integration over the characteristic triangle with vertex X, Y ). Thus, by the energy assumption 3.), we find 3.0) X ϕ Y ) px, Y )dx + Y ϕx) qx, Y ) dy 2 X + Y + E 0 ). Integrating the p equation in 2.20) vertically and use the bound on q from 3.0), we find { } Y c px, Y ) = exp ϕx) c 2 qx, Y ) l + m ) dy 3.) } exp {C 0 YϕX) qx, Y ) dy exp{2c 0 X + Y + E 0 )}. Here C 0 represents a finite number. Similarly, we have 3.2) qx, Y ) exp{2c 0 X + Y + E 0 )}. Relying on the local bounds 3.)3.2), the local solution to 2.20)3.7).2).3) can be extended to the entire plane. One may consult paper [3 for details. This completes the sketch of the proof. Let us state a useful consequence of the above construction for future reference. Corollary 3.. If the initial data n 0, n ) are smooth, the solution U := n, p, q, l, m, h, h 2 ) of 2.20)3.7).2).3) is a smooth function of the variables X, Y ). Moreover, assume that a sequence of smooth functions n i 0, ni ) i satisfies n i 0 n 0, n i 0) x n 0 ) x, n i n uniformly on compact subsets of R. Then one has the convergence of the corresponding solutions: n i, p i, q i, l i, m i, h i, h i 2) U uniformly on bounded subsets of the X-Y plane.
14 G. CHEN, P. ZHANG, AND Y. ZHENG. Inverse transformation By expressing the solution nx, Y ) in terms of the original variables t, x), we shall recover a solution of the Cauchy problem.).3). This will provide a proof of Theorem.. We integrate 3.) with data t = 0, x = x on γ to find t = tx, Y ), x = xx, Y ), which exist for all X, Y ) in R 2. We need the inverse functions X = Xt, x), Y = Y t, x). The inverse functions do not exist as a one-to-one correspondence between t, x) in R 2 and X, Y ) in R 2. There may be a nontrivial set of points in the X, Y ) plane that maps to a single point t, x). To investigate it, we find the partial derivatives of the inverse mapping, valid at points where h 0, h 2 0,.) X t = c ph, Y t = c qh 2, X x = ph, Y x = qh 2. Thus 2.5) holds and so does 2.6) for our solution. As a preliminary, we examine the regularity of the solution U = n, p, q, l,...) constructed in the previous section. Since the initial data n 0 ) x, n etc. are only assumed to be in L 2, the functions U may well be discontinuous. More precisely, on bounded subsets of the X-Y plane, the solutions satisfy the following: -: The functions l, l 2,, l 3, h, p are Lipschitz continuous w.r.t. Y, measurable w.r.t. X. -: The functions m, m 2, m 3, h 2, q are Lipschitz continuous w.r.t. X, measurable w.r.t. Y. -: The vector field n is Lipschitz continuous w.r.t. both X and Y. In order to define n as a vector field of the original variables t, x, we should formally invert the map X, Y ) t, x) and write nt, x) = n Xt, x), Y t, x) ). The fact that the above map may not be one-to-one does not cause any real difficulty. Indeed, given t, x ), we can choose an arbitrary point X, Y ) such that tx, Y ) = t, xx, Y ) = x, and define nt, x ) = nx, Y ). To prove that the values of n do not depend on the choice of X, Y ), we proceed as follows. Assume that there are two distinct points such that tx, Y ) = tx 2, Y 2 ) = t, xx, Y ) = xx 2, Y 2 ) = x. We consider two cases: Case : X X 2, Y Y 2. Consider the set Γ x := {X, Y ) ; xx, Y ) x } and call Γ x its boundary. By 3.), x is increasing in X and decreasing in Y. Hence, this boundary can be represented as the graph of a Lipschitz continuous function: X Y = φx + Y ). We now construct the Lipschitz continuous curve γ consisting of -: a horizontal segment joining X, Y ) with a point A = X A, Y A ) on Γ x, with Y A = Y, -: a portion of the boundary Γ x, -: a vertical segment joining X 2, Y 2 ) to a point B = X B, Y B ) on Γ x, with X B = X 2. Observe that the map X, Y ) t, x) is constant along γ. By 3.) this implies h = 0 on the horizontal segment, h 2 = 0 on the vertical segment, and h = h 2 = 0 on the portion of the boundary Γ x. When either h = 0 or h 2 = 0 or both, we have from the conserved quantities 2.22) that l = 0 or m = 0 or both, correspondingly. Upon examining the derivatives of n in 2.20), we have the same pattern of vanishing property. Thus, along the path from A to B, the values of the components of n remain constant, proving our claim. Case 2: X X 2, Y Y 2. In this case, we consider the set { Γ t := X, Y ) ; tx, Y ) t },
15 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 5 and construct a curve γ connecting X, Y ) with X 2, Y 2 ) similarly as in case. Details are entirely similar to Case. We now prove that the function nt, x) = n Xt, x), Y t, x) ) thus obtained are Hölder continuous on bounded sets. Toward this goal, consider any characteristic curve, say t x + t), with dx + /dt = c. By construction, this is parametrized by the function X tx, Y ), xx, Y ) ), for some fixed Y. Using the chain rule and the inverse mapping formulas.), we obtain Thus we have n t + cn x = n X X t + cx x ) + n Y Y t + cy x ) = 2cX x n X. τ 0 nt + cn x 2 dt = Xτ X 0 2cX x n X ) 2 2X t ) dx.2) = X τ X 0 2c ph p l 2c )2 ph 2c dx = X τ X 0 p l 2 2c h dx X τ X 0 p 2c dx C τ, for some constant C τ depending only on τ. Notice we have used l 2 h, which follows from 2.2). Similarly, integrating along any backward characteristics t x t) we obtain τ.3) n t cn x 2 dt Cτ. 0 Since the speed of characteristics is ±c, and c is uniformly positive and bounded, the bounds.2)-.3) imply that the function n = nt, x) is Hölder continuous with exponent /2. In turn, this implies that all characteristic curves are C with Hölder continuous derivative. In addition, from.2)-.3) it follows that R, S at 2.) are square integrable on bounded subsets of the t-x plane. However, we should check the consistency that R, S at 2.) are indeed the same as recovered from 2.2). Let us check only one of them, R = l/h. We find n t + cn x = 2cX x n X = 2c ph p l 2c = l h. Finally, we prove that n satisfies the equations of system.) in distributional sense, according to iii) of Definition.. We note that [ 2 φt n t φ x c 2 n x dxdt.) = φ t [ nt + cn x ) + n t cn x ) cφ x [ nt + cn x ) n t cn x ) dxdt = [ φ t cφ x nt + cn x ) dxdt + [ φ t + cφ x nt cn x ) dxdt By 2.6), this is equal to = [ φ t cφ x R dxdt + [ φt + cφ x S dxdt..5) Using the Jacobian.6) [ 2cYx φ Y R + 2cXx φ X S dxdt. x, t) X, Y ) = pqh h 2 2c
16 6 G. CHEN, P. ZHANG, AND Y. ZHENG derived from 3.), and the inverse.), we see that it is equal to [ 2c RφY + 2c pqh h 2 SφX dxdy qh 2 ph 2c.7) = [ph RφY + qh 2 SφX dxdy = [p lφy + q mφ X dxdy = [ p l)y q m) X φ dxdy. Thanks to 2.), 2.2) and 2.20), we have that the first component of the integrand equals to φ [ pl ) Y qm ) X = φ pq [ c 2 c 3 γ)h + h 2 2h h 2 ) 23c 2 γ) l m n = φ pqh h 2 2c = φ pqh h 2 2c = φ pqh h 2 2c = 2φ pqh h 2 2c [c 2 γ 2c 2 + 2) 3c2 γ l m n h 2 h c 2 h h 2 [c 2 γ 2c 2 R 2 + S 2 ) 3c2 γ R S n c 2 [c 2 γ c 2 n t 2 + c 2 n x 2 ) 3c2 γ c 2 n t 2 c 2 n x 2 ) n. nt 2 + 2c 2 γ) n x 2) n, which implies that the first equation in.) holds in integral form. Similarly, n satisfies the second and third equations of system.) in distributional sense. 5. Upper bound on energy We convert the energy conservation.2) formally to the X, Y ) plane to look for conservation of energy. Recall that the energy conservation law.2) can be written as 2.3) in terms of R and S. By the variables 2.2), we rewrite the equation 2.3) as It yields a closed form 5.) which, using the formula 5.2) can be written as 5.3) h + h 2 2 ) t [ c h h 2 ) x = 0. + ) [ c dx + h h 2 2 ) dt h h 2 dt = t X dx + t Y dy = ph 2c dx + qh 2 2c dy dx = x X dx + x Y dy = ph 2 dx qh 2 2 dy p h ) dx q h 2) dy.
