宇宙航空研究開発機構研究開発報告
JAXA Research and Development Report
JAXA極超音速風洞における6分力計測試験に係る 誤差評価について
Error Evaluation in JAXA Hypersonic Wind Tunnel Force Measurement Tests
藤井 啓介,高間 良樹
FUJII Keisuke and TAKAMA Yoshiki
2020年7月
宇宙航空研究開発機構
Japan Aerospace Exploration Agency
2 ޡࠩධՁʹؔ͢ΔཧɾఆࣜԽ 8
2.1 ܭଌޡࠩͷۭྗਪఆޡࠩͷ. . . . 8
2.2 ؾྲྀͷඇҰ༷ੑ͕ٴ΅͢6ྗܭଌͷӨڹ . . . . 12
3 ޡࠩධՁͷ෩ಎࢼݧͷద༻ 16 3.1 JAXAۃԻ෩ಎͱ6ྗܭଌܥͷ֓ཁ . . . . 16
3.2 ཁૉܭଌޡࠩ . . . . 16
3.2.1 ఈ໘ѹpbܭଌޡࠩͷਪఆ . . . . 17
3.2.2 ϐτʔѹൺpp02o ޡࠩͷਪఆ . . . . 19
3.2.3 HWT2ʹ͓͚Δඪ४ܕࢼݧʹΑΔݕূ . . . . 23
3.3 ඇҰ༷ੑޮՌਪఆͷ࣮ݧ݁ՌΛ༻͍ͨݕূ . . . . 26
3.3.1 ෩ಎࢼݧ֓ཁ(HWT14-51). . . . 26
3.3.2 ඇҰ༷ੑޮՌਪఆͷݕূ . . . . 28
3.3.3 HWT2ʹ͓͚ΔඇҰ༷ੑޮՌͷਪఆ . . . . 30
3.4 ࣠ରশܗঢ়ඪ४ܕΛ༻͍ͨ֯ޡࠩͷఱടग़ྗͷӨڹධՁ . . . . 30
3.4.1 ࠲ඪܥͷఆٛ . . . . 34
3.4.2 HWT2ඪ४ܕࢼݧ݁Ռ࠶ཧ . . . . 34
3.4.3 HWT1ඪ४ܕࢼݧ݁Ռ࠶ཧ . . . . 39
4 ݁ 41 A HWT2ʹ͓͚ΔදҰ༷ྲྀMachɺඇҰ༷ੑͱɺෆ͔֬͞ 45 B ఱടग़ྗ͔Βͷࢼݧܕॏྔॏ৺ٴͼఱടऔ֯ͷਪఆ 46 B.1 ҹՃՙॏͱఱടग़ྗ . . . . 48
B.2 ఱടॲཧʹ͓͚Δมͷఆٛ . . . . 48
B.3 ॏྔɾॏ৺ɾΦϑηοτྔٴͼॳظ࢟֯ޡࠩਪఆ . . . . 51
B.4 ௨෩࣌ॲཧ . . . . 54
5
C ఱട֯ޡࠩʹΑΔޡࠩ 54
6 6 10
14 14 14 15 17 21 24 24 26 28 28 32 32 37
39 43
44 46 46 49 52
52
This document is provided by JAXA
౻Ҫܒհɺߴؒྑथ
Error Evaluation in JAXA Hypersonic Wind Tunnel Force Measurement Tests
Fujii Keisuke and Takama Yoshiki
Abstract
The free-stream Mach number of JAXA 1.27m/0.5m hypersonic wind tunnel had been reported to actually fluctuate between blows with a small extent which could still be one of the major error sources in aerody- namic coefficients reduced from measurements. The cause of the fluctuation still remains unclear, however, an attempt to remedy such the unexpected varying Mach number effect has been made by accounting repre- sentative dynamic pressure variation between blows with leveraging pitot pressure monitoring measurement which is originally for wind tunnel validity evaluation purposes. The effectiveness of the remedy has then been evaluated based on data acquired through HB2 standard model tests ever conducted in the facility, in accordance with the error propagation relation developed for the proposed procedure to determine the free-stream Mach number.
