観測量と物理量の関係.pptx
|
|
- ゆめじ くぬぎ
- 6 years ago
- Views:
Transcription
1 (I! F! ( (! "! (#, $ #, $!! di! d"! =!I! + B! (T ex T ex : "! n 2 / g 2 = exp(! h! n 1 / g 1 kt ex " I! ("! = I! (0e "! +! e ("! " #! B! [T ex ("! ]d " d! " = # " ds = h" 4$ %("(n dsb h" 1 12 [1! exp(! ] kt ex 0 "! (RL Eq.1.78
2 d! " = # " ds = h" 4$ %("(n dsb h" 1 12 [1! exp(! ] kt ex B 12 = cm -3 A 21 2h! 3 / c 2 = 32" 4 µ 12 3ch 2 d! " = 8# 3 µ 12 [ " c $("]dn 1[1! exp(! h" ] kt ex dn 1 =n 1 ds (n 1 cm -2 (line profile "v=c/[!$(!] d! = 8" 3 µ 12 (km s -1-1 dn 1 h# [1" exp(" ]!v kt ex d! " (RL Eq.1.78 (RL Eq ~ 1!!!("!!(" d! =1 "v/c=1/[!$ (!]!!! v I! "! (0 %! (& bg ($(!"0 "! ( "!!I! = I! " B! = e ("! "" # $! B! [T ex (" #! ]! d "#! " (1" e "! B! 0 T ex!i!!i! = I! " B! = (1" e "! [B! (T ex " B! ]! " = N 1 [ " c #("]8$ 3 µ 12 [1! exp(! h" kt ex ] B!! "" # (
3 "! F! F! = " I! (",#cos" d! cos# #=0 (cos# P! (#, $ ( F! = " I! (",#P! (",#d! P! (0, 0 =1 P! (#, $ (0, 0 $ % "! A = P! (",#d! P = 1 2 A ed! " I! (",#P! (",#d! A e A e $ % =& 2 ( P=kT A d! (! T A =! 2 2k 1 " I " (#,$P " (#,$d! =! 2 I "! A 2k "! =%! (T R T R (T B "! =2kT R /& 2! T A = 1 " T R (!,"P # (!,"d! = T R! A D A e #D 2 $ A #(&/D 2
4 "! F! = " I! P! (",#d! = I!! A T A = 1 " T R P! (",#d! = T R! A "! ($ s F! = " I!! d! = I!! S! S T A = 1! " P! (",#d! = T S R! A! S! A!I! = (1! e! " [B! (T ex! B! ]!T A = (1! e! " [T ex!t bg ] ( T A!T A T bg! "! T R =& 2 "! /2k T R T ( T R =! 2 I! 2k = h! k 1 exp(h! / kt!1 " f (T ( (T A ( (T R =T A */'
5 " I! ("! = I! (0e "! +! e ("! " #! B! [T ex ("! ]d " d! " = 8# 3 µ 12 0 [ " c $("]dn h" 1 [1! exp(! ] kt ex (!I = (1" e! [B " (T ex " B " ]! = 8" 3 µ 12 N 1 h# [1" exp(" ]!v kt ex "!!I = (1" e! [B " (T ex " B " ]! = 8" 3 µ 12 N 1 h# [1" exp(" ]!v kt ex n 1 n 2 ( n 1 n 2 i n i n 0 n i / n 0 = exp(-e i / kt k n i n i (rate equations (
6 (rate equations dn j dt dn j dt = (All transitions to j-(all transitions from j!=!0 =! [(Transition to j -(Transition from j]+! [(Transition to j -(Transition from j] Radiative dn j dt Collisional =![(A ij + B ij Jn i " B ji Jn j ]"![(A ji + B ji Jn j " B ij Jn i ]+!(C ij n i -C ji n j i> j i< j C ij i!j (s -1 ( (~80%~20% n (cm -3 v (cm/s ((v (cm 2 C ij = n <! ij v > i# j C ij n i = C ji n j C ij C ji = n j n i = g j g i exp(! E ij kt C ij = n <! ij v > v (( v C ij C ji = g j g i exp(! E ij kt k T k C ij (C ji
7 dn j dt =![(A ij + B ij Jn i! B ji Jn j ]!![(A ji + B ji Jn j! B ij Jn i ]+!(C ij n i -C ji n j = 0 i> j i< j J J n j I I n j n j ( 3 K I J n j I J ( I J ( n j i! j!i = (1" e! [B " (T ex " B " ] # B " (T ex " B " ("" T ex (n(h 2, N mol, T k (T ex =T k "" ( T k 12 CO ( 12 CO ( ( T k (J, K=(1, 1(2, 2 CO
8 !I = (1" e! [B " (T k " B " ] #![B " (T k " B " ]! = 8" 3 µ 12 N 1 h# [1" exp(" ]!v kt k N 1 T k ("v T k ( N 1 N mol (cm -2 N mol = N 1 Z g 1 exp(!e 10 kt k Z"E CO C 18 O CO (isotopologues 13 CO C 18 O Dickman (1978, ApJS, 37, CO (J=1-0 (Av; N H =2$10 21 Av cm -2 N(H 2 = (5.0 ± 2.5!10 5!N( 13 CO N( 13 CO = N 0 Z =!v( 13 CO!" (1" 0!Z 8! 3 µ 2 1" exp("h# / kt k N(H 2 (cm -2 (cm 2 H 2 ($