17 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 7 This is the energy form in the X, Y ) plane. The solutions n = nx, Y ) constructed in Section 2 are conservative, in the sense that the integral of the form 5.3) along every Lipschitz continuous, closed curve in the X-Y plane is zero. Y A D Ω B γ τ O X C γ 0 Figure. Energy conservation We use 5.3) to establish that the energy of our solution is bounded, i.e., the energy inequality.26). Fix τ > 0, and r >>. Define the set { } 5.) Ω := X, Y ) ; 0 tx, Y ) τ, X r, Y r. See Figure, where segment AD is where Y = r while segment BC is where X = r. By construction, the map X, Y ) t, x) will act as follows: A τ, a), B τ, b), C 0, c), D 0, d), for some a < b and d < c. Integrating the -form 5.3) along the boundary of Ω we obtain p h ) dx q h 2) dy 5.5) AB = DC CB p h ) dx q h 2) dy DA dy q h 2 ) p h ) dx p h ) DC dx q h 2) dy = [ c d 2 n t 2 0, x) + c 2 n 0, x) ) n x 2 0, x) dx. On the other hand, we use 5.2) to compute b [ n t 2 τ, x) + c 2 n τ, x) ) n x 2 τ, x) dx a 2 5.6) p h ) q h 2 ) = dx dy E 0. AB {h 2 0} AB {h 0} Notice that the last relation in 5.5) is satisfied as an equality, because at time t = 0, along the curve γ 0 the variables h, h 2 never assume the value zero. The proof for the case τ < 0 is similar. Letting r + in 5.), one has a, b +. Therefore 5.5) and 5.6) together imply Et) E 0, proving.26).
18 8 G. CHEN, P. ZHANG, AND Y. ZHENG 6. Regularity of trajectories 6.. Lipschitz continuity. In this part, we first prove the Lipschitz continuity of the map t n, n 2, n 3 )t, ) in the L 2 distance, stated in.23). For any h > 0, we have Thus nt + h, x) nt, x) = h 6.) n i t + h, x) n i t, x) L 2 h 0 0 n t t + τh, x) dτ. n it t + τh, ) L 2 dτ h 2E 0, i = Continuity of derivatives. We prove the continuity of functions t n t, n 2t, n 3t )t, ) and t n x, n x, n x )t, ), as functions with values in L p, p < 2. To keep tradition, we use the exponent p here at the expense of repeating one of our primary variables.) This will complete the proof of Theorem.. We first consider the case where the initial data n 0 ) x and n are smooth with compact support. In this case, the solution n = nx, Y ) remains smooth on the entire X-Y plane. Fix a time τ. We claim that d 6.2) nt, ) dt = n t τ, ) t=τ where 6.3) n t τ, x) := n X X t + n Y Y t = p l 2c c + q m ph 2c c qh 2 = l 2h + m 2h 2. Notice that 6.3) defines the values of n t τ, ) at almost every point x R. By the inequality.26), we obtain 6.) n t τ, x) 2 dx 2 Eτ) 2 E 0. To prove 6.2), we consider the set 6.5) Γ τ := {X, Y ) tx, Y ) τ}, R and let γ τ be its boundary. Let ε > 0 be given. There exist finitely many disjoint intervals [a i, b i R, i =,..., N, with the following property. Call A i, B i the points on γ τ such that xa i ) = a i, xb i ) = b i. Then one has 6.6) min { h P ), h 2 P ) } < 2ε at every point P on γ τ contained in one of the arcs A i B i, while 6.7) h P ) > ε, h 2 P ) > ε, for every point P along γ τ, not contained in any of the arcs A i B i. Call J := i N [a i, b i, J = R \J, and notice that, as a function of the original variables, n = nt, x) is smooth in a neighborhood of the set {τ} J. Using Minkowski s inequality and the differentiability of n on J, we can write, for i = 3, lim h 0 h R n i τ + h, x) n i τ, x) h n it τ, x) p ) /p dx 6.8) lim h 0 h J n i τ + h, x) n i τ, x) p ) /p dx + J nit τ, x) p dx ) /p.