Non-uniformity of the free-stream, however, cannot be accounted as an error source in the above uncertainty analysis, though previous M5 tests in the 0.5m hypersonic wind tunnel showed it actually has considerable effects, especially on the pitching moment coefficient. The mathematical formulation for estimating the error induced by the non-uniformity was then derived in terms of the three-dimensional spatial power spectrum of the pitot pressure ratio distribution and of the test model shape information, separately. Standard model test results where the test model was placed in different locations in the free-stream core region, agreed well with the estimated error from the non-uniformity, especially in the longitudinal aerodynamic characteristics, exhibiting the validity of the estimation formulation.
One of major error sources in the lateral-directional characteristics in the facility, however, turned out to be alignment errors of the balance coordinate and of the model coordinate, after examining again aerodynamic characteristics obtained in the axisymmetric standard model and reorganizing them by correcting the model coordinate directions based on the balance alignment angles estimated from static tare data.
keywords : Error in force measurements, Mach number fluctuation, Non-uniformity, Alignment error
֓ཁ
JAXA 1.27m/0.5mۃԻ෩ಎࢼݧ6ྗܭଌʹ͓͚ΔޡࠩཁҼͱͯ͠Ұ༷ྲྀMach͕มಈ͢Δݱͷ֬
ೝ͞Εͨ͜ͱΛड͚ɺؾྲྀ݈શੑ֬ೝͷͨΊͷϐτʔѹͷϞχλʔܭଌ݁ՌΛར༻͠ɺ͜Ε·ͰෆมͱԾఆ͠
ͯॲཧ͞Ε͍ͯͨҰ༷ྲྀMachΛɺ௨෩ຖʹਪఆɾमਖ਼͢Δ͜ͱͰಈѹਪఆٴͼۭྗܭଌਫ਼ͷ্Λ
藤井 啓介 ,高間 良樹
Error Evaluation in JAXA Hypersonic Wind Tunnel Force Measurement Tests
FUJII Keisuke
*1, TAKAMA Yoshiki
*1概要
ࢼΈͨɻͦͷࡍʹैདྷσʔλॲཧٴͼ͜ͷಈѹमਖ਼ॲཧʹଈͨ͠ޡࠩΛཧͨ͠͏͑Ͱɺܭଌਫ਼ͷޮ
ՌͷݕূΛ͜Ε·ͰܧଓతʹߦΘΕ͖͍ͯͯͨHB2ඪ४ܕࢼݧͷ݁ՌΛͱʹߦͬͨɻಉ࣌ʹɺJAXAۃ
Ի෩ಎͰͷඪ४తܭଌʹ͓͚ΔؾྲྀಛੑɾਪఆޡࠩɺܭଌޡࠩΛཧ͠Ұൠͷ6ྗܭଌࢼݧʹ͓͍ͯظ
͞ΕΔޡࠩਪఆํ๏Λཧ͠ɺͦͷଥੑ֬ೝΛߦͬͨɻߋʹؾྲྀͷඇҰ༷ੑʹΑΓൃੜ͢ΔۭؾྗɾϞʔϝ ϯτܭଌʹ͓͚Δෆ͔֬͞ΛɺؾྲྀಈѹͷۭؒύϫʔεϖΫτϧͱɺܕܗঢ়ใͱ͔Β༧ଌ͢Δख๏Λ
։ൃ͠ɺͦͷ༧ଌଥੑΛඪ४ܕࢼݧ݁ՌΛجʹධՁͨ͠ɻͦͷ݁Ռɺಛʹॎ3ྗʹ͓͚ΔඇҰ༷ੑޮՌ Λ༧ଌ͢Δ͜ͱ͕Ͱ͖Δ͜ͱΛ֬ೝͨ͠ɻԣɾํಛੑʹؔ͢ΔۃԻ෩ಎࢼݧʹ͓͚ΔओཁͳޡࠩཁҼ
ҰํͰɺҰൠʹۭؾྗɾϞʔϝϯτͷେ͖͕͞খ͍ͨ͞ΊɺಈѹมಈͰɺඇҰ༷ੑͷޮՌͰͳ͘ɺఱട
ܕ࠲ඪͷऔޡࠩʹىҼ͢Δɺଞྗͷ࿙ΕͰ͋Δ߹ͷଟ͍͜ͱ͕ߟ͑ΒΕͨͨΊɺ෩ಎܕΛऔΓ͚
ͨঢ়ଶͰɺఱടʹՃΘΔॏྗΛར༻ͨ͠ఱടऔ֯ਪఆํ๏Λ৽ͨʹ։ൃ͠ɺաڈʹ࣮ࢪ͞Εͨ࣠ରশܗঢ় ͷඪ४ܕࢼݧʹద༻ͨ͠ɻͦͷ݁ՌɺఱടऔΓ͚֯ਪఆ݁ՌΛجʹܕͷؾྲྀʹର͢Δ࢟Λิਖ਼͢Δ
͜ͱͰɺԣɾํಛੑʹؔ͢ΔओཁޡࠩཁҼͱͯ͠ɺఱടɾܕऔΓ͚֯ਫ਼͋ΓಘΔ͜ͱΛ֬ೝͨ͠ɻ
ه߸
A ४Ұ࣍ݩྲྀʹ͓͚Δྲྀ࿏அ໘ੵ , m2
A2, A3, A4 ࠲ඪม3×3ߦྻ(ࣜ(27)ʹΑΔʣ , ND
A2p, A3p, A4p ࠲ඪม3×3ߦྻ(ࣜ(26)ʹΑΔʣ , ND AF ײʢࣜ(2)ʹΑΔʣ , N−1 Aijk ఱടֱਖ਼
AM ܕ࠲ඪɾଌఆࣨ࠲ඪͷ࠲ඪม3×3ߦྻʢࣜ(29)ʣ
Ap02 ײʢࣜ(2)ʹΑΔʣ , ND Apb ײʢࣜ(2)ʹΑΔʣ , Pa−1 Apo ײʢࣜ(2)ʹΑΔʣ , Pa−1 a0, a1, a2 ࣜ(24)ͰݱΕΔ , ND ap ؾྲྀίΞදϐτʔѹ/ϞχλʔܭଌҐஔϐτʔѹ(≡pp02s02) , ND a∗p ಛఆྖҬฏۉϐτʔѹൺͱಛఆҐஔϐτʔѹൺͱͷൺ , ND Bijk ఱടֱਖ਼ʢࣜ(25)ʹΑΔ)
CAF લ໘࣠ྗ , ND
CN B ϤʔΠϯάϞʔϝϯτɹ , ND
CY ԣྗ , ND
Cp ѹྗ , ND