9 !I = (1" e! [B " (T ex " B " ]! = 8" 3 µ 12 N 1 h# [1" exp(" ]!v kt ex ( T ex (n(h 2, N mol, T k I (n(h 2, T k I ( (Sobolev V(RR (Large Velocity Gradient Goldreich & Kwan (1974, ApJ, 189, 441; GK74 Scoville & Solomon (1974, ApJ, 187, L71; SS74 Castor (1970, MNRAS, 149, 111 Townes & Schawlow (1975; TS75
10 The Large Velocity Gradient (LVG Approximation LVG V(R R (rate equations (Emergent Specific Intensity LVG Sobolev WR ( T ex!i = (1" e! [B(T ex " B ]!!I = $ e (! "! # B[T ex (! # ]d! # " (1" e! B 0 T B = (1! e! [ f (T ex! f ] f (T! h! k 1 exp(h! / kt "1
11 n 2 n 1 = g 2 g 1 exp(! h! 12 kt ex GK74 n 2 n 1 = exp(! h! 12 kt ex n 1, n 2 ( g J =2J+1! " J=0 g J =1 o o /(g J n mol (n mol ' d! = 8" 3 µ 12 dn 1 h# [1" exp(" ]!v kt ex J (=0, 1, 2,! ( "J=1 1J2J+1 dn J g J dn d! J,J+1 = 8" 3 µ J,J+1! J,J+1 = 8" 3 µ J,J+1 N!v g (n " n J J J+1 dn!v g J ( " +1
12 µ (J, J+1 TS75 (Eq.1-76 µ J,J+1 = µ 2 J +1 2J +1 µ J,J+1 g J = µ J+1, J g J+1 g J =2J+1 µ J+1,J = µ 2 J +1 2J + 3 µ! J,J+1 = 8" 3 µ 2 ' ' N!v (J +1( " +1 B J+1,J = g J g J+1 B J,J+1 =!!!!!!!!= 32" 4 µ 2 3ch 2 J +1 2J + 3 E J = hbj(j +1 A J+1,J! J+1,J = (E J+1! E J / h = 2B(J +1 2h! 3 J+1,J!!!!/c = 32" 4 µ J+1,J 2 3ch 2 (RL Eq (GK74 Eq.4
13 T B (J +1, J = (1! e! J,J+1 [ f [T ex (J, J +1]! f ]! J+1,J = 8" 3 µ 2 N!v (J +1( " +1 ( f [T ex (J, J +1] = h! k 1 / +1!1 µj N "V N (N/"V (+1 / T A (J=0, 1, 2,3! (rate equations T A n(h 2, T k, N dn g J J = g J+1 +1 A J+1,J + (g J+1 +1 B J+1,J! g J B J,J+1 J J+1,J dt!!!!!!!!!!!!g J A J,J-1! (g J B J,J-1! g J-1-1 B J-1,J J J,J-1 #!!!!!!!!!!!+ (C LJ g J g L n L! C JL g L g J L"J (GK74 Eq.10 C JL [C 12 /C 21 =exp(-h# 12 /kt k ]C C JL C JL /g L Sobolev
14 Castor (1970 1! exp(!"! = " * J J+1,J = (1!! J+1,J B(T ex +! J+1,J B [g J+1 +1 A J+1,J + (g J+1 +1 B J+1,J! g J B J,J+1 B ]! J+1,J![g J A J,J-1 + (g J B J,J-1! g J-1-1 B J-1,J B ]! J,J-1 + #(C LJ g J g L n L! C JL g L g J = 0 L"J! J+1,J = 1! exp(!" J+1,J " J+1,J (GK74 Eq.11 ( g J+1 +1 A J+1,J + (g J+1 +1 B J+1,J! g J B J,J+1 B(T ex = 0
15 T ex T B = (1! e! [ f (T ex! f ]!!!!!"![ f (T ex! f ]!!!(! # 0!!!!!" f (T ex! f!!!(! # $ ( f (T! h! k 1 exp(h! / kt "1 LVG T ex C N/%V Cn(H 2 +He<&v> (T ex!c!(n / "v!n < " v > n(h 2 +He (N/%V (photon trapping LVG J IJ " " J C IJ =n(h 2, He, <& IJ v> n(h 2 T k T k <& IJ v> T k, N/"V, n(h 2 ( (T k, N/"V, n(h 2 (N/DV, T ex ( T A (, T ex => T A (T k, N/"V, n(h 2 T B T k T B (N/"V, n, T B (n mol /(dv/dr, n, T B (X mol /(dv/dr, n [X mol =n mol /n(h 2 ] T k 12 CO N/ "Vn(H 2 2
16 CO (SS74 (N/%V $n(h 2 CO (Ratio (superthermal (population inversion (SS74 Fig. 1b. The ratio of antenna temperature in the CO J=2 1 and J=1 0 transitions obtained from 10- level calculations at T k =40 K.
17 (SS74 CS µ µ µ (n(h 2 ~10 3 cm -3 CS (T ex <T k ; sub-thermal CS! Fig. 2. Contours of antenna temperature in the J=1 0, 2 1, 3 2 CS transitions from 10-level calculations at T k =40 K. (SS74 CO T B ~ N/"V T B ~n(h 2 Fig. 3. The dramatic effects of radiative trapping are demonstrated for the J=1 0 CO transition in the two-level approximation. Dashed contours are obtained for excitation only by H 2 collisions; solid contours include excitation by trapped radiation.
