A. Fresnel) (M. Planck) 1905 (A. Einstein) X (A. Ampère) (M. Faraday) 1864 (C. Maxwell) 1871 (H. R. Hertz) (G. Galilei)

Size: px
Start display at page:

Download "A. Fresnel) 19 1900 (M. Planck) 1905 (A. Einstein) X (A. Ampère) (M. Faraday) 1864 (C. Maxwell) 1871 (H. R. Hertz) 1888 2.2 1 7 (G. Galilei) 1638 2"

Transcription

1 tatekawa (at) akane.waseda.jp x t x t (I. Newton) C. Huygens) 19 (T. Young) 1

2 A. Fresnel) (M. Planck) 1905 (A. Einstein) X (A. Ampère) (M. Faraday) 1864 (C. Maxwell) 1871 (H. R. Hertz) (G. Galilei)

3 1: (O. Roemer) (Io) [m/s] (J. Bladley) v c θ = v c, (1) 3

4 2: L 3: 1 c = [m/s] (2) (A. Fizeau) L = [km]) 1 sin θ θ 4

5 c = 2L t = = [m/s]. (3) (J. L. Foucault) 1862 c = (2.980 ± 0.5) 10 8 [m/s], (4) [µm] (Cd) Kr

6 (J. Harrison) ( 133 Cs) c = [m/s]. (5) 1 1/ (J. L. Lagrange) (W. R. Hamilton) (L. E. Boltzmann)

7 S V u V v 4: S, S S S V 19 4[km/h] 40[km/h] 44[km/h] 4 S, S S S V S u S v = u + V c c 7

8 v = 30[km/s] β = v c 10 4, 10 4 (A. Michelson) L 1 c c v c + v t (1) = L 1 c v + L 1 c + v = 2L 1 1 c 1 β 2, (6) 8 c 2 v β = v/c 8

9 L 2 L 1 5: t (2) = 2L 2 1 c, (7) 1 β 2 (0 ) = t (1) t (2), (8) 90 t (2) = 2L 2 c 1 1 β 2, (9) t (1) = 2L 1 1 c, (10) 1 β 2 9

10 (90 ) = t (2) t (1), (11) t(0 ) t(90 ) = t (1) + t (1) = 2(L 1 + L 2 ) c t(2) t (2) ( ) 1 1 β 2 1, (12) 1 β 2 β 1 9 L 1 = L 2 = L t(0 ) t(90 ) 2L c β2, (13) λ s s = 1 λ c ( t(0 ) t(90 )) 2L λ β2, (14) L = 1.2[m], λ = [m], s = 0.04 (E. Morley) 1887 L = 11[m] s 0.4 s < 0.01 G. F. FitzGerald) (H. A. Lorentz) 9 (1 β 2 ) a 1 aβ 2 10

11 ma = F, (15) r = r vt, (16) v ma = F, (17) % 20% 70% 11

12 (event) P Q x P, x Q d d 2 = (x Q x P ) 2, (18) P, Q s 2 P Q c 2 (t Q t P ) 2 + (x Q x P ) 2. (19) 12

13 (19) (Minkowski) P Q ( s) 2 = c 2 ( t) 2 + ( x) 2, (20) 12 PQ x Q x P = c(t Q t P ), (21) s 2 P Q = 0, (22) (s P Q) 2 = c 2 ( t Q t P ) 2 + ( x Q x P ) 2 = 0, (23) P Q 2 2 S P, Q (t p, x p ) (t q, x q ) 12 13

14 s 2 P Q c 2 (t Q t P ) 2 + (x Q x P ) 2. (24) S P Q (s P Q) 2 = c 2 (t Q t P ) 2 < 0 (25) s 2 P Q = (s P Q) 2 < 0, (26) 1 2 c (x Q x P ) 2 = { tq t P } 2 { tq } 2 v(t) dt < c dt = c 2 (t Q t P ) 2, (27) t P S P, Q (T p, X p ) (T q, X q ) s 2 P Q c 2 (T Q T P ) 2 + (X Q X P ) 2. (28) S P Q (s P Q) 2 = (X Q X P ) 2 > 0 (29) s 2 P Q = (s P Q) 2 > 0, (30) 14

15 ct O y x 6: (31) x ct t = 0, x = 0 O P x 2 > c 2 t 2 Q x 2 < c 2 t 2 c 2 t 2 + x 2 = 0, x y c 2 t 2 = x 2 = x 2 + y 2, (31) t (31) 6 ct O ct O O 15

16 3.4 t r = ( x) 2 + ( y) 2 + ( z) 2, S S x = y = z = 0, (32) ( s) 2 = c 2 ( t) 2 + ( r) 2 = c 2 ( t ) 2, (33) t = t 1 1 c 2 ( r t ) 2 = t v = r t, v = v, 1 v2 c 2, (34) (34)

