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dealing with the changes, additions, and deletions in these types that inevitably occur during the development cycle. Because nullability is one of a number of attributes of any particular database field, and because dealing with changes in nullability is no different from dealing with name and data type changes, the idea of making a value type nullable in C# when it isn t nullable in the database just in case the underlying database schema changes makes little sense. If the nullability of a field changes, simply use the same established change process you d use if an int field changed to a long field. Using nullable types unnecessarily is detrimental to performance memory is wasted storing a Boolean value for each nullable type and processor cycles are wasted checking this Boolean when calculations involving the nullable type are performed. Don t mix nullability concepts within an assembly. If you re currently using special values, System.Data.SqlTypes types, or third-party nullability libraries to deal with nullability, don t introduce Nullable<T> or C# nullable types without migrating existing code to use these new features.

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Similar to cohesive forces, adhesive forces are electromagnetic attractive forces that act between particles of different substances If a glass tube with a small inner diameter is placed in water, the water rises inside the tube The water rises because the adhesive forces between glass and water molecules are stronger than the cohesive forces between water molecules This phenomenon is called capillary action The water continues to rise until the weight of the water that is lifted balances the total adhesive force between the glass and water molecules If the radius of the tube increases, the volume and the weight of the water will increase proportionally faster than the surface area of the tube Thus, water is lifted higher in a narrow tube than in a wider one Capillary action causes molten wax to rise in a candle s wick and water to move up through the soil and into the roots of plants When a glass tube is placed in a beaker of water, the surface of the water climbs the outside of the tube, as shown in Figure 13-9a The adhesive forces between the glass molecules and water molecules are greater than the cohesive forces between the water molecules In contrast, the cohesive forces between mercury molecules are greater than the adhesive forces between the mercury and glass molecules, so the liquid does not climb the tube These forces also cause the center of the mercury s surface to depress, as shown in Figure 13-9b

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Plants Cohesive forces in liquids actually allow them to be stretched just like rubber bands This stretching is difficult to achieve in the laboratory, but it is common in plants The strength of the cohesive forces in water keeps the water from breaking and bubbling as it goes through the plant tissue to the leaves If not for these forces, trees could not grow higher than about 10 m

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When Experiment 1 is functioning correctly, we re ready to use the same setup to actually drive a motor Any small DC motor that will run at 9V will be fine for Experiment 2 The following motors from my local Radio Shack both did the job: RS #273-255 (9V to 12V) and RS #273-256 (9V to 18V) Of course, larger motors will drain your 9V battery faster, so for this experiment you may want to use the smallest 9V motor you can find If you happen to have a 12V motor and battery, you can substitute those as well The setup for the remaining three experiments is the same; simply disconnect the auxiliary LED breadboard from the L298 board and connect your motor to the right motor screw terminals on the L298 board (However, don t dismantle the auxiliary breadboard yet; we re going to use it again in the next chapter) When the motor is powered, it will tend to jump around a bit, so you will either need to hold onto it or attach it to something that is heavy enough to hold it in place I used a heavy piece of steel from my shop (see the photo in Figure 17-8) When your setup is complete, run the Exp1&2DirectionTestbas program again; the motor should change direction each time a new subroutine is executed If your motor doesn t come to a full stop between each direction change, you may want to lengthen the wait statement in the stopp subroutine until you find a value that works

Why does a puddle of water disappear on a hot, dry day As you learned in 12, the particles in a liquid are moving at random speeds If a fast-moving particle can break through the surface layer, it will escape from the liquid Because there is a net downward cohesive force at the surface, however, only the most energetic particles escape This escape of particles is called evaporation

Figure 13-9 Water climbs the outside wall of this glass tube (a), while the mercury is depressed by the rod (b) The forces of attraction between mercury atoms are stronger than any adhesive forces between the mercury and the glass

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