18 (Sakamoto et al. 1994
( ) ,
II 2007 4 0. 0 1 0 2 ( ) 0 3 1 2 3 4, - 5 6 7 1 1 1 1 1) 2) 3) 4) ( ) () H 2.79 10 10 He 2.72 10 9 C 1.01 10 7 N 3.13 10 6 O 2.38 10 7 Ne 3.44 10 6 Mg 1.076 10 6 Si 1 10 6 S 5.15 10 5 Ar 1.01 10 5 Fe 9.00
More informationAHPを用いた大相撲の新しい番付編成
5304050 2008/2/15 1 2008/2/15 2 42 2008/2/15 3 2008/2/15 4 195 2008/2/15 5 2008/2/15 6 i j ij >1 ij ij1/>1 i j i 1 ji 1/ j ij 2008/2/15 7 1 =2.01/=0.5 =1.51/=0.67 2008/2/15 8 1 2008/2/15 9 () u ) i i i
More information輻射の量子論、選択則、禁制線、許容線
Radiative Processes in Astrophysics 005/8/1 http://wwwxray.ess.sci.osaka- u.ac.jp/~hayasida Semi-Classical Theory of Radiative Transitions r r 1/ 4 H = ( cp ea) m c + + eφ nonrelativistic limit, Coulomb
More information006 11 8 0 3 1 5 1.1..................... 5 1......................... 6 1.3.................... 6 1.4.................. 8 1.5................... 8 1.6................... 10 1.6.1......................
More information/ Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiat
/ Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiation and the Continuing Failure of the Bilinear Formalism,
More informationE 1/2 3/ () +3/2 +3/ () +1/2 +1/ / E [1] B (3.2) F E 4.1 y x E = (E x,, ) j y 4.1 E int = (, E y, ) j y = (Hall ef
4 213 5 8 4.1.1 () f A exp( E/k B ) f E = A [ k B exp E ] = f k B k B = f (2 E /3n). 1 k B /2 σ = e 2 τ(e)d(e) 2E 3nf 3m 2 E de = ne2 τ E m (4.1) E E τ E = τe E = / τ(e)e 3/2 f de E 3/2 f de (4.2) f (3.2)
More informationpositron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) MeV : thermalization m psec 100
positron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) 0.5 1.5MeV : thermalization 10 100 m psec 100psec nsec E total = 2mc 2 + E e + + E e Ee+ Ee-c mc
More information6 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
1 6 6.1 (??) (P = ρ rad /3) ρ rad T 4 d(ρv ) + PdV = 0 (6.1) dρ rad ρ rad + 4 da a = 0 (6.2) dt T + da a = 0 T 1 a (6.3) ( ) n ρ m = n (m + 12 ) m v2 = n (m + 32 ) T, P = nt (6.4) (6.1) d [(nm + 32 ] )a
More information「諸雑公文書」整理の中間報告
30 10 3 from to 10 from to ( ) ( ) 20 20 20 20 20 35 8 39 11 41 10 41 9 41 7 43 13 41 11 42 7 42 11 41 7 42 10 4 4 8 4 30 10 ( ) ( ) 17 23 5 11 5 8 8 11 11 13 14 15 16 17 121 767 1,225 2.9 18.7 29.8 3.9
More information(Blackbody Radiation) (Stefan-Boltzmann s Law) (Wien s Displacement Law)
( ) ( ) 2002.11 1 1 1.1 (Blackbody Radiation).............................. 1 1.2 (Stefan-Boltzmann s Law)................ 1 1.3 (Wien s Displacement Law)....................... 2 1.4 (Kirchhoff s Law)...........................
More informationn ξ n,i, i = 1,, n S n ξ n,i n 0 R 1,.. σ 1 σ i .10.14.15 0 1 0 1 1 3.14 3.18 3.19 3.14 3.14,. ii 1 1 1.1..................................... 1 1............................... 3 1.3.........................
More information弾性定数の対称性について
() by T. oyama () ij C ij = () () C, C, C () ij ji ij ijlk ij ij () C C C C C C * C C C C C * * C C C C = * * * C C C * * * * C C * * * * * C () * P (,, ) P (,, ) lij = () P (,, ) P(,, ) (,, ) P (, 00,
More informationThe Physics of Atmospheres CAPTER :
The Physics of Atmospheres CAPTER 4 1 4 2 41 : 2 42 14 43 17 44 25 45 27 46 3 47 31 48 32 49 34 41 35 411 36 maintex 23/11/28 The Physics of Atmospheres CAPTER 4 2 4 41 : 2 1 σ 2 (21) (22) k I = I exp(
More information空き容量一覧表(154kV以上)
1/3 A. 電気所 ( 発電所, 変電所, 配電塔 ) における変圧器の空き容量 覧 < 留意事項 > (1) 空容量は 安であり 系統接続の前には 接続検討のお申込みによる詳細検討が必要となります その結果 空容量が変更となる場合があります (2) 熱容量を考慮した空き容量を記載しております その他の要因 ( や系統安定度など ) で連系制約が発 する場合があります (3) 表 は 既に空容量がないため
More information2/8 一次二次当該 42 AX 変圧器 なし 43 AY 変圧器 なし 44 BA 変圧器 なし 45 BB 変圧器 なし 46 BC 変圧器 なし
1/8 A. 電気所 ( 発電所, 変電所, 配電塔 ) における変圧器の空き容量一覧 < 留意事項 > (1) 空容量は目安であり 系統接続の前には 接続検討のお申込みによる詳細検討が必要となります その結果 空容量が変更となる場合があります (2) 特に記載のない限り 熱容量を考慮した空き容量を記載しております その他の要因 ( や系統安定度など ) で連系制約が発生する場合があります (3)