17 τ2 τ 1 dt = t2 t 1 dt 1 v(t)2 c 2. (35) v S τ 2 τ 1 ( τ) 2 ( s)2 c 2, (36) 3.5 S(t, x, y, z) S (t, x, y, z ) S S x v t = t, x = x vt, y = y, z = z, (37) ( s) 2 = c 2 ( t) 2 + ( x) 2 + ( y) 2 + ( z) 2, (38) ( s ) 2 = (c 2 v 2 )( t) 2 2v( t)( x) + ( x) 2 + ( y) 2 + ( z) 2, (39) β = v/c

18 ct x y z = a 00 a 01 a 02 a 03 a 10 a 11 a 12 a 13 a 20 a 21 a 22 a 23 a 30 a 31 a 32 a 33 ct x y z. (40) 4 4 S S x v t = t = 0 S S y = y, z = z, (41) a 22 = a 33 = 1, (42) a 20 = a 21 = a 23 = a 30 = a 31 = a 32 = 0, (43) y = y, z = z a 02 = a 03 = a 12 = a 13 = 0, (44) ct = a 00 ct + a 01 x, (45) x = a 10 ct + a 11 x, (46) y = y, (47) z = z, (48) S x = 0 S x v x = vt, (49) 18

19 (45) (46) ct = a 00 ct, x = a 10 ct, (50) a 10 ct = a 00 vt, (51) a 10 a 00 = v c, (52) S x = 0 S x v x = vt, (53) (46) a 10 ct + a 11 x = 0, (54) a 10 a 11 = v c, (55) (52) (55) a 00 = a 11, (56) γ a 00 = a t = t = 0 x S x = ct, (57) (45) (46) ct = (a 00 + a 01 )ct, (58) x = (a 10 + a 11 )x, (59) S x = ct, (60) a 00 + a 01 = a 10 + a 11, (61) 19

20 a 01 = a 10 (52) a 01 = a 10 = v c γ, (62) γ ct = γ (ct v ) c x, (63) x = γ ( vt + x), (64) γ S S S S (63) (64) ct = x = 1 v/c γ[1 (v/c) 2 ] ct + γ[1 (v/c) 2 ] x, (65) v/c 1 γ[1 (v/c) 2 ] ct + γ[1 (v/c) 2 ] x, (66) S S v v ( ct = γ ct + v c x ), (67) x = γ (vt + x ), (68) γ = 1 1 (v/c) 2, (69) 14 β = v/c 0 (63) (64) γ 1 (63) ct = ct t = t, (70) (64) x = vt + x, (71) 14 γ γ 20

21 y V V v x 7: S S V x S v S v c S S V x S v S v 7 v v x = γ( x + V t ), (72) y = y, (73) z = z, (74) t = γ ( t + Vc ) 2 x, (75) v x = x t = γ( x + V t ) γ ( t + V c x ) = V + v x 1 + V, (76) 2 c v 2 x v y = y t = v z = z t = v y γ ( ) 1 + V, (77) c v 2 x v z γ ( ) 1 + V, (78) c v 2 x V < c, v < c v < c 21

22 y v V x 8: S S V x S v S v c γ 1 v x = V + v x, v y = v y, v z = v z, S S 8 x x θ θ v x = v cos θ, v y = v sin θ, (79) v x = v cos θ, v y = v sin θ, (80) v x = v cos θ = x t = V + v cos θ 1 + V c 2 v cos θ, (81) v y = v sin θ = y t = v sin θ γ ( 1 + V c v cos θ ), (82) 2 22

23 : θ θ θ = 0 θ = 180 θ θ θ θ tan θ = v sin θ γ(v + v cos θ ), (83) v = v = c, tan θ = sin θ γ(β + cos θ ), (84) θ θ 9 θ θ β = 0 90 β = β = S S S 23

24 15 SF S S x = 0 t 10 S t = t 2 t 1, (85) S S v S t = t 2 t 1 = γ (t 2 + v c 2 t 1 v ) c 2 = γ(t 2 t 1) = γ t > t, (86) S S S x 11 S l = x = x 2 x 1, (87) 15 24

25 S V t 10: t t S V 11: x S t S 16 x = x 2 x 1 = γ(x 2 x 1 ) = γ x, (88) δx = 1 γ l < l, (89)

26 (ct) (x) S S x ct = 0 ct = 0 S ct = v c x, tan θ = v c, S ct x = 0 x = 0 S x = v ct = vt, c 12 S x = 0 ct P 12 ct x ct B A 26