19 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 9 We now provide an estimate on the measure of the bad set J: meas J) = J dx = ph i A i B i 2 dx qh 2 2 dy 6.9) 2ε p h ) 2ε i A i B i 2 dx q h 2) 2 dy ε p h ) 2ε γ τ dx q h 2) dy ε 2ε E 0. Notice that dt = 0 on γ τ, so the two parts of the integral are actually equal. Now choose q = 2/2 p) so that p 2 + q =. Using Hölder s inequality with conjugate exponents 2/p and q, and recalling 6.), we obtain for any i = 3 J n i τ + h, x) n i τ, x) p dx ) meas J) /q J n i τ + h, x) n i τ, x) 2 p/2 dx Therefore, 6.0) J meas J) /q n i τ + h, ) n i τ, ) ) 2 p/2 L 2 meas J) /q h 2[ ) p/2 2E 0. lim sup h 0 h ε [ J n i τ + h, x) n i τ, x) p dx 2ε E 0 /pq [2E /2. 0 In a similar way we estimate n it τ, x) p dx [ meas J) /q 6.) J J ) /p n it τ, x) dx) 2 p/2, n it τ, x) p dx) /p meas J) /pq [2E 0 p/2. Since ε > 0 is arbitrary, from 6.8), 6.0) and 6.) we conclude 6.2) lim n i τ + h, x) n i τ, x) h n it τ, x) p /p dx) = 0. h 0 h R The proof of continuity of the map t n it is similar. Fix ε > 0. Consider the intervals [a i, b i as before. Since n is smooth on a neighborhood of {τ} J, it suffices to estimate lim sup nit h 0 τ + h, x) n it τ, x) p dx lim sup h 0 J n it τ + h, x) n it τ, x) p dx [ /q lim sup h 0 meas J) J n it τ + h, x) n it τ, x) 2 dx [ lim sup ε h 0 2ε E /q nit 0 τ + h, ) L 2 + nit τ, ) ) p L 2 [ ε 2ε E 0 /q [ E 0 p. ) p/2
20 20 G. CHEN, P. ZHANG, AND Y. ZHENG Since ε > 0 is arbitrary, this proves continuity. To extend the result to general initial data, such that n 0 ) x, n = n t t=0 L 2, we use Corollary 3. and consider a sequence of smooth initial data, with n ν 0 ) x, n ν C c, with n ν 0 n 0 uniformly, n ν 0 ) x n 0 ) x almost everywhere and in L 2, n ν n almost everywhere and in L 2. The continuity of the function t n x t, ) as maps with values in L p, p < 2, is proved in an entirely similar way. 7. Energy conservation This part is devoted to the proof of Theorem.3, stating that, in some sense, the total energy of the solution remains constant in time. A key tool in our analysis is the wave interaction potential, defined in the smooth case by Λt) := 6 x>y R 2 t, x) S 2 t, y) dxdy. To define it in the general case, for any fixed time τ, we let µ τ = µ τ + µ + τ be the positive measure on the real line defined as follows. In the smooth case, 7.) µ τ To define µ ± τ a, b) ) = b a R 2 τ, x) dx, µ + τ a, b) ) = in the general case, let γ τ be the boundary of the set 7.2) Γ τ := {X, Y ) tx, Y ) τ}, b a S 2 τ, x) dx. and let γ τ be its boundary. Given any open interval a, b), let A = X A, Y A ) and B = X B, Y B ) be the points on γ τ such that Then xa) = a, X P Y P X A Y A for every point P γ τ with xp ) a, xb) = b, X P Y P X B Y B for every point P γ τ with xp ) b. 7.3) µ τ a, b) ) = µ τ a, b) ) + µ + τ a, b) ), where 7.) µ ) τ a, b) := AB p h ) dx µ + τ a, b) ) := AB q h 2 ) It is clear that µ τ, µ + τ are bounded, nonnegative measures, and µ τ R) = E 0, for all τ. The wave interaction potential is defined as 7.5) Λt) := µ t µ + t ){ x, y) ; x > y }. Lemma 7. Bounded variation). The map t Λt) has locally bounded variation; i.e., there exists a one-sided Lipschitz constant L 0 such that Λt) Λs) L 0 t s), t > s > 0. Before we prove the lemma, let us first give a formal argument, valid when the solution nt, x) remains smooth. Thanks to 2.8) and 2.0), we obtain 7.6) t R 2 x c R 2 ) =A, t S 2 + x c S 2 ) = A, dy.
21 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 2 where 7.7) A = c R 2 S S 2c 2 ) R. Then 7.8) d dt [6Λt) 2C L 2c R 2 S 2 dx + S 2 + R 2) dx A dx R 2 S 2 c dx + E 0 2c R 2 S R S 2 dx. L For each ε > 0 we have R ε /2 + ε /2 R 2. Choosing ε > 0 such that c C L E 0 2 ε, 2c we thus obtain d dt [6Λt) C L L R 2 S 2 dx + 6 E2 0 c ε 2c L 6 E2 0 c ε 2c Hence, the map t Λt) has bounded variation on any bounded interval. It can be discontinuous, with downward jumps. Proof. We reproduce the formal argument in terms of the variables X, Y. In particular, we reproduce 7.8) in integral form in the X, Y ) plane. By 2.2), for any ε > 0, there exists a constant κ ε such that Hence m ε h 2 ) + κ ε h 2, l ε h ) + κ ε h. 7.9) h )m h 2 )l ε h ) h 2 ) + κ ε [ h )h 2 + h 2 )h. Fix 0 s < t. Consider the sets Γ s, Γ t as in 7.2) and define Γ st := Γ t \Γ s. Recall that We can write 7.0) dx dt = pqh h 2 2c dx dy, R 2 = h h, S 2 = h 2 h 2. t R 2 + S 2 s dxdt = t s)e 0 = Γ st ) h h + h 2 h 2 pqh h 2 2c dxdy. The first identity holds only for smooth solutions, but the second one is always valid. Recalling 5.) and 7.), and then using 7.9)-7.0), we obtain h Λt) Λs) p h 2 q dxdy Γ st c + E 0 Γst 6c 2 pq [ h )m h 2 )l dxdy h ) h 2 ) pq dxdy 6 Γ st c + E 0 Γst 6c 2 pq {κ ε [ h )h 2 + h 2 )h +ε h ) h 2 )} dxdy κt s), L.
22 22 G. CHEN, P. ZHANG, AND Y. ZHENG for a suitable constant κ. This proves the lemma. To prove Theorem.3, consider the three sets { Ω := X, Y ) ; h X, Y ) = 0, h 2 X, Y ) 0, Ω 2 := Ω 3 := { X, Y ) ; h 2 X, Y ) = 0, h X, Y ) 0, { X, Y ) ; h X, Y ) = 0, h 2 X, Y ) = 0, c 2 n X, Y )) γ ) n X, Y ) 0}, c 2 n X, Y )) γ ) n X, Y ) 0}, c 2 n X, Y )) γ ) n X, Y ) 0}. Here c 2 γ ) n 0 is equivalent to n ± or 0, since we assume that α γ. From the equations 2.20), it follows that 7.) meas Ω ) = meas Ω 2 ) = 0. Indeed, Y l 0 on Ω since h = 0 implies l = 0 by 2.2). Similarly X m 0 on Ω 2 since h 2 = 0 implies m = 0. And, for any i = 3, l i 0 implies h 0, m i 0 implies h 2 0, by 2.2). Let Ω 3 be the set of Lebesgue points of Ω 3. We now show that 7.2) meas {tx, Y ) ; X, Y ) Ω 3 } ) = 0. To prove 7.2), fix any P = X, Y ) Ω 3 and let τ = tp ). We claim that 7.3) lim sup h,k 0+ Λτ h) Λτ + k) h + k = + Q σ P * σ + t = t t = t Figure 2. Lebesgue point By assumption, for any ε > 0 arbitrarily small we can find δ > 0 with the following property. For any square Q centered at P with side of length l < δ, there exists a vertical segment σ and a horizontal segment σ, as in Figure 2, such that 7.) meas Ω 3 σ ) ε)l, meas Ω 3 σ ) ε)l, Call { t + := max tx, Y ) ; X, Y ) σ σ }, { t := min tx, Y ) ; X, Y ) σ σ }.