More informationatomic line spectrum emission line absorption line atom proton neutron nuclei electron Z atomic number A mass number neutral atom ion energy
1 22 22.1 atomic line spectrum emission line absorption line atom proton neutronnuclei electron Z atomic number A mass number neutral atom ion energy level ground stateexcited state ionized state 22.2
More information1 1 1 1-1 1 1-9 1-3 1-1 13-17 -3 6-4 6 3 3-1 35 3-37 3-3 38 4 4-1 39 4- Fe C TEM 41 4-3 C TEM 44 4-4 Fe TEM 46 4-5 5 4-6 5 5 51 6 5 1 1-1 1991 1,1 multiwall nanotube 1993 singlewall nanotube ( 1,) sp 7.4eV
More informationI-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
16 I ( ) (1) I-1 I-2 I-3 (2) I-1 ( ) (100 ) 2l x x = 0 y t y(x, t) y(±l, t) = 0 m T g y(x, t) l y(x, t) c = 2 y(x, t) c 2 2 y(x, t) = g (A) t 2 x 2 T/m (1) y 0 (x) y 0 (x) = g c 2 (l2 x 2 ) (B) (2) (1)
More information1 9 v.0.1 c (2016/10/07) Minoru Suzuki T µ 1 (7.108) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1)
1 9 v..1 c (216/1/7) Minoru Suzuki 1 1 9.1 9.1.1 T µ 1 (7.18) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1) E E µ = E f(e ) E µ (9.1) µ (9.2) µ 1 e β(e µ) 1 f(e )
More informationD:/BOOK/MAIN/MAIN.DVI
8 2 F (s) =L f(t) F (s) =L f(t) := Z 0 f()e ;s d (2.2) s s = + j! f(t) (f(0)=0 f(0) _ = 0 d n; f(0)=dt n; =0) L dn f(t) = s n F (s) (2.3) dt n Z t L 0 f()d = F (s) (2.4) s s =s f(t) L _ f(t) Z Z ;s L f(t)
More informationII ( ) (7/31) II ( [ (3.4)] Navier Stokes [ (6/29)] Navier Stokes 3 [ (6/19)] Re
II 29 7 29-7-27 ( ) (7/31) II (http://www.damp.tottori-u.ac.jp/~ooshida/edu/fluid/) [ (3.4)] Navier Stokes [ (6/29)] Navier Stokes 3 [ (6/19)] Reynolds [ (4.6), (45.8)] [ p.186] Navier Stokes I Euler Navier
More information23 1 Section ( ) ( ) ( 46 ) , 238( 235,238 U) 232( 232 Th) 40( 40 K, % ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4
23 1 Section 1.1 1 ( ) ( ) ( 46 ) 2 3 235, 238( 235,238 U) 232( 232 Th) 40( 40 K, 0.0118% ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4 2 ( )2 4( 4 He) 12 3 16 12 56( 56 Fe) 4 56( 56 Ni)
More information01_教職員.indd
T. A. H. A. K. A. R. I. K. O. S. O. Y. O. M. K. Y. K. G. K. R. S. A. S. M. S. R. S. M. S. I. S. T. S. K.T. R. T. R. T. S. T. S. T. A. T. A. D. T. N. N. N. Y. N. S. N. S. H. R. H. W. H. T. H. K. M. K. M.
More informationMott散乱によるParity対称性の破れを検証
Mott Parity P2 Mott target Mott Parity Parity Γ = 1 0 0 0 0 1 0 0 0 0 1 0 0 0 0 1 t P P ),,, ( 3 2 1 0 1 γ γ γ γ γ γ ν ν µ µ = = Γ 1 : : : Γ P P P P x x P ν ν µ µ vector axial vector ν ν µ µ γ γ Γ ν γ
More information2004
2008 3 20 400 1 1,222 7 1 2 3 55.8 54.8 3 35.8 6 64.0 50.5 93.5 1 1,222 1 1,428 1 1,077 6 64.0 52.5 80.5 56.6 81.5 30.2 1 2 3 7 70.5 1 65.6 2 61.3 3 51.1 1 54.0 2 49.8 3 32.0 68.8 37.0 34.3 2008 3 2 93.5
More informationAuerbach and Kotlikoff(1987) (1987) (1988) 4 (2004) 5 Diamond(1965) Auerbach and Kotlikoff(1987) 1 ( ) ,
,, 2010 8 24 2010 9 14 A B C A (B Negishi(1960) (C) ( 22 3 27 ) E-mail:fujii@econ.kobe-u.ac.jp E-mail:082e527e@stu.kobe-u.ac.jp E-mail:iritani@econ.kobe-u.ac.jp 1 1 1 2 3 Auerbach and Kotlikoff(1987) (1987)
More informationohpr.dvi
2003/12/04 TASK PAF A. Fukuyama et al., Comp. Phys. Rep. 4(1986) 137 A. Fukuyama et al., Nucl. Fusion 26(1986) 151 TASK/WM MHD ψ θ ϕ ψ θ e 1 = ψ, e 2 = θ, e 3 = ϕ ϕ E = E 1 e 1 + E 2 e 2 + E 3 e 3 J :
More information取扱説明書[N906i]
237 1 dt 2 238 1 i 1 p 2 1 ty 239 240 o p 1 i 2 1 u 1 i 2 241 1 p v 1 d d o p 242 1 o o 1 o 2 p 243 1 o 2 p 1 o 2 3 4 244 q p 245 p p 246 p 1 i 1 u c 2 o c o 3 o 247 1 i 1 u 2 co 1 1 248 1 o o 1 t 1 t
More information( )
7..-8..8.......................................................................... 4.................................... 3...................................... 3..3.................................. 4.3....................................
