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According to the previous discussion of gases and solids, a hot object has more thermal energy than a similar cold object, as shown in Figure 12-2 This means that, as a whole, the particles in a hot object have greater thermal energy than the particles in a cold object This does not mean that all the particles in an object have exactly the same amount of energy; they have a wide range of energies However, the average energy of the particles in a hot object is higher than the average energy of the particles in a cold object To understand this, consider the heights of students in a twelfth-grade class Although the students heights vary, you can calculate the average height of the students in the class This average is likely to be greater than the average height of students in a ninth-grade class, even though some ninth-grade students may be taller than some twelfth-grade students



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Figure 12-2 Particles in a hot object have greater kinetic and potential energies than particles in a cold object do





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Temperature Temperature depends only on the average kinetic energy of the particles in the object Because temperature depends on average kinetic energy, it does not depend on the number of atoms in an object To understand this, consider two blocks of steel The first block has a mass of 1 kg, and the second block has a mass of 2 kg If the 1-kg block is at the same temperature as the 2-kg block, the average kinetic energy of the particles in each block is the same However, the 2-kg block has twice the mass of the 1-kg block Hence, the 2-kg block has twice the amount of particles as the 1kg block Thus, the total amount of kinetic energy of the particles in the 2kg block is twice that of the 1-kg mass Total kinetic energy is divided by the total number of particles in an object to calculate its average kinetic energy Therefore, the thermal energy in an object is proportional to the number of particles in it Temperature, however, is not dependent on the number of particles in an object

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Which are true (Choose all that apply) A Compilation fails B An exception is thrown at runtime C Loop #1 will run most of its iterations before Loop #2 D Loop #2 will run most of its iterations before Loop #1 E There is no way to predict which loop will mostly run first

Before Thermal Equilibrium Hot object (A) Cold object (B)

When an RF transmitter is feeding a half-wave antenna, positive and negative charges move back and forth along the antenna (Figs 5-9 and 5-10) The first picture shows the position of the charges at some arbitrary time, T0 The RF charges being observed are at the ends of the antenna, and there is a maximum difference in potential between the ends, A and B The remaining illustrations show the instantaneous positions of the charges at regular intervals of 225 throughout a complete cycle To the right of each instantaneous position of the charges are curves representing the current and voltage at that particular time for any point on the antenna For example, at time T0, the positive and negative charges are at points A and B on the antenna The voltage between these points represents a maximum difference of potential The current, being 90 out of phase in respect to the voltage, is everywhere zero These distribution curves are standing waves derived in the same manner as those covered in the previous paragraph The next illustration shows the position of the charges at time T1 The standing wave of current is a relative maximum at the center of the antenna This current loop has nodes that remain at the ends of the antenna, and it is, therefore, 90 out of phase with the standing wave of voltage At T2 and T3, the charges move closer together, and the standing wave of voltage slowly decreases in amplitude Conversely, the current loop increases in magnitude When the charges meet after 90 of the RF cycle (T4), the effect is that of having the positive and negative charges cancel The voltage loop accordingly is zero everywhere on the antenna, and the current loop rises to its maximum value, unimpeded by any charge on the antenna At time T5, the charges have passed each other, each charge having moved past the center point of the antenna The polarity of the voltage loops is reversed, and they build up in the opposite direction, keeping the node always at the center point of the antenna The reversal of polarity is shown in the charge positions at T3, T4, and.

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