27 ct B A P O x 12: S S B S (ct, 0) S (ct, x B ) { ct = γ 0 = γ ( ct v ( c v c { ) } x B ) ct + x B, (90) }, (91) x B T T T = 1 γ T < T, (92) S S (a) 27

28 (a) (b) 13: (a) (b) (b) S S (x = 0) t = 0 t = 0 x = 0 14 t = 0 x = 0 Q P R 28

29 ct Q R P x 14: Q P R

30 ct B A O x 15: x = 0 ct ct A ct B 15 S ct A S ct A S ct B 0 τ A 30

31 2τ A τ A 15 A 15 A A A i m x 2v 2m x 31

32 m 2m m 2m 2v v 16: m x 2v 2m x v 2m m 3v v v m 2v + 2m ( v) = 0, (93) 0 v = v + 2v 1 (v 2v/c 2 ) = 3v 1 (2v 2 /c 2 ), (94) mv 2 3mṽ v ṽ = v ṽ = v 1 (2v 2 /c 2 ) v, (95) 32

33 4.2 x v t t x v = x t, (96) x t t x τ s ( s) 2 = c 2 ( τ) 2 = c 2 ( t) 2 + ( x) 2 { ( x = c 2 + t = c 2 {1 )} ( t) 2 ( v c ) 2 } ( t) 2, (97) t x ct x, y, z ct u t (ct) τ u x x τ,, (98) u y y τ, u z z τ. (99)

34 4 u 4 4 p t mu t, (100) p x mu x, p y mu y, p z mu z, (101) v v v = v, v 2 = v = v 2 x + v 2 y + v 2 z, (102) v 4 0 ( ) 2 (ct) (u t ) 2 + (u x ) 2 + (u y ) 2 + (u z ) 2 = + τ = = ( ) 2 x + τ ( ) 2 y + τ ( ) 2 z τ 1 { ( τ) 2 ( (ct)) 2 + ( x) 2 + ( y) 2 + ( z) 2} 1 ( τ) ( (p t ) 2 + (p x ) 2 + (p y ) 2 + (p z ) 2 = m (ct) τ = = { c 2 ( τ) 2} = c 2, (103) ) 2 ( + m x ) 2 ( + m y ) 2 ( + m z ) 2 τ τ τ 1 { m 2 ( τ) 2 ( (ct)) 2 + ( x) 2 + ( y) 2 + ( z) 2} 1 m 2 ( τ) 2 { c 2 ( τ) 2} = (mc) 2, (104) 4 v p t = mu t = m (ct) τ p x = mu x = m x τ = m t τ = mc t = γmc, τ (105) x t = γmv x, (106) 34

35 p y = mu y = m y τ = m t y τ p z = mu z = m z τ = m t τ γ = 1 ( v c ) 2 ( = t τ t = γmv y, (107) z t = γmv z, (108) ), (109) m γm, (110) 4 1 p x = m v x, (111) m m 19 m v c c cp t = γmc 2. (112) γ (109) β = v/c 1 Taylor (1 + ε) (1 + ε) 2 = 1 + 2ε + ε 2, (113) (1 + ε) 3 = 1 + 3ε + 3ε 2 + ε 3, (114) (1 + ε) 4 = 1 + 4ε + 6ε 2 + 4ε 3 + ε 4, (115) ε 19 m 0 35

36 ε n ε n ε (1 + ε) n 1 + nε, (116) n (116) n ε = (1 + ε) 1/ ε, (117) (109) ( v ) 2 1 ( v ) ( 2 ( v ) ) 2 1 1, ε =, (118) c 2 c c 4 0 (112) cp t ( 1 1 ( v ) ) 2 mc 2, (119) 2 c cp t mc mv2, (120) v 0 0 E 0 = mc 2, (121) 21 E cp t, (122) m 36

37 5 E = mc 2, (123) 1km 1km 1km 1km 5000km 5000km 5000km 5000km 37

38 , 5. ( ) 6. J.J

168 13 Maxwell ( H ds = C S rot H = j + D j + D ) ds (13.5) (13.6) Maxwell Ampère-Maxwell (3) Gauss S B 0 B ds = 0 (13.7) S div B = 0 (13.8) (4) Farad

168 13 Maxwell ( H ds = C S rot H = j + D j + D ) ds (13.5) (13.6) Maxwell Ampère-Maxwell (3) Gauss S B 0 B ds = 0 (13.7) S div B = 0 (13.8) (4) Farad 13 Maxwell Maxwell Ampère Maxwell 13.1 Maxwell Maxwell E D H B ε 0 µ 0 (1) Gauss D = ε 0 E (13.1) B = µ 0 H. (13.2) S D = εe S S D ds = ρ(r)dr (13.3) S V div D = ρ (13.4) ρ S V Coulomb (2) Ampère C H =