More information日本統計学会誌, 第44巻, 第2号, 251頁-270頁
44, 2, 205 3 25 270 Multiple Comparison Procedures for Checking Differences among Sequence of Normal Means with Ordered Restriction Tsunehisa Imada Lee and Spurrier (995) Lee and Spurrier (995) (204) (2006)
More informationhttp://www.ns.kogakuin.ac.jp/~ft13389/lecture/physics1a2b/ pdf I 1 1 1.1 ( ) 1. 30 m µm 2. 20 cm km 3. 10 m 2 cm 2 4. 5 cm 3 km 3 5. 1 6. 1 7. 1 1.2 ( ) 1. 1 m + 10 cm 2. 1 hr + 6400 sec 3. 3.0 10 5 kg
More informationH22環境地球化学4_化学平衡III_ ppt
1 2 3 2009年度 環境地球化学 大河内 温度上昇による炭酸水の発泡 気泡 温度が高くなると 溶けきれなくなった 二酸化炭素が気泡として出てくる 4 2009年度 環境地球化学 圧力上昇による炭酸水の発泡 栓を開けると 瓶の中の圧力が急激に 小さくなるので 発泡する 大河内 5 CO 2 K H CO 2 H 2 O K H + 1 HCO 3- K 2 H + CO 3 2- (M) [CO
More informationIV (2)
COMPUTATIONAL FLUID DYNAMICS (CFD) IV (2) The Analysis of Numerical Schemes (2) 11. Iterative methods for algebraic systems Reima Iwatsu, e-mail : iwatsu@cck.dendai.ac.jp Winter Semester 2007, Graduate
More information3-2 -
1 2-1 - 3-2 - 4 3-3 - Specific Absorption Rate 5 1 2 1 1-4 - - 5 - - 6 - - 7 - - 8 - - 9 - - 10 - - 11 - - 12 - 5-13 - / / / / / / / / / / - 14 - - 15 - - 16 - - 17 - - 18 - 2 2-19 - 3-20 - - 21 - 1 1
More information1/68 A. 電気所 ( 発電所, 変電所, 配電塔 ) における変圧器の空き容量一覧 平成 31 年 3 月 6 日現在 < 留意事項 > (1) 空容量は目安であり 系統接続の前には 接続検討のお申込みによる詳細検討が必要となります その結果 空容量が変更となる場合があります (2) 特に記載
1/68 A. 電気所 ( 発電所, 変電所, 配電塔 ) における変圧器の空き容量一覧 平成 31 年 3 月 6 日現在 < 留意事項 > (1) 空容量は目安であり 系統接続の前には 接続検討のお申込みによる詳細検討が必要となります その結果 空容量が変更となる場合があります (2) 特に記載のない限り 熱容量を考慮した空き容量を記載しております その他の要因 ( 電圧や系統安定度など ) で連系制約が発生する場合があります
More informationMOSFET HiSIM HiSIM2 1
MOSFET 2007 11 19 HiSIM HiSIM2 1 p/n Junction Shockley - - on-quasi-static - - - Y- HiSIM2 2 Wilson E f E c E g E v Bandgap: E g Fermi Level: E f HiSIM2 3 a Si 1s 2s 2p 3s 3p HiSIM2 4 Fermi-Dirac Distribution
More information総研大恒星進化概要.dvi
The Structure and Evolution of Stars I. Basic Equations. M r r =4πr2 ρ () P r = GM rρ. r 2 (2) r: M r : P and ρ: G: M r Lagrange r = M r 4πr 2 rho ( ) P = GM r M r 4πr. 4 (2 ) s(ρ, P ) s(ρ, P ) r L r T
More informationm dv = mg + kv2 dt m dv dt = mg k v v m dv dt = mg + kv2 α = mg k v = α 1 e rt 1 + e rt m dv dt = mg + kv2 dv mg + kv 2 = dt m dv α 2 + v 2 = k m dt d
m v = mg + kv m v = mg k v v m v = mg + kv α = mg k v = α e rt + e rt m v = mg + kv v mg + kv = m v α + v = k m v (v α (v + α = k m ˆ ( v α ˆ αk v = m v + α ln v α v + α = αk m t + C v α v + α = e αk m
More information(MRI) 10. (MRI) (MRI) : (NMR) ( 1 H) MRI ρ H (x,y,z) NMR (Nuclear Magnetic Resonance) spectrometry: NMR NMR s( B ) m m = µ 0 IA = γ J (1) γ: :Planck c
10. : (NMR) ( 1 H) MRI ρ H (x,y,z) NMR (Nuclear Magnetic Resonance) spectrometry: NMR NMR s( B ) m m = µ 0 IA = γ J (1) γ: :Planck constant J: Ĵ 2 = J(J +1),Ĵz = J J: (J = 1 2 for 1 H) I m A 173/197 10.1
More informationD v D F v/d F v D F η v D (3.2) (a) F=0 (b) v=const. D F v Newtonian fluid σ ė σ = ηė (2.2) ė kl σ ij = D ijkl ė kl D ijkl (2.14) ė ij (3.3) µ η visco
post glacial rebound 3.1 Viscosity and Newtonian fluid f i = kx i σ ij e kl ideal fluid (1.9) irreversible process e ij u k strain rate tensor (3.1) v i u i / t e ij v F 23 D v D F v/d F v D F η v D (3.2)
More informationQMI_10.dvi
... black body radiation black body black body radiation Gustav Kirchhoff 859 895 W. Wien O.R. Lummer cavity radiation ν ν +dν f T (ν) f T (ν)dν = 8πν2 c 3 kt dν (Rayleigh Jeans) (.) f T (ν) spectral energy
More informationLCR e ix LC AM m k x m x x > 0 x < 0 F x > 0 x < 0 F = k x (k > 0) k x = x(t)