co ܕ࠲ඪʹ͓͚Δॏ৺ҐஔྻϕΫτϧ≡(cx, cy, cz)t , m
cx, cy, cz ॏ৺Ґஔx, y, z࠲ඪ , m
CN B′ ༗ޮܴ֯ํʹରԠ͢ΔϤʔΠϯάϞʔϝϯτ(ࣜ(22)ʣ , ND CY′ ༗ޮܴ֯ํʹରԠ͢Δԣྗ(ࣜ(21)ʣ , ND
D ܕදܘ , m
Db 3×6ఱടᎡΈߦྻɹʢࣜ(30)ʹΑΔʣ
Df ఱട࢟֯ਪఆ࣌F ͷ6×6ॏΈର֯ߦྻ , ND F ྗۭؒϕΫτϧͷۭؒϑʔϦΤม͞Εͨͷ , Nm3
ࢼΈͨɻͦͷࡍʹैདྷσʔλॲཧٴͼ͜ͷಈѹमਖ਼ॲཧʹଈͨ͠ޡࠩΛཧͨ͠͏͑Ͱɺܭଌਫ਼ͷޮ
ՌͷݕূΛ͜Ε·ͰܧଓతʹߦΘΕ͖͍ͯͯͨHB2ඪ४ܕࢼݧͷ݁ՌΛͱʹߦͬͨɻಉ࣌ʹɺJAXAۃ
Ի෩ಎͰͷඪ४తܭଌʹ͓͚ΔؾྲྀಛੑɾਪఆޡࠩɺܭଌޡࠩΛཧ͠Ұൠͷ6ྗܭଌࢼݧʹ͓͍ͯظ
͞ΕΔޡࠩਪఆํ๏Λཧ͠ɺͦͷଥੑ֬ೝΛߦͬͨɻߋʹؾྲྀͷඇҰ༷ੑʹΑΓൃੜ͢ΔۭؾྗɾϞʔϝ ϯτܭଌʹ͓͚Δෆ͔֬͞ΛɺؾྲྀಈѹͷۭؒύϫʔεϖΫτϧͱɺܕܗঢ়ใͱ͔Β༧ଌ͢Δख๏Λ
։ൃ͠ɺͦͷ༧ଌଥੑΛඪ४ܕࢼݧ݁ՌΛجʹධՁͨ͠ɻͦͷ݁Ռɺಛʹॎ3ྗʹ͓͚ΔඇҰ༷ੑޮՌ Λ༧ଌ͢Δ͜ͱ͕Ͱ͖Δ͜ͱΛ֬ೝͨ͠ɻԣɾํಛੑʹؔ͢ΔۃԻ෩ಎࢼݧʹ͓͚ΔओཁͳޡࠩཁҼ
ҰํͰɺҰൠʹۭؾྗɾϞʔϝϯτͷେ͖͕͞খ͍ͨ͞ΊɺಈѹมಈͰɺඇҰ༷ੑͷޮՌͰͳ͘ɺఱട
ܕ࠲ඪͷऔޡࠩʹىҼ͢Δɺଞྗͷ࿙ΕͰ͋Δ߹ͷଟ͍͜ͱ͕ߟ͑ΒΕͨͨΊɺ෩ಎܕΛऔΓ͚
ͨঢ়ଶͰɺఱടʹՃΘΔॏྗΛར༻ͨ͠ఱടऔ֯ਪఆํ๏Λ৽ͨʹ։ൃ͠ɺաڈʹ࣮ࢪ͞Εͨ࣠ରশܗঢ় ͷඪ४ܕࢼݧʹద༻ͨ͠ɻͦͷ݁ՌɺఱടऔΓ͚֯ਪఆ݁ՌΛجʹܕͷؾྲྀʹର͢Δ࢟Λิਖ਼͢Δ
͜ͱͰɺԣɾํಛੑʹؔ͢ΔओཁޡࠩཁҼͱͯ͠ɺఱടɾܕऔΓ͚֯ਫ਼͋ΓಘΔ͜ͱΛ֬ೝͨ͠ɻ
ه߸
A ४Ұ࣍ݩྲྀʹ͓͚Δྲྀ࿏அ໘ੵ , m2
A2, A3, A4 ࠲ඪม3×3ߦྻ(ࣜ(27)ʹΑΔʣ , ND
A2p, A3p, A4p ࠲ඪม3×3ߦྻ(ࣜ(26)ʹΑΔʣ , ND AF ײʢࣜ(2)ʹΑΔʣ , N−1 Aijk ఱടֱਖ਼
AM ܕ࠲ඪɾଌఆࣨ࠲ඪͷ࠲ඪม3×3ߦྻʢࣜ(29)ʣ
Ap02 ײʢࣜ(2)ʹΑΔʣ , ND Apb ײʢࣜ(2)ʹΑΔʣ , Pa−1 Apo ײʢࣜ(2)ʹΑΔʣ , Pa−1 a0, a1, a2 ࣜ(24)ͰݱΕΔ , ND ap ؾྲྀίΞදϐτʔѹ/ϞχλʔܭଌҐஔϐτʔѹ(≡pp02s02) , ND a∗p ಛఆྖҬฏۉϐτʔѹൺͱಛఆҐஔϐτʔѹൺͱͷൺ , ND Bijk ఱടֱਖ਼ʢࣜ(25)ʹΑΔ)
CAF લ໘࣠ྗ , ND
CN B ϤʔΠϯάϞʔϝϯτɹ , ND
CY ԣྗ , ND
Cp ѹྗ , ND
co ܕ࠲ඪʹ͓͚Δॏ৺ҐஔྻϕΫτϧ≡(cx, cy, cz)t , m
cx, cy, cz ॏ৺Ґஔx, y, z࠲ඪ , m
CN B′ ༗ޮܴ֯ํʹରԠ͢ΔϤʔΠϯάϞʔϝϯτ(ࣜ(22)ʣ , ND CY′ ༗ޮܴ֯ํʹରԠ͢Δԣྗ(ࣜ(21)ʣ , ND
D ܕදܘ , m
Db 3×6ఱടᎡΈߦྻɹʢࣜ(30)ʹΑΔʣ
Df ఱട࢟֯ਪఆ࣌F ͷ6×6ॏΈର֯ߦྻ , ND F ྗۭؒϕΫτϧͷۭؒϑʔϦΤม͞Εͨͷ , Nm3
F ྗɾϞʔϝϯτ6ݩྻϕΫτϧ , N·ͨNm
FA ࣠ྗ , N
Fi Fͷiํ , Nm3
f ྗۭؒϕΫτϧ , N
fC ܕʹΔۭؾྗͷಛੑʢࣜ(13)ʣ , m2 i,j,k ࠲ඪܥަ୯ҐϕΫτϧ , ND
K ෆ͔֬͞ղੳแׅ , ND
KB ෆ͔֬͞ղੳόΠΞεภࠩͷแׅʹ૬͢Δ , ND
L ද͞ , m
Ld ཚͷද͞εέʔϧ , m
Lm ڙࢼܕͷද͞εέʔϧ , m
M Ϛοϋ , ND
M ϞʔϝϯτۭؒϕΫτϧͷۭؒϑʔϦΤม͞Εͨͷ , Nm4 M2B ܕ࠲ඪɾఱട࠲ඪؒͷ࠲ඪม3×3ߦྻ(ࣜ(28)ʣ , ND
Mi Mͷiํ , Nm4
m ϞʔϝϯτۭؒϕΫτϧ , Nm
mC ܕʹΔۭྗϞʔϝϯτͷಛੑʢࣜ(15)ʣ , m3
p ѹྗ , Pa
p02 (දత)ϐτʔѹɹ , Pa
p02s ܭଌҐஔʹ͓͚Δϐτʔѹɹ , Pa
pT.C. ଌఆࣨѹྗ , Pa
Qf ಈѹqͷۭؒϑʔϦΤม , Nm
q ಈѹ , Pa
Runit ୯ҐReynolds , m−1
S ໘ੵ , m2
S ఱടग़ྗྻϕΫτϧ ≡(S1, . . . , S6)t , V
Si ఱടग़ྗ , V
s ද໘ཁૉۭؒϕΫτϧ , m2
s 3ݩྻϕΫτϧɹ≡(sx, sy, sz)t , ND
sx ≡sinθg , ND
sy ≡cosθgsinϕg , ND
sz ≡ −cosθgcosϕg , ND
t ࣌ؒ , s
U ෆ͔֬͞
V ମੵ , m3
W ॏྔ , N
Wc ॏྔॏ৺ʹؔ͢Δ4ݩྻϕΫτϧ≡(W, cx, cy, cz)t , Nຢm
x ҐஔۭؒϕΫτϧ , m
xo ܕݪͷҐஔۭؒϕΫτϧ , m
x, y, z xͷ࠲ඪ , m
α ܴ֯ , deg
α, β, γ , m−1
αeff ༗ޮܴ֯ , deg
β ԣΓ֯ , deg
γ ൺൺ
δ ޡࠩ
δ∗ ਪఆޡࠩ
Θ (β, θ, ϕ)ྻϕΫτϧ , deg
Θg (θg, ϕg)2ݩྻϕΫτϧ , deg θ, ϕ ϐον֯ɺϩʔϧ֯ , deg
σ ඪ४ภࠩ
