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第五章 結論與未來研究方向
根據 EWMA 管制圖之管制界限應隨時間變動,藉由縮減前期管制界限的範圍,
改善傳統 EWMA 管制圖對於製程初期異常的敏感度,本研究所採用的變動管制界限 形式,為各期管制統計量分配的 α/2 和 1 − α/2 分位數,由於各期管制統計量分配 型態未知,因此利用傅立葉級數近似各期管制統計量之累積分佈函數,進而求得分位 數作為變動管制界限。研究結果顯示,此種變動管制界限對於提升管制圖在製程初期 偵測能力之效果,主要取決於加權常數 λ,一般而言,加權常數越小對於改善製程初 期之偵測能力效果越好,且縮減的抽樣次數固定,例如:當 λ = 0.05 時,在各種參 數設定和不同偏移程度之下,大約皆能縮減 5 次抽樣即能偵測出製程為失控狀態,因 此能有效提升對於製程微小偏移的偵測能力;而偏移幅度較大時,能縮減抽樣次數至 1 ∼ 2 次,若以縮減效果而言,隨樣本數或 α 越大效果越好,且當製程為厚尾分配 (如:雙指數分配) 時,對於改善製程初期偵測能力的效果更為明顯。
針對後續研究方向以及待改進方法,在此提出以下建議:
1. 以往無母數 EWMA 管制圖相關文獻中,大多未提及變動管制界限之效果,例 如:Hackl and Ledolter (1991) 所提出對於單一觀測值,給定一組參考樣本 Y1, Y2, · · · , Yg−1 計算其標準化排序
Rt = 2
g (R∗t − g + 1 2 ) Rt∗ = 1 +
g−1
X
i=1
I(Xt> Yi)
其中,Rt 為 iid 離散型均勻分配,依據 Rt 建構 EWMA 管制程序監控製程中 心值,其乃利用模擬方法求得適當固定管制界限,因此可將本文所提出之方法運 用於此,建構變動管制界限並探討其效果。
2. Steiner (1999) 認為當 EWMA 管制圖之管制界限隨時間變動僅相似於快速起
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始反應的性質,欲使 EWMA 管制圖具備快速起始反應之性質,進而提出藉由 調整項 FIRadj = 1 − (1 − f∗)1+a(k−1) 縮減前期管制界限以提升偵測能力,則新 的管制界限如下:
U CLk = µ0+ L σX 1 − (1 − f∗)1+a(k−1) r λ
2 − λ(1 − (1 − λ)2k) LCLk = µ0− L σX 1 − (1 − f∗)1+a(k−1)
r λ
2 − λ(1 − (1 − λ)2k) 其中 f∗ 及 a 為可調整常數,Steiner 認為大約 20 個觀察值之後快速起始反應 就沒有什麼效果,使得 a = (−2/log(1 − f∗) − 1)/19,而 f∗ 其目的即為調整 起始值介於目標值及管制界限之間,大多使用 0.5。本研究僅提出無母數管制 圖建構變動管制界限之方法及觀察結果,因此可進一步研究管制參數 α 變動方 式,以達快速起始反應之功能。
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偶數。則可根據 composite Simpson’s rule 誤差公式求得| I | =
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第 II 部分,為估計機率誤差
| II | ≤ hn 3
Aˆzn−1− Azn−1 max
ξ∈(0,x)f0(ξ)
(1 + 4 + 2 + · · · + 4 + 1)
= x
Aˆzn−1 − Azn−1
max
ξ∈(0,x)f0(ξ)
‧
‧
cos(nx) cos(mx) dx
+ bn Z π
−π
sin(nx) cos(mx) dx
其中 sin(mx)
cos(nx) cos(mx) dx =
Theorem 1 (Fourier convergence). 已知 f 為一分段平滑的週期函數,則
(SNf )(x) = f (x+) + f (x−)