338 7 7.3 LCR 2.4.3 e ix LC AM 7.3.1 7.3.1.1 m k x m x x > 0 x < 0 F x > 0 x < 0 F = k x k > 0 k 5.3.1.1 x = xt 7.3 339 m 2 x t 2 = k x 2 x t 2 = ω 2 0 x ω0 = k m ω 0 1.4.4.3 2 +α 14.9.3.1 5.3.2.1 2 x
More informationI ( ) 2019
I ( ) 2019 i 1 I,, III,, 1,,,, III,,,, (1 ) (,,, ), :...,, : NHK... NHK, (YouTube ),!!, manaba http://pen.envr.tsukuba.ac.jp/lec/physics/,, Richard Feynman Lectures on Physics Addison-Wesley,,,, x χ,
More information吸収分光.PDF
3 Rb 1 1 4 1.1 4 1. 4 5.1 5. 5 3 8 3.1 8 4 1 4.1 External Cavity Laser Diode: ECLD 1 4. 1 4.3 Polarization Beam Splitter: PBS 13 4.4 Photo Diode: PD 13 4.5 13 4.6 13 5 Rb 14 6 15 6.1 ECLD 15 6. 15 6.3
More information閨75, 縺5 [ ィ チ573, 縺 ィ ィ
39ィ 8 998 3. 753 68, 7 86 タ7 9 9989769 438 縺48 縺55 3783645 タ5 縺473 タ7996495 ィ 59754 8554473 9 8984473 3553 7. 95457357, 4.3. 639745 5883597547 6755887 67996499 ィ 597545 4953473 9 857473 3553, 536583, 89573,
More information¼§À�ÍýÏÀ – Ê×ÎòÅŻҼ§À�¤È¥¹¥Ô¥ó¤æ¤é¤®
email: takahash@sci.u-hyogo.ac.jp Spring semester, 2012 Outline 1. 2 / 26 Introduction : (d ) : 4f 1970 ZrZn 2, MnSi, Ni 3 Al, Sc 3 In Stoner-Wohlfarth Moriya-Kawabata (1973) 3 / 26 Properties of Weak
More informationOHP.dvi
t 0, X X t x t 0 t u u = x X (1) t t 0 u X x O 1 1 t 0 =0 X X +dx t x(x,t) x(x +dx,t). dx dx = x(x +dx,t) x(x,t) (2) dx, dx = F dx (3). F (deformation gradient tensor) t F t 0 dx dx X x O 2 2 F. (det F
More information...3 1-1...3 1-1...6 1-3...16 2....17...21 3-1...21 3-2...21 3-2...22 3-3...23 3-4...24...25 4-1....25 4-2...27 4-3...28 4-4...33 4-5...36...37 5-1...
DT-870/5100 &DT-5042RFB ...3 1-1...3 1-1...6 1-3...16 2....17...21 3-1...21 3-2...21 3-2...22 3-3...23 3-4...24...25 4-1....25 4-2...27 4-3...28 4-4...33 4-5...36...37 5-1....39 5-2...40 5-3...43...49
More information[1.1] r 1 =10e j(ωt+π/4), r 2 =5e j(ωt+π/3), r 3 =3e j(ωt+π/6) ~r = ~r 1 + ~r 2 + ~r 3 = re j(ωt+φ) =(10e π 4 j +5e π 3 j +3e π 6 j )e jωt
3.4.7 [.] =e j(t+/4), =5e j(t+/3), 3 =3e j(t+/6) ~ = ~ + ~ + ~ 3 = e j(t+φ) =(e 4 j +5e 3 j +3e 6 j )e jt = e jφ e jt cos φ =cos 4 +5cos 3 +3cos 6 =.69 sin φ =sin 4 +5sin 3 +3sin 6 =.9 =.69 +.9 =7.74 [.]
More information(2004 ) 2 (A) (B) (C) 3 (1987) (1988) Shimono and Tachibanaki(1985) (2008) , % 2 (1999) (2005) 3 (2005) (2006) (2008)
,, 23 4 30 (i) (ii) (i) (ii) Negishi (1960) 2010 (2010) ( ) ( ) (2010) E-mail:fujii@econ.kobe-u.ac.jp E-mail:082e527e@stu.kobe-u.ac.jp E-mail:iritani@econ.kobe-u.ac.jp 1 1 16 (2004 ) 2 (A) (B) (C) 3 (1987)
More informationK 1 mk(
R&D ATN K 1 mk(0.01 0.05 = ( ) (ITS-90)-59.3467 961.78 (T.J.Seebeck) A(+ T 1 I T 0 B - T 1 T 0 E (Thermoelectromotive force) AB =d E(AB) /dt=a+bt----------------- E(AB) T1 = = + + E( AB) α AB a b ( T0
More informationsyuryoku
248 24622 24 P.5 EX P.212 2 P271 5. P.534 P.690 P.690 P.690 P.690 P.691 P.691 P.691 P.702 P.702 P.702 P.702 1S 30% 3 1S 3% 1S 30% 3 1S 3% P.702 P.702 P.702 P.702 45 60 P.702 P.702 P.704 H17.12.22 H22.4.1
More information土壌環境行政の最新動向(環境省 水・大気環境局土壌環境課)
201022 1 18801970 19101970 19201960 1970-2 1975 1980 1986 1991 1994 3 1999 20022009 4 5 () () () () ( ( ) () 6 7 Ex Ex Ex 8 25 9 10 11 16619 123 12 13 14 5 18() 15 187 1811 16 17 3,000 2241 18 19 ( 50
More information200201690 2005 11 56 36) 21 200 alternative methods The Encyclopedia of Bodywork1996 300 1-2-1 1 2 1-1-2 0.2 0.2 3 1-3-1 4 5 7 3 m 6 (yoga) 1970 19141998 7 8 3 3 9 T 1 10 4 9 / 3 6 6 6 7 6 10 8 100h
More informationi 18 2H 2 + O 2 2H 2 + ( ) 3K
i 18 2H 2 + O 2 2H 2 + ( ) 3K ii 1 1 1.1.................................. 1 1.2........................................ 3 1.3......................................... 3 1.4....................................
