hw2sol

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Math 678. Homework 2 Solutions. #3, p.85 Following the proof of the mean value property, denote φ(r)= R - ∂B(0,r) u(y)dS(y) and use the same argument to show that φ 0 (r)= R - B(0,r) Δu(y)dS = - R - B(0,r) f (y)dS. Then fix some > 0 and notice that φ(r) - φ()= Z r φ 0 (s)ds, with φ() u(0) as 0. Since u = g on ∂B(0,r), φ(r)= R - ∂B(0,r) g(y)dS(y). We can use polar coordinates and interchange the order of integration (leav- ing out the term that vanishes as 0) to compute the righthand side: - Z r φ 0 (s)ds = Z r 1 s n-1 (n) Z B(0,s) f (y)dSds = 1 (n) Z r Z s 0 Z ∂B(0,t) f (y) s n-1 dy dt ds = 1 (n) Z r Z r t Z ∂B(0,t) f (y) s n-1 dy ds dt = 1 (n) Z r Z ∂B(0,t) Z r t f (y) s n-1 ds dy dt = 1 (n) Z r Z ∂B(0,t) f (y) Z r t 1 s n-1 ds dy dt = - 1 n(n - 2)α(n) Z r Z ∂B(0,t) f (y) h 1 r n-2 - 1 t n-2 i dy dt = 1 n(n - 2)α(n) Z B(0,r) f (y) h 1 |y| n-2 - 1 r n-2 i dy As 0, this leaves us with u(0) = R - ∂B(0,r) g(y)dS(y)+ 1 n(n - 2)α(n) Z B(0,r) f (y) h 1 r n-2 - 1 |y| n-2 i dy #5, p.85 (a) Using the mean value property argument, we can show that for the same φ(r) as defined above, φ 0 (r)= r n R - B(x,r) Δv(y)dy 0. Let us write φ(r) - φ(0) = Z r 0 φ 0 (s)ds 0, which means that R - ∂B(x,r) v(y)dS(y)= φ(r) φ(0) = v(x). Then notice that Z B(x,r) v(y)dS(y)= Z r 0 Z ∂B(x,s) v(y)dS(y)ds = Z r 0 (n)s n-1 h R - ∂B(x,s) v(y)dS(y) i ds (n) h R r 0 s n-1 ds i v(x)= (n)r n v(x)/n = α(n)r n v(x) The conclusion follows. (b) Suppose there is an interior maximum for v(x) at x 0 . Then u(x 0 )= max ¯ U u = M and by (a) for any ball B(x 0 ,r), M = u(x 0 ) R B(x0,r) v(y)dy 1

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Page 1: hw2sol

Math 678. Homework 2 Solutions.

#3, p.85Following the proof of the mean value property, denote φ(r) =

∫−

∂B(0,r)u(y)dS(y)

and use the same argument to show that φ′(r) =∫−

B(0,r)∆u(y)dS = −

∫−

B(0,r)f(y)dS.

Then fix some ε > 0 and notice that φ(r)−φ(ε) =∫ r

ε

φ′(s)ds, with φ(ε)→ u(0)

as ε→ 0. Since u = g on ∂B(0, r), φ(r) =∫−

∂B(0,r)g(y)dS(y).

We can use polar coordinates and interchange the order of integration (leav-ing out the term that vanishes as ε→ 0) to compute the righthand side:

−∫ r

ε

φ′(s)ds =∫ r

ε

1sn−1nα(n)

∫B(0,s)

f(y)dSds =

1nα(n)

∫ r

ε

∫ s

0

∫∂B(0,t)

f(y)sn−1

dy dt ds =1

nα(n)

∫ r

ε

∫ r

t

∫∂B(0,t)

f(y)sn−1

dy ds dt =

1nα(n)

∫ r

ε

∫∂B(0,t)

∫ r

t

f(y)sn−1

ds dy dt =1

nα(n)

∫ r

ε

∫∂B(0,t)

f(y)∫ r

t

1sn−1

ds dy dt =

− 1n(n− 2)α(n)

∫ r

ε

∫∂B(0,t)

f(y)[ 1rn−2

− 1tn−2

]dy dt =

1n(n− 2)α(n)

∫B(0,r)

f(y)[ 1|y|n−2

− 1rn−2

]dy

As ε→ 0, this leaves us with

u(0) =∫−

∂B(0,r)g(y)dS(y) +

1n(n− 2)α(n)

∫B(0,r)

f(y)[ 1rn−2

− 1|y|n−2

]dy

#5, p.85 (a) Using the mean value property argument, we can show thatfor the same φ(r) as defined above, φ′(r) = r

n

∫−B(x,r) ∆v(y)dy ≥ 0. Let us write

φ(r) − φ(0) =∫ r

0

φ′(s)ds ≥ 0, which means that∫−∂B(x,r) v(y)dS(y) = φ(r) ≥

φ(0) = v(x). Then notice that∫B(x,r)

v(y)dS(y) =∫ r

0

∫∂B(x,s)

v(y)dS(y)ds =∫ r

0

nα(n)sn−1[ ∫−

∂B(x,s)v(y)dS(y)

]ds ≥

nα(n)[ ∫ r

0sn−1ds

]v(x) = nα(n)rnv(x)/n = α(n)rnv(x)

The conclusion follows.

(b) Suppose there is an interior maximum for v(x) at x0. Then u(x0) =maxU u = M and by (a) for any ball B(x0, r), M = u(x0) ≤

∫B(x0,r)

v(y)dy ≤

1

Page 2: hw2sol

M . Equality is achieved when u ≡ M on B(x0, r). For a connected domain, itfollows that u ≡M on U , so maximum principle holds.

(c) Let v(x) = f(u(x)) with f -convex. Any convex function f is continuous,and satisfies Jensen’s inequality on a bounded domain G:

f(∫−Gu(x)dx) ≤

∫−Gf(u(x))dx

If u is harmonic, u(x) =∫−B(x,r) u(y)dy, so from Jensen’s inequality, f(u(x)) ≤∫

−B(x,r) f(u(y))dy. So (a) holds even if the function is not smooth.

To show that the function is subharmonic according to the definition−∆(f(u(x))) ≤0 in the case the function f ∈ C2(U), we can use direct computation:

−∆v = −n∑i=1

vxixi= −

n∑i=1

f ′′(u)u2xi−

n∑i=1

f ′(u)uxixi= −f ′′(u)

n∑i=1

u2xi−f ′(u)∆u ≤ 0.

(d) You can notice |Du| is harmonic for a harmonic function u (direct buttedious computation). Since f(x) = |x|2 is a convex function on R, we can usethe result of (c), which proves that the function |Du|2 is subharmonic.

You can also show this by direct computation:

vxixi=

n∑k=1

(2u2xixi

+ 2uxkxixi) ≥ 2

n∑k=1

uxkxixi.

Summing over all i and noticing that∑i

∑k

uxkxixi =∑k

∂xk

∑i

uxixi = 0,

we get the conclusion.

Part II.Consider any ball B(x, r) ⊂ U , a function v ∈ C(U) such that v(x) ≤∫

−B(x,r) vdy and a harmonic function u defined on a domain that includes thisball. Consider the difference w = v − u. Clearly, w ≤ 0 on ∂B(x, r). We needto show w ≤ 0 in B(x, r).

The function w is subharmonic on B(x, r) in the sense that w(x) = u(x) −v(x) ≤

∫−B(x,r) w(y)dy, continuous on B(x, r) and hence satisfies the strong, and

hence the weak maximum principle, as shown in 5(b) above. So maxB(x,r)(w) =max∂B(x,r) w = 0, as needed.

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