σf ྗͷඪ४ภۭࠩؒϕΫτϧ , N σm Ϟʔϝϯτͷඪ४ภۭࠩؒϕΫτϧ , Nm subscript
0 ਅ
b ఈ໘
o ఽΈঢ়ଶ
∞ Ұ༷ྲྀঢ়ଶ
CM Ϟʔϝϯτج४Ґஔ
superscript
′ มಈ
x, y, z xͷ࠲ඪ , m
α ܴ֯ , deg
α, β, γ , m−1
αeff ༗ޮܴ֯ , deg
β ԣΓ֯ , deg
γ ൺൺ
δ ޡࠩ
δ∗ ਪఆޡࠩ
Θ (β, θ, ϕ)ྻϕΫτϧ , deg
Θg (θg, ϕg)2ݩྻϕΫτϧ , deg θ, ϕ ϐον֯ɺϩʔϧ֯ , deg
σ ඪ४ภࠩ
σf ྗͷඪ४ภۭࠩؒϕΫτϧ , N σm Ϟʔϝϯτͷඪ४ภۭࠩؒϕΫτϧ , Nm subscript
0 ਅ
b ఈ໘
o ఽΈঢ়ଶ
∞ Ұ༷ྲྀঢ়ଶ
CM Ϟʔϝϯτج४Ґஔ
superscript
′ มಈ
1 ং
JAXAϕ0.5m/1.27mۃԻ෩ಎ[1]ʹ͓͚Δݱঢ়ͷσʔλॲཧɺ෩ಎؾྲֱྀਖ਼ࢼݧ[2]ʹΑͬͯಘΒΕͨ
Ұ༷ྲྀMach͕ෆมͰ͋ΔͱԾఆ͠ɺܭଌ͞ΕΔ෩ಎఽΈѹྗpoɺఽΈԹTo͔Βɺฏߧ࣮ࡏؾମΛԾఆ
͢Δ͜ͱʹΑͬͯҰ༷ྲྀ੩ѹp∞ٴͼಈѹqΛਪఆ͠ɺఱടग़ྗͰ͋ΔۭؾྗΛແ࣍ݩԽ͢Δख๏Λ࠾༻ͯ͠
͖͍ͯΔɻ͔͠͠ͳ͕ΒɺҰൠʹϊζϧுաఔʹ͓͍ͯٸʹݮগ͢ΔີͱڞʹɺৼಈྭىΤωϧΪʔ͕
ࣄ্࣮ౚ݁ͯ͠͠·͏͍ΘΏΔnozzle freezing͕εϩʔτۙͰൃੜ͢Δ͜ͱ͕༧ଌ͞Ε͓ͯΓ[3]ɺ࣮ࡍɺۙ
ͷ෩ࢼσʔλͷ࠶ཧʹ͓͍ͯฏߧ࣮ࡏؾମΛԾఆͨ͠ϊζϧுؔࣜΑΓϊζϧౚ݁Λٖ͢Δશ ؾମؔࣜͷํ͕ɺೡΖۭྗಛੑଌఆΒ͖ͭΛݮͤ͞Δͱ͍͏ใࠂ͕ͳ͞Ε͍ͯΔ[4]ɻͦͷόϥ͖ͭධ Ձͷࡍʹ͜Ε·Ͱͷ෩ಎࢼݧʹ͓͍ͯҰ༷ྲཱྀੑ֬ೝͷతͰಉ࣌ܭଌ͍ͯͨ͠ϐτʔѹϞχλʕܭଌΛ
࠶ཧͨ͠ͱ͜Ζɺ௨෩ຖʹϐτʔѹൺp02/po͕ແࢹͰ͖ͳ͍ϨϕϧͰมಈ͍ͯ͠Δ͜ͱ͕͋Θͤͯ֬ೝ͞Ε
ͨɻ͜ΕɺෆมͰ͋ΔͱԾఆ͞Ε͍ͯͨҰ༷ྲྀMach͕มಈ͍ͯ͠Δ͜ͱɺ·ͨͦͷมಈྔ͕࣮ݧ݁
Ռͷ࠶ݱੑݕূʹ͓͍ͯେ͖ͳӨڹΛ༩͑ΔఔͰ͋Δ͜ͱΛҙຯ͍ͯͨ͠ɻ͜Ε·Ͱͷ6ྗܭଌʹ͓͚Δ ޡࠩධՁͰɺؾྲֱྀਖ਼ࢼݧ࣌ʹಘΒΕͨMachͷۭؒతɾ࣌ؒతมಈྔͱɺ֤ܭଌྔʹ͓͚ΔޡࠩΛΈ߹
ΘͤͨͷΈͰ͋ΓɺࢼݧΩϟϯϖʔϯຖʹมಈ͢Δϐτʔѹൺp02/poʢ͋Δ͍ɺҰ༷ྲྀMach)ʹؔ͢Δ ߟྀ͕ͳ͔ͬͨͨΊɺঢ়گʹΑΓఆ͞ΕΔޡࠩൣғҎ্ͷ࠶ݱੑࠩҟͷੜ͡Δ͜ͱ͕༧ଌ͞Εɺ࣮ࡍಉҰ
ܕʹΑΔҟͳΔ࣌ظʹ࣮ࢪͨ͠ࢼݧΩϟϯϖʔϯʹ͓͍ͯఆޡࠩҎ্ͷ࠶ݱੑόϥ͖ͭͷ͋Δ͜ͱ͕͔ͬ
ͨɻͦ͜Ͱܭଌ੍͕େ͖͍ͷͷϐτʔѹϞχλʔܭଌΛ༻͍ࢼݧຖͰมಈ͢ΔཧྔΛ‘ܭଌޡࠩ’ͱͯ͠
ѻ͏ͷͰͳ͘ਖ਼ʹධՁ͢Δ͜ͱͰɺΑΓਫ਼ͷߴ͍ࢼݧɾܭଌΛࢦ͢͜ͱͱͨ͠ɻͦͷΑ͏ͳσʔλॲ ཧΛ͢Δ߹ɺ֤ʑͷܭଌޡࠩɺ࠶ݱੑόϥ͖ͭͷ6ྗ’ܭଌ’ޡࠩͷΛ໌֬Խ͠ɺͦͷํ๏ʹΑΔ ޡࠩݮޮՌΛධՁ͢Δඞཁ͕ੜ͡ɺJAXAϕ1.27mۃԻ෩ಎʹ͓͚Δैલͱ৽نఏҊख๏ʹΑΔσʔλ ॲཧͦΕͧΕʹଈͨ͠ޡࠩΛཧͨ͠ɻ͜͜Ͱɺ6ྗۭྗத࠷ؔ࿈ཧྔͷଟ͍લ໘࣠ྗ
CAFʹॏΛஔ͖ɺաڈʹ࣮ࢪ͞Εͨඪ४ܕࢼݧٴͼؾྲֱྀਖ਼ࢼݧΛجʹɺఆ͞ΕΔ֤ܭଌɾਪఆཁૉ
ʹ͓͚ΔޡࠩͷجૅσʔλཧɾଥੑධՁΛߦ͏͜ͱͱͨ͠ɻ͜ͷཧʹΑΓ୯ಠͷ̒ྗࢼݧʹ͓͚Δޡ
ࠩྔਪఆʹඞཁͳ෩ಎಛੑʹؔ͢Δෆ֬ఆੑɺ֤ܭଌʹ͓͚ΔޡࠩྔΛ໌֬Խ͢Δ͜ͱΛతͱͨ͠ɻ
ͦΕΒ֤ܭଌɾਪఆޡࠩͷݕ౼Ͱ෩ಎҰ༷ྲྀίΞྖҬͰͷϐτʔѹฏۉ͓Αͼɺͦͷฏۉͷมಈ
͢ΔྔΛߟྀͨ͠ޡࠩධՁΛߦ͍ͬͯΔ͕ɺ6ྗܭଌͷಈѹͷޮՌɺ͋Δ͍ؾྲྀͷඇҰ༷ੑͷޮՌ Λਖ਼ʹධՁ͍ͯ͠Δͱݴ͑ͳ͍ɻؾྲྀͷඇҰ༷ੑʹىҼ͢ΔۭྗಛੑͷޮՌʹؔͯ͠ɺܕҐஔΛൺ
ֱత༰қʹมߋͰ͖Δϕ0.5mۃԻ෩ಎ(HWT1)ʹ͓͚Δඪ४ܕࢼݧʹΑΓಛʹϐονϯάϞʔϝϯτ
ͷӨڹ͕͔ͳΒͣ͠ແࢹͰ͖ͳ͍ྔͱͳ͍ͬͯΔ͜ͱ͕໌͍ͯ͠Δ[5]ɻ͔͠͠ͳ͕ΒͦͷඇҰ༷ੑͷޮ
Ռܕܗঢ়ʹڧ͘ґଘ͢Δ͜ͱఆ͞ΕΔͨΊɺඪ४ܕࢼݧͷޮՌΛಛఆͨ͠ͷΈͰɺҰൠͷࢼݧ ʹ͓͚ΔޡࠩධՁΛ͢Δ͜ͱ͕Ͱ͖ͳ͍ɻඇҰ༷ੑޮՌͷޡࠩݶքΛΔͨΊͷྗͱͯ͜͠Ε·Ͱʹɺಈѹ
ʹ͓͚Δ͞εέʔϧΛߟྀͤͣಈѹͷۭؒతมಈྔ͕ͦͷ··ۭؾྗͷภΓޡࠩͱͳΔͱ͍͏ϞσϧΛ
༻͍Δ؆қख๏࣮ࢪ͞ΕΔ͜ͱ͕͕͋ͬͨɺͦͷΑ͏ͳํ๏ͰɺྗܭଌͷӨڹʹؔ͠ෆ͔֬͞ͷ্ݶΛ
͑Δ͜ͱͰ͖ΔͷͷɺϞʔϝϯτܭଌʹ͓͚Δෆ͔֬͞ʹؔͯ͠ɺ߹ཧతͳ͞εέʔϧΛߟྀ͠ͳ
͍ͨΊ্ݶ͢ΒධՁ͢Δ͜ͱͰ͖͍ͯͳ͍ɻྫ͑ಈѹඇҰ༷ੑͷද͞εέʔϧLdʹ͘Β
ܕදLm͕ेʹେ͖͍߹(Ld≪Lm)ඇҰ༷ੑͷӨڹฏۉԽ͞ΕແࢹͰ͖Δͱ༧Ͱ͖ΔҰํͰɺ ٯͷঢ়گͷ߹(Ld≫Lm)ɺܭଌ͞ΕΔۭؾྗͷόϥ͖ͭؾྲྀඇҰ༷ੑͷಈѹόϥ͖ͭͱಉఔͱͳΔͷ ͱ༧͞Εɺද͞εέʔϧ͕ಉఔLm≈LdͱͳΓͦ͏Ͱ͋Δ߹ɺӨڹͦͷதؒͷఔͱͳΔͱߟ
͑ΒΕΔͨΊɺܕද͞ͱಈѹද͞εέʔϧͱͷؔͰͦͷӨڹมԽ͢ΔͣͷͷͰ͋Δɻ ߋʹϞʔϝϯτʹؔͯ͠ɺLd ≪Lmͷ߹ͰLm≪Ldͷ͍ͣΕͷ߹ͰܕҐஔͷӨڹۃݶͰ
ফ໓͢Δ͜ͱͱͳΓɺLm≈Ldͷۙʹ͓͍ͯͷΈ༗ݶΛͱΔͱ༧Ͱ͖Δ͕ɺͦͷ্ݶΛ؆ศʹಘΔ൚
༻తͳख๏͜Ε·ͰʹఏҊ͞Ε͍ͯͳ͍ɻ͜ͷɺ෩ಎࢼݧΛ௨ͯ͡τϦϜܴ֯ͷ༧ଌඞཁͳ໘ͷ
1 序論