More information

一般演題(ポスター)

一般演題(ポスター) 6 5 13 : 00 14 : 00 A μ 13 : 00 14 : 00 A β β β 13 : 00 14 : 00 A 13 : 00 14 : 00 A 13 : 00 14 : 00 A β 13 : 00 14 : 00 A β 13 : 00 14 : 00 A 13 : 00 14 : 00 A β 13 : 00 14 : 00 A 13 : 00 14 : 00 A

More information

467 468 469 470 471 472 473 474 475 476 477 478 479 480 481 482 483 484 485 486 487 488 489 490 B =(1+R ) B +G τ C C G τ R B C = a R +a W W ρ W =(1+R ) B +(1+R +δ ) (1 ρ) L B L δ B = λ B + μ (W C λ B )

More information

24.15章.微分方程式

24.15章.微分方程式 m d y dt = F m d y = mg dt V y = dy dt d y dt = d dy dt dt = dv y dt dv y dt = g dv y dt = g dt dt dv y = g dt V y ( t) = gt + C V y ( ) = V y ( ) = C = V y t ( ) = gt V y ( t) = dy dt = gt dy = g t dt

More information

0.,,., m Euclid m m. 2.., M., M R 2 ψ. ψ,, R 2 M.,, (x 1 (),, x m ()) R m. 2 M, R f. M (x 1,, x m ), f (x 1,, x m ) f(x 1,, x m ). f ( ). x i : M R.,,

0.,,., m Euclid m m. 2.., M., M R 2 ψ. ψ,, R 2 M.,, (x 1 (),, x m ()) R m. 2 M, R f. M (x 1,, x m ), f (x 1,, x m ) f(x 1,, x m ). f ( ). x i : M R.,, 2012 10 13 1,,,.,,.,.,,. 2?.,,. 1,, 1. (θ, φ), θ, φ (0, π),, (0, 2π). 1 0.,,., m Euclid m m. 2.., M., M R 2 ψ. ψ,, R 2 M.,, (x 1 (),, x m ()) R m. 2 M, R f. M (x 1,, x m ), f (x 1,, x m ) f(x 1,, x m ).

More information

チュートリアル:ノンパラメトリックベイズ

チュートリアル:ノンパラメトリックベイズ { x,x, L, xn} 2 p( θ, θ, θ, θ, θ, } { 2 3 4 5 θ6 p( p( { x,x, L, N} 2 x { θ, θ2, θ3, θ4, θ5, θ6} K n p( θ θ n N n θ x N + { x,x, L, N} 2 x { θ, θ2, θ3, θ4, θ5, θ6} log p( 6 n logθ F 6 log p( + λ θ F θ

More information

II

II II 28 5 31 3 I 7 1 9 1.1.......................... 9 1.1.1 ( )................ 9 1.1.2........................ 14 1.1.3................... 15 1.1.4 ( )................. 16 1.1.5................... 17

More information

85 4

85 4 85 4 86 Copright c 005 Kumanekosha 4.1 ( ) ( t ) t, t 4.1.1 t Step! (Step 1) (, 0) (Step ) ±V t (, t) I Check! P P V t π 54 t = 0 + V (, t) π θ : = θ : π ) θ = π ± sin ± cos t = 0 (, 0) = sin π V + t +V

More information

C:/KENAR/0p1.dvi

C:/KENAR/0p1.dvi 2{3. 53 2{3 [ ] 4 2 1 2 10,15 m 10,10 m 2 2 54 2 III 1{I U 2.4 U r (2.16 F U F =, du dt du dr > 0 du dr < 0 O r 0 r 2.4: 1 m =1:00 10 kg 1:20 10 kgf 8:0 kgf g =9:8 m=s 2 (a) x N mg 2.5: N 2{3. 55 (b) x

More information

K E N Z U 01 7 16 HP M. 1 1 4 1.1 3.......................... 4 1.................................... 4 1..1..................................... 4 1...................................... 5................................

More information

5 36 5................................................... 36 5................................................... 36 5.3..............................

5 36 5................................................... 36 5................................................... 36 5.3.............................. 9 8 3............................................. 3.......................................... 4.3............................................ 4 5 3 6 3..................................................

