成長機構

Similar documents
1 (Berry,1975) 2-6 p (S πr 2 )p πr 2 p 2πRγ p p = 2γ R (2.5).1-1 : : : : ( ).2 α, β α, β () X S = X X α X β (.1) 1 2

O x y z O ( O ) O (O ) 3 x y z O O x v t = t = 0 ( 1 ) O t = 0 c t r = ct P (x, y, z) r 2 = x 2 + y 2 + z 2 (t, x, y, z) (ct) 2 x 2 y 2 z 2 = 0

TOP URL 1

2,200 WEB * Ξ ( ) η ( ) DC 1.5 i

30

LLG-R8.Nisus.pdf

201711grade1ouyou.pdf

x E E E e i ω = t + ikx 0 k λ λ 2π k 2π/λ k ω/v v n v c/n k = nω c c ω/2π λ k 2πn/λ 2π/(λ/n) κ n n κ N n iκ k = Nω c iωt + inωx c iωt + i( n+ iκ ) ωx

医系の統計入門第 2 版 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 第 2 版 1 刷発行時のものです.

I-2 (100 ) (1) y(x) y dy dx y d2 y dx 2 (a) y + 2y 3y = 9e 2x (b) x 2 y 6y = 5x 4 (2) Bernoulli B n (n = 0, 1, 2,...) x e x 1 = n=0 B 0 B 1 B 2 (3) co

( )

Microsoft Word - 11問題表紙(選択).docx

1 (1) () (3) I 0 3 I I d θ = L () dt θ L L θ I d θ = L = κθ (3) dt κ T I T = π κ (4) T I κ κ κ L l a θ L r δr δl L θ ϕ ϕ = rθ (5) l

) a + b = i + 6 b c = 6i j ) a = 0 b = c = 0 ) â = i + j 0 ˆb = 4) a b = b c = j + ) cos α = cos β = 6) a ˆb = b ĉ = 0 7) a b = 6i j b c = i + 6j + 8)

Z: Q: R: C: sin 6 5 ζ a, b

2 G(k) e ikx = (ik) n x n n! n=0 (k ) ( ) X n = ( i) n n k n G(k) k=0 F (k) ln G(k) = ln e ikx n κ n F (k) = F (k) (ik) n n= n! κ n κ n = ( i) n n k n

( ) sin 1 x, cos 1 x, tan 1 x sin x, cos x, tan x, arcsin x, arccos x, arctan x. π 2 sin 1 x π 2, 0 cos 1 x π, π 2 < tan 1 x < π 2 1 (1) (

No δs δs = r + δr r = δr (3) δs δs = r r = δr + u(r + δr, t) u(r, t) (4) δr = (δx, δy, δz) u i (r + δr, t) u i (r, t) = u i x j δx j (5) δs 2

Untitled

.2 ρ dv dt = ρk grad p + 3 η grad (divv) + η 2 v.3 divh = 0, rote + c H t = 0 dive = ρ, H = 0, E = ρ, roth c E t = c ρv E + H c t = 0 H c E t = c ρv T

QMII_10.dvi

64 3 g=9.85 m/s 2 g=9.791 m/s 2 36, km ( ) 1 () 2 () m/s : : a) b) kg/m kg/m k

V(x) m e V 0 cos x π x π V(x) = x < π, x > π V 0 (i) x = 0 (V(x) V 0 (1 x 2 /2)) n n d 2 f dξ 2ξ d f 2 dξ + 2n f = 0 H n (ξ) (ii) H

ω 0 m(ẍ + γẋ + ω0x) 2 = ee (2.118) e iωt x = e 1 m ω0 2 E(ω). (2.119) ω2 iωγ Z N P(ω) = χ(ω)e = exzn (2.120) ϵ = ϵ 0 (1 + χ) ϵ(ω) ϵ 0 = 1 +

TOP URL 1

simx simxdx, cosxdx, sixdx 6.3 px m m + pxfxdx = pxf x p xf xdx = pxf x p xf x + p xf xdx 7.4 a m.5 fx simxdx 8 fx fx simxdx = πb m 9 a fxdx = πa a =

TOP URL 1


() (, y) E(, y) () E(, y) (3) q ( ) () E(, y) = k q q (, y) () E(, y) = k r r (3).3 [.7 ] f y = f y () f(, y) = y () f(, y) = tan y y ( ) () f y = f y

微分積分 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. このサンプルページの内容は, 初版 1 刷発行時のものです.