ઃܭΛ͢Δঢ়گʹ͓͍ͯॏཁͳཁૉͱͳΔՄೳੑ͕ߟ͑ΒΕΔͨΊɺؾྲྀͷඇҰ༷ੑͷٴ΅ۭ͢ؾྗɺಛʹۭ
ྗϞʔϝϯτͷӨڹΛࢼݧܕʹԠͯ͡దʹ༧ଌ͢Δ͜ͱͷඞཁੑΛ͍ࣔͯ͠Δͱ͍͑ΔɻۭؾྗɾϞʔ ϝϯτͷӨڹΛܾఆ͢Δͱߟ͑ΒΕΔؾྲྀඇҰ༷ੑͷදLdα, β, γͷٯͱͱΒ͑Δ͜ͱ͕Ͱ
͖ɺ෩ಎؾྲྀಈѹͷۭؒύϫʔεϖΫτϧ͕ӨڹධՁͷͨΊʹඞཁͳใͰ͋Δͱߟ͑ΒΕͨɻͦͷͨΊ ؾྲֱྀਖ਼ࢼݧͰಘΒΕ͍ͯΔಈѹͷۭؒύϫʔεϖΫτϧΛͱΓɺͷ͞εέʔϧͱܕදͱͷ
ؔΛߟྀ͢ΔӨڹධՁͷఆࣜԽΛߦ͏͜ͱͱͨ͠ɻ·ͨͦͷධՁ๏ͷݕূͱͯ͠ɺաڈʹHWT1M5෩ಎʹ
͓͍࣮ͯࢪ͞ΕͨܕઃஔҐஔมߋޮՌࢼݧ݁Ռʹ͓͚Δۭྗಛੑมಈྔͱɺ༧ଌ݁ՌͱͷൺֱΛߦ͍ɺͦͷ ଥੑΛ֬ೝ͢Δ͜ͱͱͨ͠ɻ
ۃԻ෩ಎ6ྗܭଌʹ͓͚ΔओཁͳޡࠩཁҼҎ্ʹΑΓධՁͰ͖Δͱߟ͑ΒΕΔ͕ɺ௨ৗͷࢼݧܗଶͰ
Ұൠʹۭؾྗͷখ͍͞ԣɾํಛੑʹؔͯ͠ɺఱടɾܕऔ֯ޡࠩΛ௨ͨ͠ΑΓେ͖ͳۭؾྗͷൃੜ͠
͍ͯΔॎ3ྗͷӨڹ͕ೡΖओཁͳޡࠩཁҼͱͳΓಘΔ͜ͱ͕໌͖ͯͨ͠ɻࢼݧܕऔ࣌ʹൃੜ͢Δ
ܕ࠲ඪܥͱఱട࠲ඪܥʹ͓͚Δऔ֯ޡࠩʹىҼ͢ΔޡࠩධՁʹ͓͍ͯɺࢼݧܕऔঢ়ଶʹ͓͚Δܕ࢟
֯ܭଌʹՃ͑ɺͦͷঢ়ଶʹ͓͚Δఱട࢟֯ܭଌΛߦ͏͜ͱͰɺܕɾఱടؒऔ֯Λਪఆ͢Δඞཁ͕͋Δɻ
ͦͷΑ͏ͳഎܠ͔ΒۃԻ෩ಎͰɺܕʹಇ͘ॏྗΛෳ࢟֯έʔεͰܭଌ͢Δ͜ͱͰɺఱടॲཧʹඞ ཁͳܕॏྔɾॏ৺Ґஔɺఱടग़ྗΦϑηοτྔͷਪఆʹՃ͑ɺఱട࠲ඪܥͷ࢟֯ਪఆ͋Θͤͯߦ͏ํ๏
ΛۙऔΓೖΕ͍ͯΔɻ͜͜Ͱ͜ͷఱടऔ֯ਪఆͷଥੑΛධՁ͢Δ͜ͱΛతʹɺ͜Ε·ͰʹߦΘΕͯ
͖ͨ࣠ରশඪ४ܕࢼݧۭྗಛੑٴͼఱടֱਖ਼݁ՌΛ࠶ධՁ͢Δ͜ͱͱͨ͠ɻͦΕʹ͍ɺ෩ಎࢼݧ࣌ʹఆ
͖͢ܕɾఱടऔ֯ޡࠩͱͯ͠ݟࠐΉ͖ྔΛਪఆ͢Δ͜ͱͱͨ͠ɻ·ͨɺຊߘʹ͓͍ͯɺޡࠩݸʑ ͷܭଌͱਅͱͷࠩΛࢦ͠ɺෆ͔֬͞ܭଌपΓʹਅͷଘࡏ͢ΔൣғΛࢦ͢ͷͱ͢Δɻ
2 ޡࠩධՁʹؔ͢ΔཧɾఆࣜԽ
2.1 ܭଌޡࠩͷۭྗਪఆޡࠩͷ
Ұൠʹɺલ໘࣠ྗCAF ܭଌྔ͋Δ͍ܭଌྔ͔ΒٻΊΒΕΔঢ়ଶྔΛ༻͍ͯҎԼͷΑ͏ʹఆٛ͞Εͯ
͍Δ:
CAF ≡FA−Sb(p∞−pb) qS
͜͜Ͱɺ෩ಎࢼݧʹ͓͚ΔܭଌྔͰ͋Δ࣠ྗFAٴͼϕʔεѹpb͍ͣΕɺҎԼͷΑ͏ʹ‘ਅ’ͱܭଌޡࠩ
ͱ͔Βߏ͞ΕΔͱߟ͑ɺ·ͨਅɺܭଌޡࠩͦΕͧΕฏۉٴͼมಈʹ͚ͯߟ͑Δ͜ͱ͕Ͱ͖Δ:
FA=FA,0+δFA
=FA,0+ (FA,0)′+δFA+ (δFA)′ pb=pb,0+δpb
=pb,0+ (pb,0)′+δpb+ (δpb)′
͜͜Ͱܭଌޡࠩਅʹର͠ेখ͘͞ɺ·ͨͦΕͧΕͷฏۉʹର͠มಈेʹখ͍͞ͷͱߟ͑ɺ ඍখྔʹؔͯ͠ઢܕԽͯ͠ཧ͢Δ͜ͱͱ͢ΔɻҰํɺಈѹqɺҰ༷ྲྀ੩ѹp∞ܭଌ͞ΕΔྔͰͳ͘ɺ ܭଌྔͰ͋Δϐτʔѹp02ٴͼ෩ಎఽΈѹྗpoͱɺͦΕΒ͔Βఆٛ͞ΕΔҰ༷ྲྀMachM ͱΛ༻͍ͯҎԼ
2 誤差評価に関する整理・定式化
ઃܭΛ͢Δঢ়گʹ͓͍ͯॏཁͳཁૉͱͳΔՄೳੑ͕ߟ͑ΒΕΔͨΊɺؾྲྀͷඇҰ༷ੑͷٴ΅ۭ͢ؾྗɺಛʹۭ
ྗϞʔϝϯτͷӨڹΛࢼݧܕʹԠͯ͡దʹ༧ଌ͢Δ͜ͱͷඞཁੑΛ͍ࣔͯ͠Δͱ͍͑ΔɻۭؾྗɾϞʔ ϝϯτͷӨڹΛܾఆ͢Δͱߟ͑ΒΕΔؾྲྀඇҰ༷ੑͷදLdα, β, γͷٯͱͱΒ͑Δ͜ͱ͕Ͱ
͖ɺ෩ಎؾྲྀಈѹͷۭؒύϫʔεϖΫτϧ͕ӨڹධՁͷͨΊʹඞཁͳใͰ͋Δͱߟ͑ΒΕͨɻͦͷͨΊ ؾྲֱྀਖ਼ࢼݧͰಘΒΕ͍ͯΔಈѹͷۭؒύϫʔεϖΫτϧΛͱΓɺͷ͞εέʔϧͱܕදͱͷ
ؔΛߟྀ͢ΔӨڹධՁͷఆࣜԽΛߦ͏͜ͱͱͨ͠ɻ·ͨͦͷධՁ๏ͷݕূͱͯ͠ɺաڈʹHWT1M5෩ಎʹ
͓͍࣮ͯࢪ͞ΕͨܕઃஔҐஔมߋޮՌࢼݧ݁Ռʹ͓͚Δۭྗಛੑมಈྔͱɺ༧ଌ݁ՌͱͷൺֱΛߦ͍ɺͦͷ ଥੑΛ֬ೝ͢Δ͜ͱͱͨ͠ɻ
ۃԻ෩ಎ6ྗܭଌʹ͓͚ΔओཁͳޡࠩཁҼҎ্ʹΑΓධՁͰ͖Δͱߟ͑ΒΕΔ͕ɺ௨ৗͷࢼݧܗଶͰ
Ұൠʹۭؾྗͷখ͍͞ԣɾํಛੑʹؔͯ͠ɺఱടɾܕऔ֯ޡࠩΛ௨ͨ͠ΑΓେ͖ͳۭؾྗͷൃੜ͠
͍ͯΔॎ3ྗͷӨڹ͕ೡΖओཁͳޡࠩཁҼͱͳΓಘΔ͜ͱ͕໌͖ͯͨ͠ɻࢼݧܕऔ࣌ʹൃੜ͢Δ
ܕ࠲ඪܥͱఱട࠲ඪܥʹ͓͚Δऔ֯ޡࠩʹىҼ͢ΔޡࠩධՁʹ͓͍ͯɺࢼݧܕऔঢ়ଶʹ͓͚Δܕ࢟
֯ܭଌʹՃ͑ɺͦͷঢ়ଶʹ͓͚Δఱട࢟֯ܭଌΛߦ͏͜ͱͰɺܕɾఱടؒऔ֯Λਪఆ͢Δඞཁ͕͋Δɻ
ͦͷΑ͏ͳഎܠ͔ΒۃԻ෩ಎͰɺܕʹಇ͘ॏྗΛෳ࢟֯έʔεͰܭଌ͢Δ͜ͱͰɺఱടॲཧʹඞ ཁͳܕॏྔɾॏ৺Ґஔɺఱടग़ྗΦϑηοτྔͷਪఆʹՃ͑ɺఱട࠲ඪܥͷ࢟֯ਪఆ͋Θͤͯߦ͏ํ๏
ΛۙऔΓೖΕ͍ͯΔɻ͜͜Ͱ͜ͷఱടऔ֯ਪఆͷଥੑΛධՁ͢Δ͜ͱΛతʹɺ͜Ε·ͰʹߦΘΕͯ
͖ͨ࣠ରশඪ४ܕࢼݧۭྗಛੑٴͼఱടֱਖ਼݁ՌΛ࠶ධՁ͢Δ͜ͱͱͨ͠ɻͦΕʹ͍ɺ෩ಎࢼݧ࣌ʹఆ
͖͢ܕɾఱടऔ֯ޡࠩͱͯ͠ݟࠐΉ͖ྔΛਪఆ͢Δ͜ͱͱͨ͠ɻ·ͨɺຊߘʹ͓͍ͯɺޡࠩݸʑ ͷܭଌͱਅͱͷࠩΛࢦ͠ɺෆ͔֬͞ܭଌपΓʹਅͷଘࡏ͢ΔൣғΛࢦ͢ͷͱ͢Δɻ
2 ޡࠩධՁʹؔ͢ΔཧɾఆࣜԽ
2.1 ܭଌޡࠩͷۭྗਪఆޡࠩͷ
Ұൠʹɺલ໘࣠ྗCAF ܭଌྔ͋Δ͍ܭଌྔ͔ΒٻΊΒΕΔঢ়ଶྔΛ༻͍ͯҎԼͷΑ͏ʹఆٛ͞Εͯ
͍Δ:
CAF ≡FA−Sb(p∞−pb) qS
͜͜Ͱɺ෩ಎࢼݧʹ͓͚ΔܭଌྔͰ͋Δ࣠ྗFAٴͼϕʔεѹpb͍ͣΕɺҎԼͷΑ͏ʹ‘ਅ’ͱܭଌޡࠩ
ͱ͔Βߏ͞ΕΔͱߟ͑ɺ·ͨਅɺܭଌޡࠩͦΕͧΕฏۉٴͼมಈʹ͚ͯߟ͑Δ͜ͱ͕Ͱ͖Δ:
