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loaded. The int variable rc contains either OK or ERR depending on the function s success or failure.

setSession(s)

Figure 5.3. A typical SEM image of the PPAPE colloidal spheres obtained from the water suspension, which was prepared by dropping water into the THF solution until 50% (vol%) and then quenching the structures with excess of water and dialyzing against water for 3 days. The initial concentration of PPAPE in THF is 1.0 mg/mL. Source: From Li et al., 2006a.



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1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 #include <ncurses.h> #define FILENAME windump int main(void) { int r; initscr(); addstr( Press Enter to restore the screen\n ); refresh(); getch(); /* restore the window from disk */ r = scr_set(FILENAME); if( r == ERR) addstr( Error reading window file: press Enter\n ); wrefresh(curscr); getch(); endwin(); return 0; }

Sample output is the same as for scr_restore().





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of the structure units bearing azo chromophores among the total units. For other azo polymers, uniform colloidal spheres can also be obtained by this method. The formation and size of the colloidal spheres depend on the molecular structures and preparation conditions such as the initial concentration of the polymer in THF, the water content in the medium, and the water-dropping rate. As the polymers studied are of different types and have polydispersity in the molecular weight and DF, it is dif cult to give a quantitative relationship to correlate the polymer structures with the colloid size and formation details. As a general tendency, CWC decreases as the molecular weight and hydrophobicity increase, and the colloid size increases as the hydrophobicity increases. The in uence of the polymer structure can be better understood after discussing the colloid formation mechanism in Section 5.3.3. The effect of the preparation conditions on the colloid formation and size is discussed herein by using PEAPE (DF=49.9%) as a typical example. The initial concentration of the polymer in THF has signi cant in uence on the CWC and size of the colloidal spheres. The CWC can be obtained by measuring the variation curves of the scattered light intensity of the samples versus the water contents. The inset of Fig. 5.4 shows a typical plot of the scattered light intensity against the water content. The scattered light intensity is almost zero and remains unchanged before CWC. When the water content reaches CWC, ca. 25% (vol%) in this case, the scattered light intensity increases sharply. For the same polymer, CWC depends on the initial concentration of the polymer in THF. For different azo polymers studied by us, CWC is observed to linearly decrease as

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someMethod(x) x := getValue("x") incr(x) storeValue("x", x) afterInvocation(i,c)

14, scr_dump(), scr_restore(), scr_set()

scrl()

Scattered light intensity (a.u.)

int scrl(int n); int wscrl(WINDOW *win, int n);

24.09.2004 21:08

n is an int value indicating the number of lines to scroll the window. When n is positive, n lines are scrolled up; when n is negative, n lines are scrolled down. Refer to the w entry later in this appendix for information on the win argument.

4000 3000 2000 1000 0 0 10 20 30 40 Water content (%)

Scrolling must be enabled for the window for scroll() to function properly. See scrollok(). Scrolling does not affect the cursor s location in the window. If the cursor is on row 5, then scrolling the text in the window up or down moves only the text; the cursor remains at row 5. When text is scrolled up, blank lines are inserted at the bottom of the window; lines at the top are removed. When text is scrolled down, blanks lines are inserted at the top of the window, with lines at the bottom being removed.

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30 CWC (v%)

scrl(1);

wscrl(viewer,-3);

3.0

1 2 3 4 5 6 7 8 9 10 11 #include <ncurses.h> int main(void) { int ch; initscr(); scrollok(stdscr,TRUE); keypad(stdscr,TRUE); noecho();

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