18 I ( ) (1) I-1,I-2,I-3 (2) (3) I-1 ( ) (100 ) θ ϕ θ ϕ m m l l θ ϕ θ ϕ 2 g (1) (2) 0 (3) θ ϕ (4) (3) θ(t) = A 1 cos(ω 1 t + α 1 ) + A 2 cos(ω 2 t + α

W u = u(x, t) u tt = a 2 u xx, a > 0 (1) D := {(x, t) : 0 x l, t 0} u (0, t) = 0, u (l, t) = 0, t 0 (2)

II A A441 : October 02, 2014 Version : Kawahira, Tomoki TA (Kondo, Hirotaka )

S I. dy fx x fx y fx + C 3 C dy fx 4 x, y dy v C xt y C v e kt k > xt yt gt [ v dt dt v e kt xt v e kt + C k x v + C C k xt v k 3 r r + dr e kt S dt d

x,, z v = (, b, c) v v 2 + b 2 + c 2 x,, z 1 i = (1, 0, 0), j = (0, 1, 0), k = (0, 0, 1) v 1 = ( 1, b 1, c 1 ), v 2 = ( 2, b 2, c 2 ) v

I A A441 : April 15, 2013 Version : 1.1 I Kawahira, Tomoki TA (Shigehiro, Yoshida )

(1.2) T D = 0 T = D = 30 kn 1.2 (1.4) 2F W = 0 F = W/2 = 300 kn/2 = 150 kn 1.3 (1.9) R = W 1 + W 2 = = 1100 N. (1.9) W 2 b W 1 a = 0

untitled

II ( ) (7/31) II ( [ (3.4)] Navier Stokes [ (6/29)] Navier Stokes 3 [ (6/19)] Re

t = h x z z = h z = t (x, z) (v x (x, z, t), v z (x, z, t)) ρ v x x + v z z = 0 (1) 2-2. (v x, v z ) φ(x, z, t) v x = φ x, v z


H.Haken Synergetics 2nd (1978)

Note.tex 2008/09/19( )

c y /2 ddy = = 2π sin θ /2 dθd /2 [ ] 2π cos θ d = log 2 + a 2 d = log 2 + a 2 = log 2 + a a 2 d d + 2 = l

. ev=,604k m 3 Debye ɛ 0 kt e λ D = n e n e Ze 4 ln Λ ν ei = 5.6π / ɛ 0 m/ e kt e /3 ν ei v e H + +e H ev Saha x x = 3/ πme kt g i g e n

p = mv p x > h/4π λ = h p m v Ψ 2 Ψ

本文/目次(裏白)

S I. dy fx x fx y fx + C 3 C vt dy fx 4 x, y dy yt gt + Ct + C dt v e kt xt v e kt + C k x v k + C C xt v k 3 r r + dr e kt S Sr πr dt d v } dt k e kt

KENZOU

Gmech08.dvi

H 0 H = H 0 + V (t), V (t) = gµ B S α qb e e iωt i t Ψ(t) = [H 0 + V (t)]ψ(t) Φ(t) Ψ(t) = e ih0t Φ(t) H 0 e ih0t Φ(t) + ie ih0t t Φ(t) = [

