第五章、 研究結果與討論
5.3 噴印研究
5.3.3 壓力分佈圖
我們從壓力分佈圖發現,Case1 獲得了最大的瞬間壓力將近 300MPa,Case2 獲得最大的瞬間壓力不到 200 MPa,Case3 所獲得的 壓力曲線最溫和都不超過100MPa,如圖 5.16。
case1
case2
case3
圖 5.16 壓力分佈圖
5.3.4 分子個數分佈圖
我們想更了解此噴印究竟有多少水分子抵達板子上,所以做了水 分子個數對位置的做圖,如圖5.17
case1
case2
case3
圖5.17 水分子分佈圖
我們可以發現噴嘴吸附的分子明顯變少,且數量在 case1 約有 80 個水分子,在 case2 約有 120 個水分子,在 case3 約有 100 個水分 子,沒有特別的規律性;但板子上的水分子,就幾乎與活塞前進距離 成正比,如圖5.18,在 case1 約有 4153 個水分子於板子上,在 case2 約有1913 個水分子於板子上,在 case3 約有 903 個水分子於板子上,
這是一個極大的好消息,表示藉由這次模擬我們能做到定量的掌控,
但要注意越多的量,需要越大的瞬間壓力給予分子飛行的能量。
圖5.18 水分子個數與推進距離作圖
第六章、結論與未來展望
研究中探討不同溫度噴流過程及不同瞬時推速的噴印過程,由實 驗結果可知,我們由瞬時圖中液滴的形成、液滴形狀、分子蒸發現象、
衛星液滴的產生、打在板子上的圖形、及流場,各項分析顯示出,在 溫度較低時,是最適合做精密計算的奈米噴流加工。
當 噴 流 系 統 溫 度 為 T=278(K) 時 , 可 看 出 其 蒸 發 現 象 較 T=298,348(K)時相對較低。此外液滴打在板子上的情況也是最優良。
且較不易產生衛星液滴,十分利於精密加工。
所以接著噴印的模擬過程就選定溫度為 278K,重大發現,只要 有足夠的趨動壓力,抵達板子上的水分子會幾乎與活塞前進距離成正 比,因分子於噴頭吸附的量變少。
期待在未來利用噴墨的加工技術越來越高科技且微小化,可以經 由本研究中的模擬系統預先嘗試,降低成本,減少失誤及錯誤估計的 損失,在研究中假設噴流系統中成分為純水,實際上噴流系統中成分 都較為複雜,所以希望未來可以模擬出更多樣化的物質,讓我們的模 擬系統更加接近實際情況,得到更加準確的訊息。
希望我們能在未來全球都全力投入奈米科技的研發時,給予人 類對微加工的摸索及了解能有所幫助。
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Appendix A 減縮單位轉換
由於防止計算數值過小而造成電腦計算溢位的問題,因此通常都 會採用減縮單位來處理計算數值。
本研究中模擬的基本單位為水分子中的O,因此所有減縮單位皆 以此為基本單位,主要設定的部分為氧分子的質量、特徵長度與能 量,以及其他衍生的參數性質,如表A.1 所示。
表A.1 減縮單位換算表 減縮單位相關參數數值 SI 制單位
Mass m 1.8x10-2(kg/mole) Length σ 3.166x10-10(m)
Energy ε 648.923(J/mole) Time τ 1.667x10-12(s)
Density 1(g/cm3)
Pressure 2.04966x1032(Pa/mole) Temperature 78.113(K)