More information

1.1 ft t 2 ft = t 2 ft+ t = t+ t 2 1.1 d t 2 t + t 2 t 2 = lim t 0 t = lim t 0 = lim t 0 t 2 + 2t t + t 2 t 2 t + t 2 t 2t t + t 2 t 2t + t = lim t 0

1.1 ft t 2 ft = t 2 ft+ t = t+ t 2 1.1 d t 2 t + t 2 t 2 = lim t 0 t = lim t 0 = lim t 0 t 2 + 2t t + t 2 t 2 t + t 2 t 2t t + t 2 t 2t + t = lim t 0 A c 2008 by Kuniaki Nakamitsu 1 1.1 t 2 sin t, cos t t ft t t vt t xt t + t xt + t xt + t xt t vt = xt + t xt t t t vt xt + t xt vt = lim t 0 t lim t 0 t 0 vt = dxt ft dft dft ft + t ft = lim t 0 t 1.1

More information

Einstein 1905 Lorentz Maxwell c E p E 2 (pc) 2 = m 2 c 4 (7.1) m E ( ) E p µ =(p 0,p 1,p 2,p 3 )=(p 0, p )= c, p (7.2) x µ =(x 0,x 1,x 2,x

Einstein 1905 Lorentz Maxwell c E p E 2 (pc) 2 = m 2 c 4 (7.1) m E ( ) E p µ =(p 0,p 1,p 2,p 3 )=(p 0, p )= c, p (7.2) x µ =(x 0,x 1,x 2,x 7 7.1 7.1.1 Einstein 1905 Lorentz Maxwell c E p E 2 (pc) 2 = m 2 c 4 (7.1) m E ( ) E p µ =(p 0,p 1,p 2,p 3 )=(p 0, p )= c, p (7.2) x µ =(x 0,x 1,x 2,x 3 )=(x 0, x )=(ct, x ) (7.3) E/c ct K = E mc 2 (7.4)

More information

1 3 1.1.......................... 3 1............................... 3 1.3....................... 5 1.4.......................... 6 1.5........................ 7 8.1......................... 8..............................

More information

第89回日本感染症学会学術講演会後抄録(I)

第89回日本感染症学会学術講演会後抄録(I) ! ! ! β !!!!!!!!!!! !!! !!! μ! μ! !!! β! β !! β! β β μ! μ! μ! μ! β β β β β β μ! μ! μ!! β ! β ! ! β β ! !! ! !!! ! ! ! β! !!!!! !! !!!!!!!!! μ! β !!!! β β! !!!!!!!!! !! β β β β β β β β !!

More information

第86回日本感染症学会総会学術集会後抄録(II)

第86回日本感染症学会総会学術集会後抄録(II) χ μ μ μ μ β β μ μ μ μ β μ μ μ β β β α β β β λ Ι β μ μ β Δ Δ Δ Δ Δ μ μ α φ φ φ α γ φ φ γ φ φ γ γδ φ γδ γ φ φ φ φ φ φ φ φ φ φ φ φ φ α γ γ γ α α α α α γ γ γ γ γ γ γ α γ α γ γ μ μ κ κ α α α β α

More information

5. F(, 0) = = 4 = 4 O = 4 =. ( = = 4 ) = 4 ( 4 ), 0 = 4 4 O 4 = 4. () = 8 () = 4

5. F(, 0) = = 4 = 4 O = 4 =. ( = = 4 ) = 4 ( 4 ), 0 = 4 4 O 4 = 4. () = 8 () = 4 ... A F F l F l F(p, 0) = p p > 0 l p 0 P(, ) H P(, ) P l PH F PF = PH PF = PH p O p ( p) + = { ( p)} = 4p l = 4p (p 0) F(p, 0) = p O 3 5 5. F(, 0) = = 4 = 4 O = 4 =. ( = = 4 ) = 4 ( 4 ), 0 = 4 4 O 4 =

More information

ron04-02/ky768450316800035946

ron04-02/ky768450316800035946 β α β α β β β α α α Bugula neritina α β β β γ γ γ γ β β γ β β β β γ β β β β β β β β! ! β β β β μ β μ β β β! β β β β β μ! μ! μ! β β α!! β γ β β β β!! β β β β β β! β! β β β!! β β β β β β β β β β β β!

More information

Note.tex 2008/09/19( )

Note.tex 2008/09/19( ) 1 20 9 19 2 1 5 1.1........................ 5 1.2............................. 8 2 9 2.1............................. 9 2.2.............................. 10 3 13 3.1.............................. 13 3.2..................................

More information

第85 回日本感染症学会総会学術集会後抄録(III)

第85 回日本感染症学会総会学術集会後抄録(III) β β α α α µ µ µ µ α α α α γ αβ α γ α α γ α γ µ µ β β β β β β β β β µ β α µ µ µ β β µ µ µ µ µ µ γ γ γ γ γ γ µ α β γ β β µ µ µ µ µ β β µ β β µ α β β µ µµ β µ µ µ µ µ µ λ µ µ β µ µ µ µ µ µ µ µ

More information

Untitled

Untitled 23 1 11 A 2 A.1..................................... 2 A.2.................................. 4 A.3............................... 5 A.4.................................... 6 A.5.......................