.5 z = a + b + c n.6 = a sin t y = b cos t dy d a e e b e + e c e e e + e 3 s36 3 a + y = a, b > b 3 s363.7 y = + 3 y = + 3 s364.8 cos a 3 s365.9 y =,

gr09.dvi

e a b a b b a a a 1 a a 1 = a 1 a = e G G G : x ( x =, 8, 1 ) x 1,, 60 θ, ϕ ψ θ G G H H G x. n n 1 n 1 n σ = (σ 1, σ,..., σ N ) i σ i i n S n n = 1,,

液晶の物理1:連続体理論(弾性,粘性)

pdf

meiji_resume_1.PDF

N cos s s cos ψ e e e e 3 3 e e 3 e 3 e

24 I ( ) 1. R 3 (i) C : x 2 + y 2 1 = 0 (ii) C : y = ± 1 x 2 ( 1 x 1) (iii) C : x = cos t, y = sin t (0 t 2π) 1.1. γ : [a, b] R n ; t γ(t) = (x

4. ϵ(ν, T ) = c 4 u(ν, T ) ϵ(ν, T ) T ν π4 Planck dx = 0 e x 1 15 U(T ) x 3 U(T ) = σt 4 Stefan-Boltzmann σ 2π5 k 4 15c 2 h 3 = W m 2 K 4 5.

,. Black-Scholes u t t, x c u 0 t, x x u t t, x c u t, x x u t t, x + σ x u t, x + rx ut, x rux, t 0 x x,,.,. Step 3, 7,,, Step 6., Step 4,. Step 5,,.


untitled


73

: 2005 ( ρ t +dv j =0 r m m r = e E( r +e r B( r T 208 T = d E j 207 ρ t = = = e t δ( r r (t e r r δ( r r (t e r ( r δ( r r (t dv j =

6 2 T γ T B (6.4) (6.1) [( d nm + 3 ] 2 nt B )a 3 + nt B da 3 = 0 (6.9) na 3 = T B V 3/2 = T B V γ 1 = const. or T B a 2 = const. (6.10) H 2 = 8π kc2

untitled

(5) 75 (a) (b) ( 1 ) v ( 1 ) E E 1 v (a) ( 1 ) x E E (b) (a) (b)

1: 3.3 1/8000 1/ m m/s v = 2kT/m = 2RT/M k R 8.31 J/(K mole) M 18 g 1 5 a v t πa 2 vt kg (

概況



構造と連続体の力学基礎

tomocci ,. :,,,, Lie,,,, Einstein, Newton. 1 M n C. s, M p. M f, p d ds f = dxµ p ds µ f p, X p = X µ µ p = dxµ ds µ p. µ, X µ.,. p,. T M p.

(3) (2),,. ( 20) ( s200103) 0.7 x C,, x 2 + y 2 + ax = 0 a.. D,. D, y C, C (x, y) (y 0) C m. (2) D y = y(x) (x ± y 0), (x, y) D, m, m = 1., D. (x 2 y

TOP URL 1

6kg 1.1m 1.m.1m.1 l λ ϵ λ l + λ l l l dl dl + dλ ϵ dλ dl dl + dλ dl dl 3 1. JIS 1 6kg 1% 66kg 1 13 σ a1 σ m σ a1 σ m σ m σ a1 f f σ a1 σ a1 σ m f 4

5 5.1 E 1, E 2 N 1, N 2 E tot N tot E tot = E 1 + E 2, N tot = N 1 + N 2 S 1 (E 1, N 1 ), S 2 (E 2, N 2 ) E 1, E 2 S tot = S 1 + S 2 2 S 1 E 1 = S 2 E

: , 2.0, 3.0, 2.0, (%) ( 2.