FA=FA,0+δFA
=FA,0+ (FA,0)′+δFA+ (δFA)′ pb=pb,0+δpb
=pb,0+ (pb,0)′+δpb+ (δpb)′
͜͜Ͱܭଌޡࠩਅʹର͠ेখ͘͞ɺ·ͨͦΕͧΕͷฏۉʹର͠มಈेʹখ͍͞ͷͱߟ͑ɺ ඍখྔʹؔͯ͠ઢܕԽͯ͠ཧ͢Δ͜ͱͱ͢ΔɻҰํɺಈѹqɺҰ༷ྲྀ੩ѹp∞ܭଌ͞ΕΔྔͰͳ͘ɺ ܭଌྔͰ͋Δϐτʔѹp02ٴͼ෩ಎఽΈѹྗpoͱɺͦΕΒ͔Βఆٛ͞ΕΔҰ༷ྲྀMachM ͱΛ༻͍ͯҎԼ
ͷؔࣜʹΑΓ‘ఆٛ’͞ΕΔͷͱߟ͑Δ:
q≡po
γM2 2
1 +γ−1 2 M2
−γ−γ1
p∞≡po
1 +γ−1 2 M2
−γ−1γ
p02
po
=
1 + 2γ
γ+ 1(M2−1)
−γ−11 (γ+ 1)M2 (γ−1)M2+ 2
γ−γ1
͜͜ͰಈѹqɺҰ༷ྲྀ੩ѹp∞ϚοϋM ͱؾྲྀఽΈѹྗpoͷؔͱͯ͠ཧ͓ͯ͠ΓɺߋʹϚοϋ
M ϐτʔѹൺpp02
o ͷΈͷؔͱ͍ͯ͠Δɻ͜ͷఆٛΛ༻͍ΕɺಈѹqɺҰ༷ྲྀ੩ѹp∞ʹؔͯ͠ɺܭଌ
ྔͷ‘ਅ’ٴͼܭଌޡࠩΛ༻͍ͯɺ‘ਅ’ͱܭଌޡࠩͱʹҎԼͷ༷ʹ͚Δ͜ͱ͕Ͱ͖Δ:
q=q,0+δq
≈q,0+ ∂q
∂M(δM) + ∂q
∂po(δpo)
≈q,0+ ∂q
∂M dM dpp02o
δp02
po
+ ∂q
∂po
(δpo) p∞=p∞,0+δp∞
≈p∞,0+∂p∞
∂M dM dpp02o
δp02
po
+∂p∞
∂po
(δpo) δp02
po ≈ 1 po
δp02−p02
p2o δpo
͜ΕΒ͔Βɺલ໘࣠ྗCAFͷܭଌޡࠩͷӨڹʹؔͯ͠ҎԼͷ༷ʹཧ͢Δ͜ͱ͕Ͱ͖Δ:
CAF =CAF,0+δCAF
=FA,0+δFA−Sb(p∞,0+δp∞−pb,0−δpb) (q,0+δq)S
≈CAF,0+δFA
qS +−Sb
qS (δp∞−δpb)−CAFδq q
=CAF,0+δFA
qS + Sb
qSδpb− Sb
qS
∂p∞
∂M +CAF
q
∂q
∂M dM
dpp02o
δp02
po
− Sb
qS
∂p∞
∂po
+CAF
q
∂q
∂po
(δpo)
=CAF,0+AFδFA+Apbδpb+Ap02δp02
po +Apoδpo (1)
͜͜ͰɺCAF,0≡ FA,0−Sbq(p,0∞S,0−pb,0) લ໘࣠ྗͷ‘ਅ’Ͱ͋Γ·ͨɺ δp02
po ≈ 1
poδp02−p02
p2o δpo
AF = 1 qS Apb = Sb
qS Ap02 =−
Sb
qS
∂p∞
∂M +CAF
q
∂q
∂M dM
dpp02o Apo =−Sb
qS
∂p∞
∂po −CAF
q
∂q
∂po
(2)
ͱ͢Δɻ্ࣜதͷ p1o∂M∂q ,∂p∂qo,p1o∂p∂M∞,∂p∂p∞o,ddMp02
po ʹؔͯ͠ɺશؾମؔࣜΑΓҎԼͷ༷ʹٻΊΔ͜ͱ͕Ͱ
͖Δ:
1 po
∂q
∂M =−γMM2−2 2
1 + γ−1 2 M2
−2γ−1γ−1
∂q
∂po
=γM2 2
1 +γ−1 2 M2
−γγ−1
1 po
∂p∞
∂M =−γM
1 + γ−1 2 M2
−2γ−1γ−1
∂p∞
∂po
=
1 + γ−1 2 M2
−γ−γ1
dpp02
o
dM = 4γ γ−1
M2
γ−1−2γM2 + 1 (γ−1)M2+ 2
1 M
p02
po
લ໘࣠ྗCAF ͷޡࠩͷࣜ(1)Ͱɺ࣠ྗਅʹ͓͚Δมಈͱ֤ܭଌޡࠩʹ͓͚Δมಈʹ͓͍ͯ૬ؔ
ؔͷٙΘΕΔΈ߹ΘͤɺϐτʔѹൺԾఆpp02o ͱɺఽΈѹྗܭଌpoʹؔ͢ΔޡࠩͰ͋Γɺσʔλॲཧ ͷࡍʹϐτʔѹൺpp02o Λ‘Ծఆ’͢ΔՕॴ͕ൃੜ͢Δ߹͕͋ΔɻͦͷΑ͏ͳ߹ɺͦͷԾఆͷͨΊʹੜ͡Δޡ
ࠩδpp02
o ͱɺϐτʔѹܭଌޡࠩδp02ɺఽΈѹܭଌޡࠩδpoͱΛ͠ɺಠཱͨ͠ޡࠩཁҼͱධՁ͢Δ͖ͱߟ͑
ΒΕΔɻ࣮ࡍɺଞͷδFA, δpb, δpoͳͲܭଌܥʹ͓͚ΔޡࠩͰ͋Γɺجຊతʹηϯαܥɾॲཧܥͷޡࠩͱ͠
ͯͦͷఔ͕ఆ͞ΕΔͷͰ͋Δ͕ɺಛʹδpp02o ʹؔͯ͠ؾྲྀ࠶ݱੑ෩ಎݻ༗ͷཁૉؚ·ΕΔ͜
ͱʹҙ͕ඞཁͰ͋Δɻδpp02o ෩ಎؾྲྀίΞதʹ͓͚Δ‘දతͳ’pp02o ͷ‘ܭଌޡࠩ’͋Δ͍ਪఆޡࠩͱఆ
͞ΕΔͱߟ͑Δ͖Ͱ͋Δ͕ɺҰൠʹͦͷΑ͏ͳ‘ܭଌ’ࠔͰ͋ΔͨΊɺJAXAۃԻ෩ಎʹ͓͍ͯै
དྷ͔ΒߦΘΕ͍ͯΔΑ͏ʹMachʢʣෆมͰ͋Γϐτʔѹൺ·ͨෆมͰ͋ΔͱԾఆ͢Δ͜ͱɺ࣮
ଌ͞ΕΔϞχλʔ༻ϐτʔѹܭଌ͔Β‘දతͳ’pp02o Λਪఆ͢Δ͜ͱͳͲ͕ߟ͑ΒΕΔɻ͜͜ͰؾྲྀίΞͷ ఆΊΒΕͨҰʹ͓͍ͯϐτʔѹΛϞχλܭଌͦ͠ΕΛجʹ‘දతͳ’pp02o Λਪఆ͠ϐτʔѹൺΛٻΊΔ߹ɺ લड़ͷ௨Γδpp02o ʹɺܭଌܥޡࠩͷଞɺϐτʔѹൺͷۭؒͷͨΊ‘දతͳ’p02ϐτʔѹϞχλʔܭଌ Ґஔʹ͓͚Δϐτʔѹp02sͱඞͣ͠Ұக͠ͳ͍͜ͱΛߟྀ͢Δඞཁ͕͋Δɻͦ͜Ͱɺ‘දత’ͳϐτʔѹ p02ΛɺϐτʔѹϞχλʔ’ܭଌ’p02sͱɺͦͷൺͱͯ͠ઃఆ͢Δapʢap≡p02/p02s=ap+a′pʣͳͲʹ
͚ͯཧ͠ɺ෩ಎؾྲྀͷϐτʔѹޮՌΛධՁ͢Δ͜ͱͱ͢Δɻϐτʔѹൺͷ૬ରతۭ͕ؒ௨෩ຖʹ ෆมͰ͋Εapͷมಈa′p0ͱͳΔͱߟ͑ΒΕΔɻ͜ͷ༷ʹۭؒͷӨڹΛධՁ͠Α͏ͱͨ͠߹
‘දతͳ’ϐτʔѹൺ pp02o ϐτʔѹϞχλʔܭଌpp02so = p02s,0po +δpp02so Λ༻͍ͯɺ p02
po = p02
po
0
+δp02
po
≈ap
p02s