More information

K E N Z U 2012 7 16 HP M. 1 1 4 1.1 3.......................... 4 1.2................................... 4 1.2.1..................................... 4 1.2.2.................................... 5................................

More information

7 9 7..................................... 9 7................................ 3 7.3...................................... 3 A A. ω ν = ω/π E = hω. E

7 9 7..................................... 9 7................................ 3 7.3...................................... 3 A A. ω ν = ω/π E = hω. E B 8.9.4, : : MIT I,II A.P. E.F.,, 993 I,,, 999, 7 I,II, 95 A A........................... A........................... 3.3 A.............................. 4.4....................................... 5 6..............................

More information

1 1 2 65

1 1 2 65 3 3 2000 6 14 2 30 4 2 1 1 2 65 1!?? < > 3 2 2 100 19 19 100 100 100 < > 19 2 2 2 2 < > 2000 2000 50 1945 5 50 1945 5 45 20 20 4 1945 4 5 5 5 100 50 20 5 2 20 5 20 5 5 6 20 6 19 5 5 6 5 6 2 20 6 21

More information

B. 41 II: 2 ;; 4 B [ ] S 1 S 2 S 1 S O S 1 S P 2 3 P P : 2.13:

B. 41 II: 2 ;; 4 B [ ] S 1 S 2 S 1 S O S 1 S P 2 3 P P : 2.13: B. 41 II: ;; 4 B [] S 1 S S 1 S.1 O S 1 S 1.13 P 3 P 5 7 P.1:.13: 4 4.14 C d A B x l l d C B 1 l.14: AB A 1 B 0 AB 0 O OP = x P l AP BP AB AP BP 1 (.4)(.5) x l x sin = p l + x x l (.4)(.5) m d A x P O

More information

untitled

untitled 10 log 10 W W 10 L W = 10 log 10 W 10 12 10 log 10 I I 0 I 0 =10 12 I = P2 ρc = ρcv2 L p = 10 log 10 p 2 p 0 2 = 20 log 10 p p = 20 log p 10 0 2 10 5 L 3 = 10 log 10 10 L 1 /10 +10 L 2 ( /10 ) L 1 =10

More information

P1-1 P1-2 P1-3 P1-4 P1-5 P1-6 P3-1 P3-2 P3-3 P3-4 P3-5 P3-6 P5-1 P5-2 P5-3 P5-4 P5-5 P5-6 P7-1 P7-2 P7-3 P7-4 P7-5 P7-6 P9-1 P9-2 P9-3 P9-4 P9-5 P9-6 P11-1 P11-2 P11-3 P11-4 P13-1 P13-2 P13-3 P13-4 P13-5

More information

untitled

untitled 1 ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 2 ( ) 1 ( ) ( ) ( ) ( ) 3 ( ) a b ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 4 ( ) ( ) ( ) ( ) ( ) ( ) < > 5 a b c d ( ) ( ) ( ) ( ) ( ) 18 73 ( ) ( ) a b 6 6 c ( ) (

More information

96 7 1m =2 10 7 N 1A 7.1 7.2 a C (1) I (2) A C I A A a A a A A a C C C 7.2: C A C A = = µ 0 2π (1) A C 7.2 AC C A 3 3 µ0 I 2 = 2πa. (2) A C C 7.2 A A

96 7 1m =2 10 7 N 1A 7.1 7.2 a C (1) I (2) A C I A A a A a A A a C C C 7.2: C A C A = = µ 0 2π (1) A C 7.2 AC C A 3 3 µ0 I 2 = 2πa. (2) A C C 7.2 A A 7 Lorentz 7.1 Ampère I 1 I 2 I 2 I 1 L I 1 I 2 21 12 L r 21 = 12 = µ 0 2π I 1 I 2 r L. (7.1) 7.1 µ 0 =4π 10 7 N A 2 (7.2) magnetic permiability I 1 I 2 I 1 I 2 12 21 12 21 7.1: 1m 95 96 7 1m =2 10 7 N

More information

m 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 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

( ) LAN LAN tex ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 1

( ) LAN LAN tex ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 1 ( ) LAN LAN tex ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 1 1 4 2 17 3 Coulomb 23 4 43 5 49 6 51 7 53 8 58 9 66 10 74 11 Lienard-Wiechert potential 78 12 86 13 89 14 Laplace 114 15 138 16 152 17 162 18 166 19 191