( ; ) C. H. Scholz, The Mechanics of Earthquakes and Faulting : - ( ) σ = σ t sin 2π(r a) λ dσ d(r a) =

基礎数学I

2 1 x 2 x 2 = RT 3πηaN A t (1.2) R/N A N A N A = N A m n(z) = n exp ( ) m gz k B T (1.3) z n z = m = m ρgv k B = erg K 1 R =


all.dvi

I 1

( ) ( 40 )+( 60 ) Schrödinger 3. (a) (b) (c) yoshioka/education-09.html pdf 1

SO(3) 7 = = 1 ( r ) + 1 r r r r ( l ) (5.17) l = 1 ( sin θ ) + sin θ θ θ ϕ (5.18) χ(r)ψ(θ, ϕ) l ψ = αψ (5.19) l 1 = i(sin ϕ θ l = i( cos ϕ θ l 3 = i ϕ


) ] [ h m x + y + + V x) φ = Eφ 1) z E = i h t 13) x << 1) N n n= = N N + 1) 14) N n n= = N N + 1)N + 1) 6 15) N n 3 n= = 1 4 N N + 1) 16) N n 4

( ) Note (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ, µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) 3 * 2) [ ] [ ] [ ] ν e ν µ ν τ e


m(ẍ + γẋ + ω 0 x) = ee (2.118) e iωt P(ω) = χ(ω)e = ex = e2 E(ω) m ω0 2 ω2 iωγ (2.119) Z N ϵ(ω) ϵ 0 = 1 + Ne2 m j f j ω 2 j ω2 iωγ j (2.120)

講義ノート 物性研究 電子版 Vol.3 No.1, (2013 年 T c µ T c Kammerlingh Onnes 77K ρ 5.8µΩcm 4.2K ρ 10 4 µωcm σ 77K ρ 4.2K σ σ = ne 2 τ/m τ 77K

18 2 F 12 r 2 r 1 (3) Coulomb km Coulomb M = kg F G = ( ) ( ) ( ) 2 = [N]. Coulomb

1. 4cm 16 cm 4cm 20cm 18 cm L λ(x)=ax [kg/m] A x 4cm A 4cm 12 cm h h Y 0 a G 0.38h a b x r(x) x y = 1 h 0.38h G b h X x r(x) 1 S(x) = πr(x) 2 a,b, h,π

i 18 2H 2 + O 2 2H 2 + ( ) 3K

Mathematical Logic I 12 Contents I Zorn

III 1 (X, d) d U d X (X, d). 1. (X, d).. (i) d(x, y) d(z, y) d(x, z) (ii) d(x, y) d(z, w) d(x, z) + d(y, w) 2. (X, d). F X.. (1), X F, (2) F 1, F 2 F


Transcription:

j im πmkt jin jim π mkt j q out j q im π mkt jin j j q out out π mkt π mkt dn dt πmkt dn v( ) Rmax bf dt πmkt

R v ( J J ), J J, J J + + T T, J J m + Q+ / kt Q / kt + ( Q Q+ )/ ktm l / ktm J / J, l Q Q ; + m J J J Q / kt ( Q Q+ )/ kt Q / kt Q+ / ktm Q / kt Q / ktm + + R v J Q / ktm R aν vl T/ ktmt + Q+ / ktm Q+ / k( / T / Tm) Q / k( / T / Tm) + / T / T T/ T T m R v J + [ ] m Q+ / ktm Q+ T / ktmt Q T / ktmt Q+ / ktm + l / ktm Q / ktm Q+ / ktm J [ ] vj [] * [] * Q T/ kt T + Q T/ ktt l T/ kt T + m m m J aν, J aν aν + Rmax vνac x( G / kt) σ dolv j in α j im α πmkt v( ) R α πmkt R max

dn jim ωn jim n/ τ dt t / τ t / τ n A+ B n B / τ t / τ t / τ B / τ jim A / τ B / τ A τ j B A( Q n( ) ) im t / τ τ t / τ n τ jim( ) ( ) πmkt τ nat πmkt n t Dimnion Wln (, ) { Wl ( +, n ) + Wl (, n )} Wln (, + ) Wln (, ) { Wl ( +, n) Wln (, ) + Wl (, n)} [{ Wl ( +, n) Wln (, )} { Wln (, ) Wl (, n)}] t nτ', x la W( l, n) W( x, t) Wxt Wln Wxt τ Wxt τ (, ) (, + ) (, + ') (,) + ' + t Wl n Wx at Wxt a Wxt (, ) W ( x, t) ( ±, ) ( ±, ) (, ) ± + a + x x Wx τ' (, t) a W ( x, t) t x Wxt (, ) a W ( x, t) (, ) a, ', D W x t, D a τ t τ' x x τ' 3 Dimnion Wxt (, ) (, ) D W x t, D a t x 6τ'