po
0
+δp02s
po
+a′p
p02s
po
0
≈ap
p02s
po
0
+apδp02s
po
+a′pp02s
po
ʹΑΓධՁͰ͖ɺߋʹp02,0≈app02s,0ͱԾఆ͢Εɺpp02
o‘ܭଌ’ʹ͓͚Δ‘ܭଌޡࠩ’δpp02
o ɺ
δp02
po ≈apδp02s
po
+a′pp02s
po
(3) ͱද͢͜ͱ͕Ͱ͖Δɻ͜͜Ͱapؾྲֱྀਖ਼ࢼݧ࣌ͷฏۉΛجʹٻΊΔ͜ͱ͕Ͱ͖ɺa′pؾྲֱྀਖ਼ࢼݧͷ ࡍʹऔಘ͞ΕͨಉҰஅ໘ʹ͓͚Δʢن֨Խͨ͠ʣϐτʔѹൺʹ͓͚Δ࠶ݱੑσʔλ͔Βਪఆ͢Δ͜ͱ͕Ͱ
͖Δͷͱߟ͑ΒΕΔɻ
ͱ͢Δɻ্ࣜதͷ p1o∂M∂q ,∂p∂qo,p1o∂p∂M∞,∂p∂p∞o,ddMp02
po ʹؔͯ͠ɺશؾମؔࣜΑΓҎԼͷ༷ʹٻΊΔ͜ͱ͕Ͱ
͖Δ:
1 po
∂q
∂M =−γMM2−2 2
1 + γ−1 2 M2
−2γ−1γ−1
∂q
∂po
=γM2 2
1 +γ−1 2 M2
−γγ−1
1 po
∂p∞
∂M =−γM
1 + γ−1 2 M2
−2γ−1γ−1
∂p∞
∂po
=
1 + γ−1 2 M2
−γ−γ1
dpp02
o
dM = 4γ γ−1
M2
γ−1−2γM2 + 1 (γ−1)M2+ 2
1 M
p02
po
લ໘࣠ྗCAFͷޡࠩͷࣜ(1)Ͱɺ࣠ྗਅʹ͓͚Δมಈͱ֤ܭଌޡࠩʹ͓͚Δมಈʹ͓͍ͯ૬ؔ
ؔͷٙΘΕΔΈ߹ΘͤɺϐτʔѹൺԾఆpp02o ͱɺఽΈѹྗܭଌpoʹؔ͢ΔޡࠩͰ͋Γɺσʔλॲཧ ͷࡍʹϐτʔѹൺpp02o Λ‘Ծఆ’͢ΔՕॴ͕ൃੜ͢Δ߹͕͋ΔɻͦͷΑ͏ͳ߹ɺͦͷԾఆͷͨΊʹੜ͡Δޡ
ࠩδpp02
o ͱɺϐτʔѹܭଌޡࠩδp02ɺఽΈѹܭଌޡࠩδpoͱΛ͠ɺಠཱͨ͠ޡࠩཁҼͱධՁ͢Δ͖ͱߟ͑
ΒΕΔɻ࣮ࡍɺଞͷδFA, δpb, δpoͳͲܭଌܥʹ͓͚ΔޡࠩͰ͋Γɺجຊతʹηϯαܥɾॲཧܥͷޡࠩͱ͠
ͯͦͷఔ͕ఆ͞ΕΔͷͰ͋Δ͕ɺಛʹδpp02o ʹؔͯ͠ؾྲྀ࠶ݱੑ෩ಎݻ༗ͷཁૉؚ·ΕΔ͜
ͱʹҙ͕ඞཁͰ͋Δɻδpp02o ෩ಎؾྲྀίΞதʹ͓͚Δ‘දతͳ’pp02o ͷ‘ܭଌޡࠩ’͋Δ͍ਪఆޡࠩͱఆ
͞ΕΔͱߟ͑Δ͖Ͱ͋Δ͕ɺҰൠʹͦͷΑ͏ͳ‘ܭଌ’ࠔͰ͋ΔͨΊɺJAXAۃԻ෩ಎʹ͓͍ͯै
དྷ͔ΒߦΘΕ͍ͯΔΑ͏ʹMachʢʣෆมͰ͋Γϐτʔѹൺ·ͨෆมͰ͋ΔͱԾఆ͢Δ͜ͱɺ࣮
ଌ͞ΕΔϞχλʔ༻ϐτʔѹܭଌ͔Β‘දతͳ’pp02o Λਪఆ͢Δ͜ͱͳͲ͕ߟ͑ΒΕΔɻ͜͜ͰؾྲྀίΞͷ ఆΊΒΕͨҰʹ͓͍ͯϐτʔѹΛϞχλܭଌͦ͠ΕΛجʹ‘දతͳ’pp02o Λਪఆ͠ϐτʔѹൺΛٻΊΔ߹ɺ લड़ͷ௨Γδpp02o ʹɺܭଌܥޡࠩͷଞɺϐτʔѹൺͷۭؒͷͨΊ‘දతͳ’p02ϐτʔѹϞχλʔܭଌ Ґஔʹ͓͚Δϐτʔѹp02sͱඞͣ͠Ұக͠ͳ͍͜ͱΛߟྀ͢Δඞཁ͕͋Δɻͦ͜Ͱɺ‘දత’ͳϐτʔѹ p02ΛɺϐτʔѹϞχλʔ’ܭଌ’p02sͱɺͦͷൺͱͯ͠ઃఆ͢Δapʢap ≡p02/p02s=ap+a′pʣͳͲʹ
͚ͯཧ͠ɺ෩ಎؾྲྀͷϐτʔѹޮՌΛධՁ͢Δ͜ͱͱ͢Δɻϐτʔѹൺͷ૬ରతۭ͕ؒ௨෩ຖʹ ෆมͰ͋Εapͷมಈa′p0ͱͳΔͱߟ͑ΒΕΔɻ͜ͷ༷ʹۭؒͷӨڹΛධՁ͠Α͏ͱͨ͠߹
‘දతͳ’ϐτʔѹൺpp02o ϐτʔѹϞχλʔܭଌpp02so = p02s,0po +δpp02so Λ༻͍ͯɺ p02
po = p02
po
0
+δp02
po
≈ap
p02s
po
0
+δp02s
po
+a′p
p02s
po
0
≈ap
p02s
po
0
+apδp02s
po
+a′pp02s
po
ʹΑΓධՁͰ͖ɺߋʹp02,0≈app02s,0ͱԾఆ͢Εɺpp02
o‘ܭଌ’ʹ͓͚Δ‘ܭଌޡࠩ’δpp02
o ɺ
δp02
po ≈apδp02s
po
+a′pp02s
po
(3) ͱද͢͜ͱ͕Ͱ͖Δɻ͜͜Ͱapؾྲֱྀਖ਼ࢼݧ࣌ͷฏۉΛجʹٻΊΔ͜ͱ͕Ͱ͖ɺa′pؾྲֱྀਖ਼ࢼݧͷ ࡍʹऔಘ͞ΕͨಉҰஅ໘ʹ͓͚Δʢن֨Խͨ͠ʣϐτʔѹൺʹ͓͚Δ࠶ݱੑσʔλ͔Βਪఆ͢Δ͜ͱ͕Ͱ
͖Δͷͱߟ͑ΒΕΔɻ
ߋʹϐτʔѹϞχλܭଌྔp02sͷޡࠩͷධՁʹؔͯ͠ɺϐτʔѹൺͷ‘ܭଌ’ϐτʔѹൺͷਅ
p02s
po
oΛ
༻͍ͯɺ
p02s
po = p02s
po
o
+ 1
poδp02s−p02s
p2o δpo
ͱॻ͚ΔͣͰ͋Δɻ͜͜ͰɺҰ༷ྲྀMach͕ෆมͰ͋ΔͱԾఆ͢Δैདྷͷํ๏ʹ͓͍ͯͪΖΜɺϐτʔ ѹϞχλʕܭଌʹΑΓ֤௨෩ʹ͓͍ͯҰ༷ྲྀMachΛٻΊΑ͏ͱ͢Δ৽ͨͳํ๏ʹ͓͍ͯɺϐτʔѹܭଌ
࣌ʹ͓͚Δଌఆ͕௨෩தҰఆͰ͋ΔͱԾఆ͢ΔҎ্ɺϐτʔѹൺԾఆྔ͕ଘࡏ͢ΔɻͦͷϐτʔѹൺԾఆʹ ΑΔ‘ޡࠩ’ΛݟੵΔඞཁ͕͋ΓɺԾఆ͍ͯ͠ΔϐτʔѹൺෆมΛp
02s
po
Aͱ͢Εɺ͜ͷԾఆྔͰ͋Δ p
02s
po
Aͱ‘ਅ’p
02s
po
oͱͷ͕ࠩ͜ͷ߹ධՁ͢Δ͖‘ޡࠩ’Ͱ͋Δͱߟ͑ΒΕΔͷͰɺ δp02s
po = p02s
po
A
− p02s
po
0
= p02s
po
A−p02s
po
+ 1 po
δp02s−p02s
p2o δpo
ͦͷͨΊɺϐτʔѹൺԾఆʹ͏ޡࠩཁҼͱͯ͠
δ∗p02s
po ≡ p02s
po
A−p02s
po
(4) Λఆٛ͢Εɺ‘දతͳ’ϐτʔѹൺޡࠩδpp02o ͷࣜ(3)ɺ
δp02
po ≈apδ∗p02s
po
+ap
po
δp02s−p02sap
p2o δpo+a′pp02s
po