More information

... 3... 3... 3... 3... 4... 7... 10... 10... 11... 12... 12... 13... 14... 15... 18... 19... 20... 22... 22... 23 2

... 3... 3... 3... 3... 4... 7... 10... 10... 11... 12... 12... 13... 14... 15... 18... 19... 20... 22... 22... 23 2 1 ... 3... 3... 3... 3... 4... 7... 10... 10... 11... 12... 12... 13... 14... 15... 18... 19... 20... 22... 22... 23 2 3 4 5 6 7 8 9 Excel2007 10 Excel2007 11 12 13 - 14 15 16 17 18 19 20 21 22 Excel2007

More information

E F = q b E (2) E q a r q a q b N/C q a (electric flux line) q a E r r r E 4πr 2 E 4πr 2 = k q a r 2 4πr2 = 4πkq a (3) 4πkq a 1835 4πk 1 ɛ 0 ɛ 0 (perm

E F = q b E (2) E q a r q a q b N/C q a (electric flux line) q a E r r r E 4πr 2 E 4πr 2 = k q a r 2 4πr2 = 4πkq a (3) 4πkq a 1835 4πk 1 ɛ 0 ɛ 0 (perm 1 1.1 18 (static electricity) 20 (electric charge) A,B q a, q b r F F = k q aq b r 2 (1) k q b F F q a r?? 18 (Coulomb) 1 N C r 1m 9 10 9 N 1C k 9 10 9 Nm 2 /C 2 1 k q a r 2 (Electric Field) 1 E F = q

More information

2 3 4 mdv/dt = F cos(-)-mg sin- D -T- B cos mv d/dt = F sin(-)-mg cos+ L- B sin I d 2 /dt 2 = Ms + Md+ Mn FMsMd MnBTm DLg 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 Hm H h

More information

Gmech08.dvi

Gmech08.dvi 51 5 5.1 5.1.1 P r P z θ P P P z e r e, z ) r, θ, ) 5.1 z r e θ,, z r, θ, = r sin θ cos = r sin θ sin 5.1) e θ e z = r cos θ r, θ, 5.1: 0 r

More information

I ( ) 1 de Broglie 1 (de Broglie) p λ k h Planck ( Js) p = h λ = k (1) h 2π : Dirac k B Boltzmann ( J/K) T U = 3 2 k BT

I ( ) 1 de Broglie 1 (de Broglie) p λ k h Planck ( Js) p = h λ = k (1) h 2π : Dirac k B Boltzmann ( J/K) T U = 3 2 k BT I (008 4 0 de Broglie (de Broglie p λ k h Planck ( 6.63 0 34 Js p = h λ = k ( h π : Dirac k B Boltzmann (.38 0 3 J/K T U = 3 k BT ( = λ m k B T h m = 0.067m 0 m 0 = 9. 0 3 kg GaAs( a T = 300 K 3 fg 07345

More information

日本糖尿病学会誌第58巻第3号

日本糖尿病学会誌第58巻第3号 l l μ l l l l l μ l l l l μ l l l l μ l l l l l l l l l l l l l μ l l l l μ Δ l l l μ Δ μ l l l l μ l l μ l l l l l l l l μ l l l l l μ l l l l l l l l μ l μ l l l l l l l l l l l l μ l l l l β l l l μ

More information

http://www2.math.kyushu-u.ac.jp/~hara/lectures/lectures-j.html 2 N(ε 1 ) N(ε 2 ) ε 1 ε 2 α ε ε 2 1 n N(ɛ) N ɛ ɛ- (1.1.3) n > N(ɛ) a n α < ɛ n N(ɛ) a n

http://www2.math.kyushu-u.ac.jp/~hara/lectures/lectures-j.html 2 N(ε 1 ) N(ε 2 ) ε 1 ε 2 α ε ε 2 1 n N(ɛ) N ɛ ɛ- (1.1.3) n > N(ɛ) a n α < ɛ n N(ɛ) a n http://www2.math.kyushu-u.ac.jp/~hara/lectures/lectures-j.html 1 1 1.1 ɛ-n 1 ɛ-n lim n a n = α n a n α 2 lim a n = 1 n a k n n k=1 1.1.7 ɛ-n 1.1.1 a n α a n n α lim n a n = α ɛ N(ɛ) n > N(ɛ) a n α < ɛ

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...

...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

hirameki_09.dvi

hirameki_09.dvi 2009 July 31 1 2009 1 1 e-mail: [email protected] 2 SF 2009 7 31 3 1 5 1.1....................... 5 1.2.................................. 6 1.3..................................... 7 1.4...............................