23 ENERGY CONSERVATIVE SOLUTIONS TO LIQUID CRYSTALS 23 Since h = h 2 = 0 at nearly all points close to P, we can assume that the endpoints of the two segments σ, σ are all in Ω 3. By integrating the equation for l from 2.20), we obtain q [ c 2 σ 8c 3 γ)h + h 2 2h h 2 ) 23c 2 γ) l m n 7.5) + c c 2 l ql m )dy = 0. Notice that h, l are Lipschitz in Y and h = 0 implies l = 0, and they are zero on σ on a set with measure greater than ε)l. So we obtain 7.6) h f + l f 2 + l 2 f 3 + l 3 f ) dy = O)εl) 2 σ for any bounded functions f f. Thus we obtain from 7.5)7.6) that c 2 γ ) n 7.7) 8c 3 qh 2 dy = O)εl) 2. By 5.2), we have σ σ t Y dy = σ qh 2 2c dy. Assume without loss of generality that c 2 γ ) n > C 3 > 0, at the point P. By 7.7), we obtain t Y dy = O)εl) 2. σ Similarly we can estimate the growth of t in the X-direction. Combining them, we obtain 7.8) t + t O)εl) 2. On the other hand, 7.9) Λt ) Λt + ) C ε) 2 l 2 C 2 t + t ) for some constant C > 0, C 2 > 0. Since ε > 0 is arbitrary, this implies 7.3). Recalling that the map t Λ has bounded variation, from 7.3) it follows 7.2). We now observe that the singular part of µ τ is nontrivial only if the set { P γτ ; h P ) = 0 or h 2 P ) = 0 } has positive -dimensional measure. By the previous analysis, restricted to the region where c 2 γ ) n 0, i.e. n ± or 0, this can happen only for a set of times having zero measure. Acknowledgments. Part of this work was done when Zheng was visiting Academy of Mathematics and System Sciences, he would like to thank the financial support from Center of Interdisciplinary Sciences from AMSS. P. Zhang is partially supported by NSF of China under Grant 020 and , the one hundred talents plan from Chinese Academy of Sciences under Grant GJHZ and innovation grant from National Center for Mathematics and Interdisciplinary Sciences. Additionally, Yuxi Zheng is partially supported by NSF DMS
24 2 G. CHEN, P. ZHANG, AND Y. ZHENG References [ Giuseppe Alì and John Hunter, Orientation waves in a director field with rotational inertia, Kinet. Relat. Models, ), -37. [2 H. Berestycki, J. M. Coron and I. Ekeland eds.), Variational Methods, Progress in Nonlinear Differential Equations and Their Applications, Vol., Birkhäuser, Boston 990). [3 A. Bressan and Yuxi Zheng, Conservative solutions to a nonlinear variational wave equation, Comm. Math. Phys., ), [ D. Christodoulou and A. Tahvildar-Zadeh, On the regularity of spherically symmetric wave maps, Comm. Pure Appl. Math., 6993), [5 J. Coron, J. Ghidaglia, and F. Hélein eds.), Nematics, Kluwer Academic Publishers, 99. [6 J. L. Ericksen and D. Kinderlehrer eds.), Theory and Application of Liquid Crystals, IMA Volumes in Mathematics and its Applications, Vol. 5, Springer-Verlag, New York 987). [7 James Glimm, Solutions in the large for nonlinear hyperbolic systems of equations, Comm. Pure Appl. Math., 8965), [8 R. Hardt, D. Kinderlehrer, and Fanghua Lin, Existence and partial regularity of static liquid crystal configurations. Comm. Math. Phys., 05986), pp [9 D. Kinderlehrer, Recent developments in liquid crystal theory, in Frontiers in pure and applied mathematics : a collection of papers dedicated to Jacques-Louis Lions on the occasion of his sixtieth birthday, ed. R. Dautray, Elsevier, New York, pp ). [0 R. A. Saxton, Dynamic instability of the liquid crystal director, in Contemporary Mathematics Vol. 00: Current Progress in Hyperbolic Systems, pp , ed. W. B. Lindquist, AMS, Providence, 989. [ J. Shatah, Weak solutions and development of singularities in the SU2) σ-model, Comm. Pure Appl. Math., 988), pp [2 J. Shatah and A. Tahvildar-Zadeh, Regularity of harmonic maps from Minkowski space into rotationally symmetric manifolds, Comm. Pure Appl. Math., 5992), pp [3 J. Sterbenz and D. Tataru, Energy dispersed large data wave maps in 2 + dimensions, Comm. Math. Phys., ), pp [ J. Sterbenz and D. Tataru, Regularity of wave-maps in dimension 2 +, Comm. Math. Phys., ), pp [5 T. Tao, Global regularity of wave maps. I. Small critical Sobolev norm in high dimension, Internat. Math. Res. Notices, 200), no. 6, pp [6 T. Tao, Global regularity of wave maps. II. Small energy in two dimensions, Comm. Math. Phys., 22200), pp [7 E. Virga, Variational Theories for Liquid Crystals, Chapman & Hall, New York 99). [8 Ping Zhang and Yuxi Zheng, Weak solutions to a nonlinear variational wave equation, Arch. Ration. Mech. Anal., ), [9 Ping Zhang and Yuxi Zheng, Weak solutions to a nonlinear variational wave equation with general data, Ann. I. H. Poincaré, ), [20 Ping Zhang and Yuxi Zheng, Conservative solutions to a system of variational wave equations of nematic liquid crystals, Arch. Ration. Mech. Anal., ), [2 Ping Zhang and Yuxi Zheng, Energy Conservative Solutions to a One-Dimensional Full Variational Wave System, Comm. Pure Appl. Math., 202) in press. G. Chen) Department of Mathematics, The Pennsylvania State University, University Park, PA 6802, USA address: chen@math.psu.edu P. Zhang) Academy of Mathematics & Systems Science, and Hua Loo-Keng Key Laboratory of Mathematics, Chinese Academy of Sciences, Beijing 0090, CHINA. address: zp@amss.ac.cn Y. Zheng) Department of Mathematical Sciences, Yeshiva University, 295 Amsterdam Ave, New York, NY 0033, USA address: yzheng@yu.edu
Conservative Solutions to a Nonlinear Variational Wave Equation
Conservative Solutions to a Nonlinear Variational Wave Equation Alberto Bressan and Yuxi Zheng Department of Mathematics, The Pennsylvania State University E-mail: bressan@math.psu.edu; yzheng@math.psu.edu
More informationStructurally Stable Singularities for a Nonlinear Wave Equation
Structurally Stable Singularities for a Nonlinear Wave Equation Alberto Bressan, Tao Huang, and Fang Yu Department of Mathematics, Penn State University University Park, Pa. 1682, U.S.A. e-mails: bressan@math.psu.edu,
More informationOn Asymptotic Variational Wave Equations
On Asymptotic Variational Wave Equations Alberto Bressan 1, Ping Zhang 2, and Yuxi Zheng 1 1 Department of Mathematics, Penn State University, PA 1682. E-mail: bressan@math.psu.edu; yzheng@math.psu.edu
More informationGLOBAL SOLUTIONS TO A ONE-DIMENSIONAL NONLINEAR WAVE EQUATION DERIVABLE FROM A VARIATIONAL PRINCIPLE
Electronic Journal of Differential Equations, Vol. 207 207, No. 294, pp. 20. ISSN: 072-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu GLOBAL SOLUTIONS TO A ONE-DIMENSIONAL NONLINEAR
More informationPiecewise Smooth Solutions to the Burgers-Hilbert Equation
Piecewise Smooth Solutions to the Burgers-Hilbert Equation Alberto Bressan and Tianyou Zhang Department of Mathematics, Penn State University, University Park, Pa 68, USA e-mails: bressan@mathpsuedu, zhang
More informationEXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS WITH UNBOUNDED POTENTIAL. 1. Introduction In this article, we consider the Kirchhoff type problem
Electronic Journal of Differential Equations, Vol. 207 (207), No. 84, pp. 2. ISSN: 072-669. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu EXISTENCE OF SOLUTIONS FOR KIRCHHOFF TYPE EQUATIONS
More informationGlobal conservative solutions of the Camassa-Holm equation
Global conservative solutions of the Camassa-Holm equation Alberto Bressan Deptartment of Mathematics, Pennsylvania State University, University Park 168, U.S.A. e-mail: bressan@math.psu.edu and Adrian
More informationOn the uniqueness of heat flow of harmonic maps and hydrodynamic flow of nematic liquid crystals
On the uniqueness of heat flow of harmonic maps and hydrodynamic flow of nematic liquid crystals Fanghua Lin Changyou Wang Dedicated to Professor Roger Temam on the occasion of his 7th birthday Abstract
More informationSingularity formation for compressible Euler equations
Singularity formation for compressible Euler equations Geng Chen Ronghua Pan Shengguo Zhu Abstract In this paper, for the p-system and full compressible Euler equations in one space dimension, we provide
More informationExistence of minimizers for the pure displacement problem in nonlinear elasticity
Existence of minimizers for the pure displacement problem in nonlinear elasticity Cristinel Mardare Université Pierre et Marie Curie - Paris 6, Laboratoire Jacques-Louis Lions, Paris, F-75005 France Abstract
More informationSobolev Spaces. Chapter 10
Chapter 1 Sobolev Spaces We now define spaces H 1,p (R n ), known as Sobolev spaces. For u to belong to H 1,p (R n ), we require that u L p (R n ) and that u have weak derivatives of first order in L p
More informationA Ginzburg-Landau Type Problem for Nematics with Highly Anisotropic Elastic Term
A Ginzburg-Landau Type Problem for Nematics with Highly Anisotropic Elastic Term Peter Sternberg In collaboration with Dmitry Golovaty (Akron) and Raghav Venkatraman (Indiana) Department of Mathematics
More informationBIHARMONIC WAVE MAPS INTO SPHERES
BIHARMONIC WAVE MAPS INTO SPHERES SEBASTIAN HERR, TOBIAS LAMM, AND ROLAND SCHNAUBELT Abstract. A global weak solution of the biharmonic wave map equation in the energy space for spherical targets is constructed.
