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- (void)setCp1Y:(CGFloat)f { cp1Y = MAX(MIN(f, 1.0), 0.0); [self setNeedsDisplay:YES]; } - (void)setCp2X:(CGFloat)f { cp2X = MAX(MIN(f, 1.0), 0.0); [self setNeedsDisplay:YES]; } - (void)setCp2Y:(CGFloat)f { cp2Y = MAX(MIN(f, 1.0), 0.0); [self setNeedsDisplay:YES]; } - (id)initWithFrame:(NSRect)frame { self = [super initWithFrame:frame]; if (self) { // Initialization code here. myBounds = NSMakeRect(-0.1, -0.1, 1.2, 1.2); [self setBounds:myBounds]; } return self; } - (void)setFrameSize:(NSSize)newSize { [super setFrameSize:newSize]; [self setBounds:myBounds]; } - (void)drawRect:(NSRect)rect { // Drawing code here. } @end

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Are the units correct Dimensional analysis on the units confirms the number of free electrons per cubic centimeter Is the magnitude realistic One would expect a large number of electrons in a cubic centimeter

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1 Zinc, with a density of 713 g/cm3 and an atomic mass of 6537 g/mol, has two free electrons per atom How many free electrons are there in each cubic centimeter of zinc 2 Silver has 1 free electron per atom Use Appendix D and determine the number of free electrons in 1 cm3 of silver 3 Gold has 1 free electron per atom Use Appendix D and determine the number of free electrons in 1 cm3 of gold 4 Aluminum has 3 free electrons per atom Use Appendix D and determine the number of free electrons in 1 cm3 of aluminum 5 The tip of the Washington Monument was made of 2835 g of aluminum because it was a rare and costly metal in the 1800s Use problem 4 and determine the number of free electrons in the tip of the Washington Monument

In an insulating material, the valence band is filled to capacity and the conduction band is empty As shown in Figure 29-4, an electron must gain a large amount of energy to go to the next energy level In an insulator, the lowest energy level in the conduction band is 5 10 eV above the highest energy level in the valence band, as shown in Figure 29-4a There is at least a 5-eV gap of energies that no electrons can possess

Although electrons have some kinetic energy as a result of their thermal energy, the average kinetic energy of electrons at room temperature is not sufficient for them to jump the forbidden gap If a small electric field is placed across an insulator, almost no electrons gain enough energy to reach the conduction band, so there is no current Electrons in an insulator must be given a large amount of energy to be pulled into the conduction band As a result, the electrons in an insulator tend to remain in place, and the material does not conduct electricity

Note that we don t stop at just synthesizing the accessors for our properties. We actually implement setters for each of our properties, and in each we enforce a limited range on the input value, making it fit in the range from 0.0 to 1.0. We also mark the window as dirty, forcing the system to redraw it whenever a property changes.

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