n! t, l W( l, n) δ( l, n) W( l, n) n {( n+ l)}!{ ( n l)}! l / n l, n >>, W( l, n) ( Gau ditri.) πn Stirling' formula log n! nlogn n log Wln (, ) nlogn n nlog ( n+ l)log ( n+ l) + ( n+ l) ( n l)log ( n l) + ( n l) n+ l nlogn nlog nlog ( n l ) llog 4 n l l log ( n l ) log+ logn 4 n n+ l l l log log n (log n ) n l + n n l n l l nlogn nlog n( log+ log n ) l n n l l l n n n lwlndl (, ) < l > n, < x >< l > a na, Wlndl (, ) t < x > a Dt ( Eintin rlation ), τ 3 Dimnion < x >< y >< z > Dt

n t r r j j x y jz + div j, divj + + x y z

n t r r div j + j r n j Dgrad n Dn grad Dngradσ Dngrad( σ σ) n gradn n n n r σ ( σ) (,, ), j (, Dn, ) x y z y r jy divj Dn σ σ y y ( ) n n τ j n n τ ( ) n n n n j ( n n) ( n n ) ( ) (( σ + ) ( σ + ) ) ( σ σ) τ τ τ n τ τ x d ψ ψ ψ ±, dy y / x ψ( y) σ y / x σ ( y) σ y / x [ ] n ( y) n + ( n n ) y / x [ ] j( ) D dn x / τ n v n n dy n y x ( ) τ xσ n τ n τ n n x

n n x( W / kt) v σxνx( W/ kt), W W + Ea x d ψ ψ dy ψ A + B dψ dy y / x + y / x n n n ψ, n ( ) n n n ( A+ B) n ( A+ B+ ) n, A x x B x + x x B x ψ'( λ ) +, A λ x n A( + ) σ n λ λ λ x x x A σ /( + ), B σ /( + ) λ λ λ j ( ) D dn D λ v + ( ) σ tanh( ) n n dy n n A B x D n A x n x B D n n x x vy v λ ( ) tanh x v λ x

πr G µ + πκ r f d G πr µ + πκ ρ dr f πκ G( ρ) f µ fκ µ fκ µ kt log, ρ fκ / ktlog ρ ρ f κ / ktlog ρ fκ kt / log v v f κ f κ x, x, ρkt ρ kt f κ ρkt f κ ρ kt ρ ρ v v ρ ρ * J ν q x( G / kt) + J f * n x( G * / kt) at

dgn dn J ZN b n g * * x( n / kt ) Z πkt Å / ' t w ( ) w π ' Jπ vt dt t 3 Jv / 3 A v / 3 v A ' tw JA J Jv / 3

r r vt + ln( + ) ( + ) θ + ρ 3ρ 3 ρ + 3 r ρ ( + π 3 ) λ v σxνx ( W/ kt) tanh x R a W kt x λ νx ( / ) σ tanh λ x R aν x W/ kt σ σ aν x ( W/ kt) tanh σ σ ( ) σ σ σ < ( ) > R aνx W/ kt σ σ σ σ x x x ktσ σ σ λ ρ fκ f / x kt κ

µ ( νi + ) i i ( ) νν i j E E ( ν ν + ν ν ) φ ZT ( ) x( ) kt i, j i, j+ i+, j i, j i j 4 r H J i r j H J σ i σ j (σ ±)

UT ( ) U ST ( ) U, E U( T) U av E E / kt E / kt