More informationHOMEOMORPHISMS OF BOUNDED VARIATION
HOMEOMORPHISMS OF BOUNDED VARIATION STANISLAV HENCL, PEKKA KOSKELA AND JANI ONNINEN Abstract. We show that the inverse of a planar homeomorphism of bounded variation is also of bounded variation. In higher
More informationS chauder Theory. x 2. = log( x 1 + x 2 ) + 1 ( x 1 + x 2 ) 2. ( 5) x 1 + x 2 x 1 + x 2. 2 = 2 x 1. x 1 x 2. 1 x 1.
Sep. 1 9 Intuitively, the solution u to the Poisson equation S chauder Theory u = f 1 should have better regularity than the right hand side f. In particular one expects u to be twice more differentiable
More informationOn a Lyapunov Functional Relating Shortening Curves and Viscous Conservation Laws
On a Lyapunov Functional Relating Shortening Curves and Viscous Conservation Laws Stefano Bianchini and Alberto Bressan S.I.S.S.A., Via Beirut 4, Trieste 34014 Italy. E-mail addresses: bianchin@mis.mpg.de,
More informationin Bounded Domains Ariane Trescases CMLA, ENS Cachan
CMLA, ENS Cachan Joint work with Yan GUO, Chanwoo KIM and Daniela TONON International Conference on Nonlinear Analysis: Boundary Phenomena for Evolutionnary PDE Academia Sinica December 21, 214 Outline
More informationhal , version 1-22 Nov 2009
Author manuscript, published in "Kinet. Relat. Models 1, 3 8) 355-368" PROPAGATION OF GEVREY REGULARITY FOR SOLUTIONS OF LANDAU EQUATIONS HUA CHEN, WEI-XI LI AND CHAO-JIANG XU Abstract. By using the energy-type
More information2 A Model, Harmonic Map, Problem
ELLIPTIC SYSTEMS JOHN E. HUTCHINSON Department of Mathematics School of Mathematical Sciences, A.N.U. 1 Introduction Elliptic equations model the behaviour of scalar quantities u, such as temperature or
More informationExtremal Solutions of Differential Inclusions via Baire Category: a Dual Approach
Extremal Solutions of Differential Inclusions via Baire Category: a Dual Approach Alberto Bressan Department of Mathematics, Penn State University University Park, Pa 1682, USA e-mail: bressan@mathpsuedu
More informationOn uniqueness of weak solutions to transport equation with non-smooth velocity field
On uniqueness of weak solutions to transport equation with non-smooth velocity field Paolo Bonicatto Abstract Given a bounded, autonomous vector field b: R d R d, we study the uniqueness of bounded solutions
More informationTADAHIRO OH 0, 3 8 (T R), (1.5) The result in [2] is in fact stated for time-periodic functions: 0, 1 3 (T 2 ). (1.4)
PERIODIC L 4 -STRICHARTZ ESTIMATE FOR KDV TADAHIRO OH 1. Introduction In [], Bourgain proved global well-posedness of the periodic KdV in L T): u t + u xxx + uu x 0, x, t) T R. 1.1) The key ingredient
More informationOn Smoothness of Suitable Weak Solutions to the Navier-Stokes Equations
On Smoothness of Suitable Weak Solutions to the Navier-Stokes Equations G. Seregin, V. Šverák Dedicated to Vsevolod Alexeevich Solonnikov Abstract We prove two sufficient conditions for local regularity
More informationTHE WAVE EQUATION. d = 1: D Alembert s formula We begin with the initial value problem in 1 space dimension { u = utt u xx = 0, in (0, ) R, (2)
THE WAVE EQUATION () The free wave equation takes the form u := ( t x )u = 0, u : R t R d x R In the literature, the operator := t x is called the D Alembertian on R +d. Later we shall also consider the
More informationRegularity for Poisson Equation
Regularity for Poisson Equation OcMountain Daylight Time. 4, 20 Intuitively, the solution u to the Poisson equation u= f () should have better regularity than the right hand side f. In particular one expects
More informationSYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 21, 2003, 211 226 SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS Massimo Grosi Filomena Pacella S.