More informationスライド 1
Matsuura Laboratory SiC SiC 13 2004 10 21 22 H-SiC ( C-SiC HOY Matsuura Laboratory n E C E D ( E F E T Matsuura Laboratory Matsuura Laboratory DLTS Osaka Electro-Communication University Unoped n 3C-SiC
More information4/15 No.
4/15 No. 1 4/15 No. 4/15 No. 3 Particle of mass m moving in a potential V(r) V(r) m i ψ t = m ψ(r,t)+v(r)ψ(r,t) ψ(r,t) = ϕ(r)e iωt ψ(r,t) Wave function steady state m ϕ(r)+v(r)ϕ(r) = εϕ(r) Eigenvalue problem
More informationslide1.dvi
1. 2/ 121 a x = a t 3/ 121 a x = a t 4/ 121 a > 0 t a t = a t t {}}{ a a a t 5/ 121 a t+s = = t+s {}}{ a a a t s {}}{{}}{ a a a a = a t a s (a t ) s = s {}}{ a t a t = a ts 6/ 121 a > 0 t a 0 t t = 0 +
More informationH22応用物理化学演習1_濃度.ppt
1 2 4/12 4/19 4/27 5/10 5/17 5/24 5/31 (20 ) (20 ) (10 ) (50 ) 3 (mole fraction) X = (mol) (mol) i n 1, n 2,, n x N i X i = n i = n i n 1 + n 2 + + n x N 4 (molarity, M) 1 dm 3 ( L) (mol) (mol/l) = 1 L
More informationNetcommunity SYSTEM X7000 IPコードレス電話機 取扱説明書
4 5 6 7 8 9 . 4 DS 0 4 5 4 4 4 5 5 6 7 8 9 0 4 5 6 7 8 9 4 5 6 4 0 4 4 4 4 5 6 7 8 9 40 4 4 4 4 44 45 4 6 7 5 46 47 4 5 6 48 49 50 5 4 5 4 5 6 5 5 6 4 54 4 5 6 7 55 5 6 4 56 4 5 6 57 4 5 6 7 58 4
More information.A. D.S
1999-1- .A. D.S 1996 2001 1999-2- -3- 1 p.16 17 18 19 2-4- 1-5- 1~2 1~2 2 5 1 34 2 10 3 2.6 2.85 3.05 2.9 2.9 3.16 4 7 9 9 17 9 25 10 3 10 8 10 17 10 18 10 22 11 29-6- 1 p.1-7- p.5-8- p.9 10 12 13-9- 2
More information1 No.1 5 C 1 I III F 1 F 2 F 1 F 2 2 Φ 2 (t) = Φ 1 (t) Φ 1 (t t). = Φ 1(t) t = ( 1.5e 0.5t 2.4e 4t 2e 10t ) τ < 0 t > τ Φ 2 (t) < 0 lim t Φ 2 (t) = 0
1 No.1 5 C 1 I III F 1 F 2 F 1 F 2 2 Φ 2 (t) = Φ 1 (t) Φ 1 (t t). = Φ 1(t) t = ( 1.5e 0.5t 2.4e 4t 2e 10t ) τ < 0 t > τ Φ 2 (t) < 0 lim t Φ 2 (t) = 0 0 < t < τ I II 0 No.2 2 C x y x y > 0 x 0 x > b a dx
More informationPowerPoint Presentation
2010 KEK (Japan) (Japan) (Japan) Cheoun, Myun -ki Soongsil (Korea) Ryu,, Chung-Yoe Soongsil (Korea) 1. S.Reddy, M.Prakash and J.M. Lattimer, P.R.D58 #013009 (1998) Magnetar : ~ 10 15 G ~ 10 17 19 G (?)
More information4‐E ) キュリー温度を利用した消磁:熱消磁
( ) () x C x = T T c T T c 4D ) ) Fe Ni Fe Fe Ni (Fe Fe Fe Fe Fe 462 Fe76 Ni36 4E ) ) (Fe) 463 4F ) ) ( ) Fe HeNe 17 Fe Fe Fe HeNe 464 Ni Ni Ni HeNe 465 466 (2) Al PtO 2 (liq) 467 4G ) Al 468 Al ( 468
More information8 8 0
,07,,08, 8 8 0 7 8 7 8 0 0 km 7 80. 78. 00 0 8 70 8 0 8 0 8 7 8 0 0 7 0 0 7 8 0 00 0 0 7 8 7 0 0 8 0 8 7 7 7 0 j 8 80 j 7 8 8 0 0 0 8 8 8 7 0 7 7 0 8 7 7 8 7 7 80 77 7 0 0 0 7 7 0 0 0 7 0 7 8 0 8 8 7
More informationレジャー産業と顧客満足の課題
1 1983 1983 2 3700 4800 5500 3300 15 3 100 1000 JR 4 14 2000 55% 72% 1878 2000 5 ( ) 22 1,040 5 946 42 15 25 30 30 4 14 39 1 24 8 6 390 33 800 34 34 3 35 () 37 40 1 50 40 46 47 2 55 4.43 4 16.98 40 55
More informationPart () () Γ Part ,
Contents a 6 6 6 6 6 6 6 7 7. 8.. 8.. 8.3. 8 Part. 9. 9.. 9.. 3. 3.. 3.. 3 4. 5 4.. 5 4.. 9 4.3. 3 Part. 6 5. () 6 5.. () 7 5.. 9 5.3. Γ 3 6. 3 6.. 3 6.. 3 6.3. 33 Part 3. 34 7. 34 7.. 34 7.. 34 8. 35
More informationK E N Z OU
K E N Z OU 11 1 1 1.1..................................... 1.1.1............................ 1.1..................................................................................... 4 1.........................................