(5) Ͱ͋ΔɻͦͷͨΊɺࣜ(1)ͱΈ߹ΘͤΔ͜ͱͰɺ
CAF ≈CAF,0+AFδFA+Apbδpb+apAp02δ∗p02s
po +Ap02
ap
poδp02s
+
Apo−Ap02
p02sap
p2o
δpo+a′p p02s
po
Ap02
(6)
͜͜Ͱ֤߲ಉ࢜ͷ૬ؔͳ͍ͷͱߟ͑Δ͜ͱ͕Ͱ͖ΔΑ͏ʹͳͬͨͨΊɺલ໘࣠ྗ‘ܭଌ݁Ռ’ͷฏۉ
ٴͼඪ४ภࠩσCAF ɺ
CAF ≈CAF,0+AFδFA+Apbδpb+Ap02apδ∗p02s
po +Ap02
ap
poδp02s+
Apo −Ap02
p02sap
p2o
δpo (7) σ2CAF ≈σ2CAF,0+A2Fσ2δFA+A2pbσ2δpb
+ (Ap02ap)2σ2δ∗p02s po +
Ap02
ap
po
2
σδp202s+
Apo−Ap02
p02sap
p2o 2
σδp2o+ p02s
po
2
A2p02σa2p (8)
ͱද͢͜ͱ͕Ͱ͖Δɻࣜ(7),(8)ͰδCAF =CAF−CAF,0͍ΘΏΔจݙ[6]Ͱཧ͞ΕΔbiasޡࠩʹ૬͠ɺ δ′CAF precisionޡࠩʹ૬͢Δͱߟ͑ΒΕΔɻ͜͜ͰσCAF,0࣠ྗਅͷมಈΛҙຯ͓ͯ͠Γɺઌʹ
‘ఆٛ’͞ΕͨM, q, p∞͕ཧతʹఆٛ͞ΕΔMachɺಈѹɺ੩ѹͱҰக͠ɺ·ͨؾྲྀ͕Ұ༷Ͱ͋Γɺ͔ͭRe
ɺM ͕େ͖͘มԽ͠ͳ͍ݶΓຊདྷ0ͱͳΔͱظ͞ΕΔྔͰ͋ΔɻͦͷͨΊɺKΛแׅɺKB
ΛbiasޡࠩʹରԠ͢Δแׅʹ૬͢Δͱͯ͠ɺ෩ಎࢼݧʹ͓͚Δෆ͔֬͞ʢbiasޡ֤߲ࠩͷແ૬ؔ
ΛԾఆͯ͠ʣ KB2
CAF−CAF,02
+K2σC2AF σCAF,0= 0ΛԾఆͯ͠ҎԼͷ௨ΓධՁ͢Δ͜ͱ͕Ͱ͖Δɿ UC2AF ≈A2FUδF2 A+A2pbUδp2b+ (Ap02ap)2Uδ2∗p02s
po +
Ap02
ap
po
2
Uδp202s
+
Apo−Ap02
p02sap
p2o 2
Uδp2o+ p02s
po
2
A2p02Ua2p
(9)
͜͜Ͱɺ
UδF2A =KB2δFA
2+K2σ2δFA, Uδp2b =KB2δpb
2+K2σδp2b, Uδ2∗p02s
po =KB2δ∗p02s
po 2
+K2σδ2∗p02s po
Uδp202s =KB2δp02s
2+K2σδp202s, Uδp2o =KB2δpo
2+K2σ2δpo, Ua2p=K2σ2ap
(10)
ͱ͢Δɻ
͜͜ͰɺҰ༷ྲྀMachΛࢼݧΩϟϯϖʔϯɺRunʹ߆ΘΒͣৗʹෆมͰ͋ΔͱԾఆ͢Δ߹ͱɺ௨෩ຖʹϐ τʔѹϞχλʕܭଌʹΑΓҰ༷ྲྀMachΛਪఆ͢Δ߹ͱͰͷޡࠩධՁͷҧ͍ɺࣜ(4)ͷධՁͷҧ͍
ʹΑΓੜ͡ΔɻৗʹҰ༷ྲྀMachΛෆมͱԾఆ͢Δ߹ɺԾఆp
02s
po
A୯Ұͷෆมྔͱ͠ɺࢼݧΩϟ ϯϖʔϯɾ௨෩RunΛލ͍ͰͦͷԾఆ͔Βͷࠩͷฏۉɾඪ४ภࠩΛٻΊΔඞཁ͕͋Δͷʹର͠ɺ௨෩ຖʹ ϐτʔѹϞχλʕܭଌʹΑΓҰ༷ྲྀMachΛ௨෩ຖʹਪఆ͢Δख๏ʹ͓͍ͯɺ௨෩ຖʹઃఆ͞ΕͨԾఆ
p
02s
po
Aͱͷ͕ࠩ௨෩தʹͲͷఔมԽ͠͏Δ͔ΛධՁ͢Δඞཁ͕͋Δɻ
2.2 ؾྲྀͷඇҰ༷ੑ͕ٴ΅͢ 6 ྗܭଌͷӨڹ
ؾྲྀʹඇҰ༷ੑ͕͋Δ߹ɺ‘දతͳ’p02Λਪఆ͢ΔࡍͷޡࠩͷධՁΛલઅͰݕ౼͕ͨ͠ɺඇҰ༷ͳؾྲྀ
ʹΑΔۭؾྗͷมಈɺલઅͷཧͰۭྗ‘ਅ’(CAF,0)ͷมಈͱͯ͋͠ΒΘΕΔ͜ͱʹͳΔɻ͔͠͠
Ұൠʹ෩ಎࢼݧʹΑΓಘΒΕΔۭྗಛੑσʔλɺҰ༷ͳؾྲྀதʹ͓͍ͯൃੜ͢ΔۭؾྗΛਪఆ͢ΔͨΊͷ
ͷͰ͋Δ͜ͱΛ೦಄ʹஔ͘ͱɺؾྲྀͷඇҰ༷ੑʹΑΓੜ͍ͯ͡ΔՄೳੑͷ͋ΔྔΛਪఆ͠໌ࣔ͢Δ͜ͱ͕༗ӹ Ͱ͋Δͱߟ͑ΒΕΔɻͦͷඇҰ༷ੑͷޮՌࢼݧܕҐஔΛ෩ಎؾྲྀதʹ͘·ͳ͘มԽͤͨ͞ͱ͖ʹಘΒΕΔ
ۭྗྗɾϞʔϝϯτͷมಈͱͯ͋͠ΒΘΕΔͷͱߟ͑Δ͖Ͱ͋Δɻͦ͜Ͱɺ͞εέʔϧ͕LdͰ͋Δ Α͏ͳඇҰ༷ੑͷɺ͞εέʔϧ͕LmͰ͋Δܕ্ʹಇۭ͘ؾྗͷޮՌͷݟੵΓΛɺہॴಈѹqfͱہ ॴCpٴͼද໘ੵdsͱͷੵͰہॴۭؾྗ͕ද͞ΕΔͱ͍͏ϞσϧԽʹΑΓߦ͏͜ͱͱͨ͠ɻ͜ͷہॴ
ɺද໘ѹྗ͕ಈѹʹൺྫ͢Δͱ͍͏Ծఆʹجͮ͘ͷͰ͋Δ͕ɺಈѹʹൺҰ༷ྲྀ੩ѹ͕ۃʹখ͘͞ͳΔ ۃԻྲྀʹ͓͍ͯۙࣅతʹѹྗͱ߹க͢ΔͷͰ͋Γɺͦͷൣғʹ͓͍ͯԾఆͷଥੑ֬ೝͰ͖
Δɻ·ͣہॴಈѹΛܭଌྔͰ͋Δϐτʔѹྗ͔Βਪఆ͢Δඞཁ͕͋Δ͕ɺ͜͜ͰۃԻྲྀͷ༷ʹൺֱ
తߴMachͰɺϐτʔѹͷMachґଘੑ͕খ͘͞ͳΔ͜ͱ͔Βɺϐτʔѹͱಈѹͷൺ΄΅Ұఆͱۙ
ࣅͰ͖Δ:
p02
q = p02
po
po
p∞ 2
γM2 →2γ−γ−1γ
γ+ 1 2
γ+1γ−1
≈1.84 (M → ∞) (11)
͜ΕʹΑΓɺ෩ಎֱਖ਼ࢼݧͰಘΒΕ͍ͯΔϐτʔѹൺ͔ΒಈѹΛਪఆ͢Δ͜ͱ͕Ͱ͖Δɻ
͜͜Ͱɺզʑͷڵຯͷରͱ͢Δͷͱɺྫ͑ؾྲྀίΞྖҬͷҰxoͱܕ࠲ඪݪ͕Ұக͢Δࢼݧ
ܕʹಇۭ͘ؾྗΛߟ͑ͨͱ͖ʹɺxoͷมԽͱͱʹͦͷܕʹՃΘΔۭؾྗf(xo)ͷมԽ͢ΔྔͰ͋Γɺͦ
Ε
σ2f ≈(i,j,k) 1 Vo
Vo
fx(xo)−fx
2
fy(xo)−fx2 fz(xo)−fx2
dvxo
≈(i,j,k) 1 Vo
αo̸=0
|Fx(αo)|2
|Fy(αo)|2
|Fz(αo)|2
dαo
2π d
βo
2π
dγo
2π
≈(i,j,k)
k,l,m
NF1xk,l,mN2N3
2
NF1yk,l,mN2N3
2
NF1zk,l,mN2N3
2