More informationPreliminary Exam 2018 Solutions to Morning Exam
Preliminary Exam 28 Solutions to Morning Exam Part I. Solve four of the following five problems. Problem. Consider the series n 2 (n log n) and n 2 (n(log n)2 ). Show that one converges and one diverges
More informationON LIQUID CRYSTAL FLOWS WITH FREE-SLIP BOUNDARY CONDITIONS. Chun Liu and Jie Shen
DISCRETE AND CONTINUOUS Website: http://aimsciences.org DYNAMICAL SYSTEMS Volume 7, Number2, April2001 pp. 307 318 ON LIQUID CRYSTAL FLOWS WITH FREE-SLIP BOUNDARY CONDITIONS Chun Liu and Jie Shen Department
More informationGeneric Singularities of Solutions to some Nonlinear Wave Equations
Generic Singularities of Solutions to some Nonlinear Wave Equations Alberto Bressan Deartment of Mathematics, Penn State University (Oberwolfach, June 2016) Alberto Bressan (Penn State) generic singularities
More informationLaplace s Equation. Chapter Mean Value Formulas
Chapter 1 Laplace s Equation Let be an open set in R n. A function u C 2 () is called harmonic in if it satisfies Laplace s equation n (1.1) u := D ii u = 0 in. i=1 A function u C 2 () is called subharmonic
More informationNon-radial solutions to a bi-harmonic equation with negative exponent
Non-radial solutions to a bi-harmonic equation with negative exponent Ali Hyder Department of Mathematics, University of British Columbia, Vancouver BC V6TZ2, Canada ali.hyder@math.ubc.ca Juncheng Wei
More informationAuthor(s) Huang, Feimin; Matsumura, Akitaka; Citation Osaka Journal of Mathematics. 41(1)
Title On the stability of contact Navier-Stokes equations with discont free b Authors Huang, Feimin; Matsumura, Akitaka; Citation Osaka Journal of Mathematics. 4 Issue 4-3 Date Text Version publisher URL
More informationGRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS
LE MATEMATICHE Vol. LI (1996) Fasc. II, pp. 335347 GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS CARLO SBORDONE Dedicated to Professor Francesco Guglielmino on his 7th birthday W
More informationGENERALIZED FRONTS FOR ONE-DIMENSIONAL REACTION-DIFFUSION EQUATIONS
GENERALIZED FRONTS FOR ONE-DIMENSIONAL REACTION-DIFFUSION EQUATIONS ANTOINE MELLET, JEAN-MICHEL ROQUEJOFFRE, AND YANNICK SIRE Abstract. For a class of one-dimensional reaction-diffusion equations, we establish
More informationPARTIAL REGULARITY OF BRENIER SOLUTIONS OF THE MONGE-AMPÈRE EQUATION
PARTIAL REGULARITY OF BRENIER SOLUTIONS OF THE MONGE-AMPÈRE EQUATION ALESSIO FIGALLI AND YOUNG-HEON KIM Abstract. Given Ω, Λ R n two bounded open sets, and f and g two probability densities concentrated
More informationPDE Constrained Optimization selected Proofs
PDE Constrained Optimization selected Proofs Jeff Snider jeff@snider.com George Mason University Department of Mathematical Sciences April, 214 Outline 1 Prelim 2 Thms 3.9 3.11 3 Thm 3.12 4 Thm 3.13 5
More informationThe Minimum Speed for a Blocking Problem on the Half Plane
The Minimum Speed for a Blocking Problem on the Half Plane Alberto Bressan and Tao Wang Department of Mathematics, Penn State University University Park, Pa 16802, USA e-mails: bressan@mathpsuedu, wang
More informationMATH 819 FALL We considered solutions of this equation on the domain Ū, where
MATH 89 FALL. The D linear wave equation weak solutions We have considered the initial value problem for the wave equation in one space dimension: (a) (b) (c) u tt u xx = f(x, t) u(x, ) = g(x), u t (x,
More informationSobolev spaces. May 18
Sobolev spaces May 18 2015 1 Weak derivatives The purpose of these notes is to give a very basic introduction to Sobolev spaces. More extensive treatments can e.g. be found in the classical references
More informationABSOLUTE CONTINUITY OF FOLIATIONS
ABSOLUTE CONTINUITY OF FOLIATIONS C. PUGH, M. VIANA, A. WILKINSON 1. Introduction In what follows, U is an open neighborhood in a compact Riemannian manifold M, and F is a local foliation of U. By this
More informationA Product Property of Sobolev Spaces with Application to Elliptic Estimates
Rend. Sem. Mat. Univ. Padova Manoscritto in corso di stampa pervenuto il 23 luglio 2012 accettato l 1 ottobre 2012 A Product Property of Sobolev Spaces with Application to Elliptic Estimates by Henry C.
More informationSobolev regularity for the Monge-Ampère equation, with application to the semigeostrophic equations
Sobolev regularity for the Monge-Ampère equation, with application to the semigeostrophic equations Alessio Figalli Abstract In this note we review some recent results on the Sobolev regularity of solutions
More informationOn the Front-Tracking Algorithm
JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 7, 395404 998 ARTICLE NO. AY97575 On the Front-Tracking Algorithm Paolo Baiti S.I.S.S.A., Via Beirut 4, Trieste 3404, Italy and Helge Kristian Jenssen
More informationAsymptotic behavior of infinity harmonic functions near an isolated singularity
Asymptotic behavior of infinity harmonic functions near an isolated singularity Ovidiu Savin, Changyou Wang, Yifeng Yu Abstract In this paper, we prove if n 2 x 0 is an isolated singularity of a nonegative
More informationLiquid crystal flows in two dimensions
Liquid crystal flows in two dimensions Fanghua Lin Junyu Lin Changyou Wang Abstract The paper is concerned with a simplified hydrodynamic equation, proposed by Ericksen and Leslie, modeling the flow of
More informationREGULARITY AND EXISTENCE OF GLOBAL SOLUTIONS TO THE ERICKSEN-LESLIE SYSTEM IN R 2
REGULARITY AND EXISTENCE OF GLOBAL SOLUTIONS TO THE ERICKSEN-LESLIE SYSTEM IN R JINRUI HUANG, FANGHUA LIN, AND CHANGYOU WANG Abstract. In this paper, we first establish the regularity theorem for suitable
More informationIMA Preprint Series # 2260
LONG-TIME BEHAVIOR OF HYDRODYNAMIC SYSTEMS MODELING THE NEMATIC LIUID CRYSTALS By Hao Wu Xiang Xu and Chun Liu IMA Preprint Series # 2260 ( June 2009 ) INSTITUTE FOR MATHEMATICS AND ITS APPLICATIONS UNIVERSITY
More informationAn introduction to Mathematical Theory of Control
An introduction to Mathematical Theory of Control Vasile Staicu University of Aveiro UNICA, May 2018 Vasile Staicu (University of Aveiro) An introduction to Mathematical Theory of Control UNICA, May 2018
More informationb i (µ, x, s) ei ϕ(x) µ s (dx) ds (2) i=1
NONLINEAR EVOLTION EQATIONS FOR MEASRES ON INFINITE DIMENSIONAL SPACES V.I. Bogachev 1, G. Da Prato 2, M. Röckner 3, S.V. Shaposhnikov 1 The goal of this work is to prove the existence of a solution to
More informationALEKSANDROV-TYPE ESTIMATES FOR A PARABOLIC MONGE-AMPÈRE EQUATION
Electronic Journal of Differential Equations, Vol. 2005(2005), No. 11, pp. 1 8. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu (login: ftp) ALEKSANDROV-TYPE
More informationDETERMINATION OF THE BLOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION
DETERMINATION OF THE LOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION y FRANK MERLE and HATEM ZAAG Abstract. In this paper, we find the optimal blow-up rate for the semilinear wave equation with a power nonlinearity.