More information1 発病のとき
A A 1944 19 60 A 1 A 20 40 2 A 4 A A 23 6 A A 13 10 100 2 2 360 A 19 2 5 A A A A A TS TS A A A 194823 6 A A 23 A 361 A 3 2 4 2 16 9 A 7 18 A A 16 4 16 3 362 A A 6 A 6 4 A A 363 A 1 A A 1 A A 364 A 1 A
More information2 3 1 2 Fig.2.1. 2V 2.3.3
2 2 2.1 2000 1800 1 2.2 1 2 2.3 2.3.1 1 1 2 2.3.2 2 3 1 2 Fig.2.1. 2V 2.3.3 2 4 2.3.4 2 C CmAh = ImA th (2.1) 1000mAh 1A 1 2 1C C (Capacity) 1 3Ah 3A Rrate CAh = IA (2.2) 2.3.5 *1 2 2 2.3.6 2 2 *1 10 2
More information2014_VERAum.pptx
VERA+NRO45m VLBI Mapping of SiO v=2/v=3 J=1 0 Masers using modified coordinate of NRO45m September 24, 2014 Miyako Oyadomari Kagoshima University 12 th Mizusawa VLBI Observatory User s Meeting @MITAKA
More information平成19年度
1 2 3 4 H 3 H CC N + 3 O H 3 C O CO CH 3 CH O CO O CH2 CH 3 P O O 5 H H H CHOH H H H N + CHOH CHOH N + CH CH COO- CHOH CH CHOH 6 1) 7 2 ) 8 3 ) 4 ) 9 10 11 12 13 14 15 16 17 18 19 20 A A 0 21 ) exp( )
More informationProducts catalog
2016 商品カタログ 低圧進相用フィルムコンデンサ % kvar 90 (b) % (c) (a) (kvar) (KVA) 220 V 100 kw 100 kw =7 % =99 % 100 ( % 130 ) 7 kvar 88 7=13 133 kw 88 kvar 101 kva 13 kvar kw kw ~ 100 kw 100 kw ~ 0 kw 0 kw ~ 2000 kw 2000
More information1 1 1 11 25 2 28 2 2 6 10 8 30 4 26 1 38 5 1 2 25 57ha 25 3 24ha 3 4 83km2 15cm 5 8ha 30km2 8ha 30km2 4 14
3 9 11 25 1 2 2 3 3 6 7 1 2 4 2 1 1 1 11 25 2 28 2 2 6 10 8 30 4 26 1 38 5 1 2 25 57ha 25 3 24ha 3 4 83km2 15cm 5 8ha 30km2 8ha 30km2 4 14 60 m3 60 m3 4 1 11 26 30 2 3 15 50 2 1 4 7 110 2 4 21 180 1 38
More information09_organal2
4. (1) (a) I = 1/2 (I = 1/2) I 0 p ( ), n () I = 0 (p + n) I = (1/2, 3/2, 5/2 ) p ( ), n () I = (1, 2, 3 ) (b) (m) (I = 1/2) m = +1/2, 1/2 (I = 1/2) m = +1/2, 1/2 I m = +I, +(I 1), +(I 2) (I 1), I ( )
More information縺 縺8 縺, [ 縺 チ : () () () 4 チ93799; () "64": ィャ 9997ィ
34978 998 3. 73 68, 86 タ7 9 9989769 438 縺48 縺 378364 タ 縺473 399-4 8 637744739 683 6744939 3.9. 378,.. 68 ィ 349 889 3349947 89893 683447 4 334999897447 (9489) 67449, 6377447 683, 74984 7849799 34789 83747
More information読めば必ずわかる 分散分析の基礎 第2版
2 2003 12 5 ( ) ( ) 2 I 3 1 3 2 2? 6 3 11 4? 12 II 14 5 15 6 16 7 17 8 19 9 21 10 22 11 F 25 12 : 1 26 3 I 1 17 11 x 1, x 2,, x n x( ) x = 1 n n i=1 x i 12 (SD ) x 1, x 2,, x n s 2 s 2 = 1 n n (x i x)
More informationjse2000.dvi
pn 1 2 1 1947 1 (800MHz) (12GHz) (CPUDSP ) 1: MOS (MOSFET) CCD MOSFET MES (MESFET) (HBT) (HEMT) GTO MOSFET (IGBT) (SIT) pn { 3 3 3 pn 2 pn pn 1 2 sirafuji@dj.kit.ac.jp yoshimot@dj.kit.ac.jp 1 3 3.1 III
More information1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Stru
1. 1-1. 1-. 1-3.. MD -1. -. -3. MD 1 1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Structural relaxation
More informationkm2 km2 km2 km2 km2 22 4 H20 H20 H21 H20 (H22) (H22) (H22) L=600m L=430m 1 H14.04.12 () 1.6km 2 H.14.05.31 () 3km 3 4 5 H.15.03.18 () 3km H.15.06.20 () 1.1km H.15.06.30 () 800m 6 H.15.07.18
More information