More information

untitled

untitled No. 1 2 3 1 4 310 1 5 311 7 1 6 311 1 7 2 8 2 9 1 10 2 11 2 12 2 13 3 14 3 15 3 16 3 17 2 18 2 19 3 1 No. 20 4 21 4 22 4 23 4 25 4 26 4 27 4 28 4 29 2760 4 30 32 6364 4 36 4 37 4 39 4 42 4 43 4 44 4 46

More information

( ) 2.1. C. (1) x 4 dx = 1 5 x5 + C 1 (2) x dx = x 2 dx = x 1 + C = 1 2 x + C xdx (3) = x dx = 3 x C (4) (x + 1) 3 dx = (x 3 + 3x 2 + 3x +

( ) 2.1. C. (1) x 4 dx = 1 5 x5 + C 1 (2) x dx = x 2 dx = x 1 + C = 1 2 x + C xdx (3) = x dx = 3 x C (4) (x + 1) 3 dx = (x 3 + 3x 2 + 3x + (.. C. ( d 5 5 + C ( d d + C + C d ( d + C ( ( + d ( + + + d + + + + C (5 9 + d + d tan + C cos (sin (6 sin d d log sin + C sin + (7 + + d ( + + + + d log( + + + C ( (8 d 7 6 d + 6 + C ( (9 ( d 6 + 8 d

More information

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

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 S I.. http://ayapin.film.s.dendai.ac.jp/~matuda /TeX/lecture.html PDF PS.................................... 3.3.................... 9.4................5.............. 3 5. Laplace................. 5....

More information

1 180m g 10m/s 2 2 6 1 3 v 0 (t=0) z max t max t z = z max 1 2 g(t t max) 2 (6) 1.3 2 3 3 r = (x, y, z) e x, e y, e z r = xe x + ye y + ze z. (7) v =

1 180m g 10m/s 2 2 6 1 3 v 0 (t=0) z max t max t z = z max 1 2 g(t t max) 2 (6) 1.3 2 3 3 r = (x, y, z) e x, e y, e z r = xe x + ye y + ze z. (7) v = 1. 2. 3 3. 4. 5. 6. 7. 8. 9. I http://risu.lowtem.hokudai.ac.jp/ hidekazu/class.html 1 1.1 1 a = g, (1) v = g t + v 0, (2) z = 1 2 g t2 + v 0 t + z 0. (3) 1.2 v-t. z-t. z 1 z 0 = dz = v, t1 dv v(t), v

More information

5.. z = f(x, y) y y = b f x x g(x) f(x, b) g x ( ) A = lim h g(a + h) g(a) h g(x) a A = g (a) = f x (a, b)............................................

5.. z = f(x, y) y y = b f x x g(x) f(x, b) g x ( ) A = lim h g(a + h) g(a) h g(x) a A = g (a) = f x (a, b)............................................ 5 partial differentiation (total) differentiation 5. z = f(x, y) (a, b) A = lim h f(a + h, b) f(a, b) h........................................................... ( ) f(x, y) (a, b) x A (a, b) x (a, b)

More information

http://banso.cocolog-nifty.com/ 100 100 250 5 1 1 http://www.banso.com/ 2009 5 2 10 http://www.banso.com/ 2009 5 2 http://www.banso.com/ 2009 5 2 http://www.banso.com/ < /> < /> / http://www.banso.com/

More information

木オートマトン•トランスデューサによる 自然言語処理

木オートマトン•トランスデューサによる   自然言語処理 木オートマトン トランスデューサによる 自然言語処理 林 克彦 NTTコミュニケーション科学基礎研究所 [email protected] n I T 1 T 2 I T 1 Pro j(i T 1 T 2 ) (Σ,rk) Σ rk : Σ N {0} nσ (n) rk(σ) = n σ Σ n Σ (n) Σ (n)(σ,rk)σ Σ T Σ (A) A

More information

Microsoft Word - Wordで楽に数式を作る.docx

Microsoft Word - Wordで楽に数式を作る.docx Ver. 3.1 2015/1/11 門 馬 英 一 郎 Word 1 する必要がある Alt+=の後に Ctrl+i とセットで覚えておく 1.4. 変換が出来ない場合 ごく稀に以下で説明する変換機能が無効になる場合がある その際は Word を再起動するとまた使えるようになる 1.5. 独立数式と文中数式 数式のスタイルは独立数式 文中数式(2 次元)と文中数式(線形)の 3 種類があ り 数式モードの右端の矢印を選ぶとメニューが出てくる

More information

http://www.ike-dyn.ritsumei.ac.jp/ hyoo/wave.html 1 1, 5 3 1.1 1..................................... 3 1.2 5.1................................... 4 1.3.......................... 5 1.4 5.2, 5.3....................

More information