More informationNonlinear Diffusion in Irregular Domains
Nonlinear Diffusion in Irregular Domains Ugur G. Abdulla Max-Planck Institute for Mathematics in the Sciences, Leipzig 0403, Germany We investigate the Dirichlet problem for the parablic equation u t =
More informationA Class of Shock Wave Solutions of the Periodic Degasperis-Procesi Equation
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.9(2010) No.3,pp.367-373 A Class of Shock Wave Solutions of the Periodic Degasperis-Procesi Equation Caixia Shen
More informationWELL-POSEDNESS OF WEAK SOLUTIONS TO ELECTRORHEOLOGICAL FLUID EQUATIONS WITH DEGENERACY ON THE BOUNDARY
Electronic Journal of Differential Equations, Vol. 2017 (2017), No. 13, pp. 1 15. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu WELL-POSEDNESS OF WEAK SOLUTIONS TO ELECTRORHEOLOGICAL
More informationLipschitz Metrics for a Class of Nonlinear Wave Equations
Lipschitz Metrics for a Class of Nonlinear Wave Equations Alberto Bressan and Geng Chen * Department of Mathematics, Penn State University, University Park, Pa 1680, USA ** School of Mathematics Georgia
More informationNonlinear Analysis. A regularity criterion for the 3D magneto-micropolar fluid equations in Triebel Lizorkin spaces
Nonlinear Analysis 74 (11) 5 Contents lists available at ScienceDirect Nonlinear Analysis journal homepage: www.elsevier.com/locate/na A regularity criterion for the 3D magneto-micropolar fluid equations
More informationEquivariant self-similar wave maps from Minkowski spacetime into 3-sphere
Equivariant self-similar wave maps from Minkowski spacetime into 3-sphere arxiv:math-ph/99126v1 17 Oct 1999 Piotr Bizoń Institute of Physics, Jagellonian University, Kraków, Poland March 26, 28 Abstract
More informationRiemann integral and volume are generalized to unbounded functions and sets. is an admissible set, and its volume is a Riemann integral, 1l E,
Tel Aviv University, 26 Analysis-III 9 9 Improper integral 9a Introduction....................... 9 9b Positive integrands................... 9c Special functions gamma and beta......... 4 9d Change of
More informationSome asymptotic properties of solutions for Burgers equation in L p (R)
ARMA manuscript No. (will be inserted by the editor) Some asymptotic properties of solutions for Burgers equation in L p (R) PAULO R. ZINGANO Abstract We discuss time asymptotic properties of solutions
More informationThe Lusin Theorem and Horizontal Graphs in the Heisenberg Group
Analysis and Geometry in Metric Spaces Research Article DOI: 10.2478/agms-2013-0008 AGMS 2013 295-301 The Lusin Theorem and Horizontal Graphs in the Heisenberg Group Abstract In this paper we prove that
More informationL p Spaces and Convexity
L p Spaces and Convexity These notes largely follow the treatments in Royden, Real Analysis, and Rudin, Real & Complex Analysis. 1. Convex functions Let I R be an interval. For I open, we say a function
More informationEuler Equations: local existence
Euler Equations: local existence Mat 529, Lesson 2. 1 Active scalars formulation We start with a lemma. Lemma 1. Assume that w is a magnetization variable, i.e. t w + u w + ( u) w = 0. If u = Pw then u
More informationPartial differential equation for temperature u(x, t) in a heat conducting insulated rod along the x-axis is given by the Heat equation:
Chapter 7 Heat Equation Partial differential equation for temperature u(x, t) in a heat conducting insulated rod along the x-axis is given by the Heat equation: u t = ku x x, x, t > (7.1) Here k is a constant
More informationThe 2D Magnetohydrodynamic Equations with Partial Dissipation. Oklahoma State University
The 2D Magnetohydrodynamic Equations with Partial Dissipation Jiahong Wu Oklahoma State University IPAM Workshop Mathematical Analysis of Turbulence IPAM, UCLA, September 29-October 3, 2014 1 / 112 Outline
More informationLecture Notes on PDEs
Lecture Notes on PDEs Alberto Bressan February 26, 2012 1 Elliptic equations Let IR n be a bounded open set Given measurable functions a ij, b i, c : IR, consider the linear, second order differential
More informationNECESSARY CONDITIONS FOR WEIGHTED POINTWISE HARDY INEQUALITIES
NECESSARY CONDITIONS FOR WEIGHTED POINTWISE HARDY INEQUALITIES JUHA LEHRBÄCK Abstract. We establish necessary conditions for domains Ω R n which admit the pointwise (p, β)-hardy inequality u(x) Cd Ω(x)
More informationarxiv: v1 [math.ap] 28 Mar 2014
GROUNDSTATES OF NONLINEAR CHOQUARD EQUATIONS: HARDY-LITTLEWOOD-SOBOLEV CRITICAL EXPONENT VITALY MOROZ AND JEAN VAN SCHAFTINGEN arxiv:1403.7414v1 [math.ap] 28 Mar 2014 Abstract. We consider nonlinear Choquard
More informationOn the distance between homotopy classes of maps between spheres
On the distance between homotopy classes of maps between spheres Shay Levi and Itai Shafrir February 18, 214 Department of Mathematics, Technion - I.I.T., 32 Haifa, ISRAEL Dedicated with great respect
More informationLocal semiconvexity of Kantorovich potentials on non-compact manifolds
Local semiconvexity of Kantorovich potentials on non-compact manifolds Alessio Figalli, Nicola Gigli Abstract We prove that any Kantorovich potential for the cost function c = d / on a Riemannian manifold
More information16 1 Basic Facts from Functional Analysis and Banach Lattices
16 1 Basic Facts from Functional Analysis and Banach Lattices 1.2.3 Banach Steinhaus Theorem Another fundamental theorem of functional analysis is the Banach Steinhaus theorem, or the Uniform Boundedness
More informationRelaxation methods and finite element schemes for the equations of visco-elastodynamics. Chiara Simeoni
Relaxation methods and finite element schemes for the equations of visco-elastodynamics Chiara Simeoni Department of Information Engineering, Computer Science and Mathematics University of L Aquila (Italy)
More informationFinite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product
Chapter 4 Hilbert Spaces 4.1 Inner Product Spaces Inner Product Space. A complex vector space E is called an inner product space (or a pre-hilbert space, or a unitary space) if there is a mapping (, )
More informationA TWO PARAMETERS AMBROSETTI PRODI PROBLEM*
PORTUGALIAE MATHEMATICA Vol. 53 Fasc. 3 1996 A TWO PARAMETERS AMBROSETTI PRODI PROBLEM* C. De Coster** and P. Habets 1 Introduction The study of the Ambrosetti Prodi problem has started with the paper
More informationIowa State University. Instructor: Alex Roitershtein Summer Homework #5. Solutions
Math 50 Iowa State University Introduction to Real Analysis Department of Mathematics Instructor: Alex Roitershtein Summer 205 Homework #5 Solutions. Let α and c be real numbers, c > 0, and f is defined
More informationMultivariable Calculus
2 Multivariable Calculus 2.1 Limits and Continuity Problem 2.1.1 (Fa94) Let the function f : R n R n satisfy the following two conditions: (i) f (K ) is compact whenever K is a compact subset of R n. (ii)
More informationSELF-ADJOINTNESS OF SCHRÖDINGER-TYPE OPERATORS WITH SINGULAR POTENTIALS ON MANIFOLDS OF BOUNDED GEOMETRY
Electronic Journal of Differential Equations, Vol. 2003(2003), No.??, pp. 1 8. ISSN: 1072-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu (login: ftp) SELF-ADJOINTNESS
More informationLinear Ordinary Differential Equations
MTH.B402; Sect. 1 20180703) 2 Linear Ordinary Differential Equations Preliminaries: Matrix Norms. Denote by M n R) the set of n n matrix with real components, which can be identified the vector space R
More informationGlobal unbounded solutions of the Fujita equation in the intermediate range
Global unbounded solutions of the Fujita equation in the intermediate range Peter Poláčik School of Mathematics, University of Minnesota, Minneapolis, MN 55455, USA Eiji Yanagida Department of Mathematics,
More informationRecent Trends in Differential Inclusions
Recent Trends in Alberto Bressan Department of Mathematics, Penn State University (Aveiro, June 2016) (Aveiro, June 2016) 1 / Two main topics ẋ F (x) differential inclusions with upper semicontinuous,
More informationON THE HÖLDER CONTINUITY OF MATRIX FUNCTIONS FOR NORMAL MATRICES
Volume 10 (2009), Issue 4, Article 91, 5 pp. ON THE HÖLDER CONTINUITY O MATRIX UNCTIONS OR NORMAL MATRICES THOMAS P. WIHLER MATHEMATICS INSTITUTE UNIVERSITY O BERN SIDLERSTRASSE 5, CH-3012 BERN SWITZERLAND.
More informationDEGREE AND SOBOLEV SPACES. Haïm Brezis Yanyan Li Petru Mironescu Louis Nirenberg. Introduction
Topological Methods in Nonlinear Analysis Journal of the Juliusz Schauder Center Volume 13, 1999, 181 190 DEGREE AND SOBOLEV SPACES Haïm Brezis Yanyan Li Petru Mironescu Louis Nirenberg Dedicated to Jürgen
More informationStatic continuum theory of nematic liquid crystals.
Static continuum theory of nematic liquid crystals. Dmitry Golovaty The University of Akron June 11, 2015 1 Some images are from Google Earth and http://www.personal.kent.edu/ bisenyuk/liquidcrystals Dmitry
More informationThe Skorokhod reflection problem for functions with discontinuities (contractive case)
The Skorokhod reflection problem for functions with discontinuities (contractive case) TAKIS KONSTANTOPOULOS Univ. of Texas at Austin Revised March 1999 Abstract Basic properties of the Skorokhod reflection
More informationStability of Feedback Solutions for Infinite Horizon Noncooperative Differential Games
Stability of Feedback Solutions for Infinite Horizon Noncooperative Differential Games Alberto Bressan ) and Khai T. Nguyen ) *) Department of Mathematics, Penn State University **) Department of Mathematics,
More informationConvergence of Finite Volumes schemes for an elliptic-hyperbolic system with boundary conditions
Convergence of Finite Volumes schemes for an elliptic-hyperbolic system with boundary conditions Marie Hélène Vignal UMPA, E.N.S. Lyon 46 Allée d Italie 69364 Lyon, Cedex 07, France abstract. We are interested
More informationApplications of the compensated compactness method on hyperbolic conservation systems
Applications of the compensated compactness method on hyperbolic conservation systems Yunguang Lu Department of Mathematics National University of Colombia e-mail:ylu@unal.edu.co ALAMMI 2009 In this talk,
More informationSimple waves and a characteristic decomposition of the two dimensional compressible Euler equations
Simple waves and a characteristic decomposition of the two dimensional compressible Euler equations Jiequan Li 1 Department of Mathematics, Capital Normal University, Beijing, 100037 Tong Zhang Institute
More informationDynamic Blocking Problems for Models of Fire Propagation
Dynamic Blocking Problems for Models of Fire Propagation Alberto Bressan Department of Mathematics, Penn State University bressan@math.psu.edu Alberto Bressan (Penn State) Dynamic Blocking Problems 1 /
More informationNONHOMOGENEOUS ELLIPTIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT AND WEIGHT
Electronic Journal of Differential Equations, Vol. 016 (016), No. 08, pp. 1 1. ISSN: 107-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu NONHOMOGENEOUS ELLIPTIC
More informationBLOWUP THEORY FOR THE CRITICAL NONLINEAR SCHRÖDINGER EQUATIONS REVISITED
BLOWUP THEORY FOR THE CRITICAL NONLINEAR SCHRÖDINGER EQUATIONS REVISITED TAOUFIK HMIDI AND SAHBI KERAANI Abstract. In this note we prove a refined version of compactness lemma adapted to the blowup analysis
More informationThe inviscid limit to a contact discontinuity for the compressible Navier-Stokes-Fourier system using the relative entropy method
The inviscid limit to a contact discontinuity for the compressible Navier-Stokes-Fourier system using the relative entropy method Alexis Vasseur, and Yi Wang Department of Mathematics, University of Texas
More informationRegularity of the density for the stochastic heat equation
Regularity of the density for the stochastic heat equation Carl Mueller 1 Department of Mathematics University of Rochester Rochester, NY 15627 USA email: cmlr@math.rochester.edu David Nualart 2 Department
More informationGlobal existence of smooth solutions to two-dimensional compressible isentropic Euler equations for Chaplygin gases
Global existence of smooth solutions to two-dimensional compressible isentropic Euler equations for Chaplygin gases De-Xing Kong a Yu-Zhu Wang b a Center of Mathematical Sciences, Zhejiang University Hangzhou
More informationA one-dimensional nonlinear degenerate elliptic equation
USA-Chile Workshop on Nonlinear Analysis, Electron. J. Diff. Eqns., Conf. 06, 001, pp. 89 99. http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu or ejde.math.unt.edu login: ftp)
More informationON THE REGULARITY OF WEAK SOLUTIONS OF THE 3D NAVIER-STOKES EQUATIONS IN B 1
ON THE REGULARITY OF WEAK SOLUTIONS OF THE 3D NAVIER-STOKES EQUATIONS IN B 1, A. CHESKIDOV AND R. SHVYDKOY ABSTRACT. We show that if a Leray-Hopf solution u to the 3D Navier- Stokes equation belongs to
More informationWELL-POSEDNESS OF THE TWO-DIMENSIONAL GENERALIZED BENJAMIN-BONA-MAHONY EQUATION ON THE UPPER HALF PLANE
WELL-POSEDNESS OF THE TWO-DIMENSIONAL GENERALIZED BENJAMIN-BONA-MAHONY EQUATION ON THE UPPER HALF PLANE YING-CHIEH LIN, C. H. ARTHUR CHENG, JOHN M. HONG, JIAHONG WU, AND JUAN-MING YUAN Abstract. This paper
More informationNonlinear stabilization via a linear observability
via a linear observability Kaïs Ammari Department of Mathematics University of Monastir Joint work with Fathia Alabau-Boussouira Collocated feedback stabilization Outline 1 Introduction and main result
More informationMath The Laplacian. 1 Green s Identities, Fundamental Solution
Math. 209 The Laplacian Green s Identities, Fundamental Solution Let be a bounded open set in R n, n 2, with smooth boundary. The fact that the boundary is smooth means that at each point x the external
More informationThe heat equation in time dependent domains with Neumann boundary conditions
The heat equation in time dependent domains with Neumann boundary conditions Chris Burdzy Zhen-Qing Chen John Sylvester Abstract We study the heat equation in domains in R n with insulated fast moving
More informationMcGill University Math 354: Honors Analysis 3
Practice problems McGill University Math 354: Honors Analysis 3 not for credit Problem 1. Determine whether the family of F = {f n } functions f n (x) = x n is uniformly equicontinuous. 1st Solution: The
More information