So far we have discussed temperature change due to heat transfer. No temperature change occurs from heat transfer if ice melts and becomes liquid water (i.e., during a phase change). For example, consider water dripping from icicles melting on a roof warmed by the Sun. Conversely, water freezes in an ice tray cooled by lower-temperature surroundings.

Energy is required to melt a solid because the cohesive bonds between the molecules in the solid must be broken apart such that, in the liquid, the molecules can move around at comparable kinetic energies; thus, there is no rise in temperature. Similarly, energy is needed to vaporize a liquid, because molecules in a liquid interact with each other via attractive forces. There is no temperature change until a phase change is complete. The temperature of a cup of soda initially at $\mathrm{0\xba}\text{C}$ stays at $\mathrm{0\xba}\text{C}$ until all the ice has melted. Conversely, energy is released during freezing and condensation, usually in the form of thermal energy. Work is done by cohesive forces when molecules are brought together. The corresponding energy must be given off (dissipated) to allow them to stay together [link].

The energy involved in a phase change depends on two major factors: the number and strength of bonds or force pairs. The number of bonds is proportional to the number of molecules and thus to the mass of the sample. The strength of forces depends on the type of molecules. The heat $Q$ required to change the phase of a sample of mass $m$ is given by

where the latent heat of fusion, ${L}_{\text{f}}$, and latent heat of vaporization, ${L}_{\text{v}}$, are material constants that are determined experimentally. See ([link]).

Latent heat is measured in units of J/kg. Both ${L}_{\text{f}}$ and ${L}_{\text{v}}$ depend on the substance, particularly on the strength of its molecular forces as noted earlier. ${L}_{\text{f}}$ and ${L}_{\text{v}}$ are collectively called latent heat coefficients. They are *latent*, or hidden, because in phase changes, energy enters or leaves a system without causing a temperature change in the system; so, in effect, the energy is hidden. [link] lists representative values of ${L}_{\text{f}}$ and ${L}_{\text{v}}$, together with melting and boiling points.

The table shows that significant amounts of energy are involved in phase changes. Let us look, for example, at how much energy is needed to melt a kilogram of ice at $\mathrm{0\xba}\text{C}$ to produce a kilogram of water at $0\xb0\text{C}$. Using the equation for a change in temperature and the value for water from [link], we find that $Q={\text{mL}}_{\text{f}}=(1\text{.}0\phantom{\rule{0.25em}{0ex}}\text{kg})(\text{334}\phantom{\rule{0.25em}{0ex}}\text{kJ/kg})=\text{334}\phantom{\rule{0.25em}{0ex}}\text{kJ}$ is the energy to melt a kilogram of ice. This is a lot of energy as it represents the same amount of energy needed to raise the temperature of 1 kg of liquid water from $\mathrm{0\xba}\text{C}$ to $\text{79}\text{.}\mathrm{8\xba}\text{C}$. Even more energy is required to vaporize water; it would take 2256 kJ to change 1 kg of liquid water at the normal boiling point ($\text{100\xba}\text{C}$ at atmospheric pressure) to steam (water vapor). This example shows that the energy for a phase change is enormous compared to energy associated with temperature changes without a phase change.

L_{f} |
L_{v} |
|||||

Substance |
Melting point (ºC) |
kJ/kg |
kcal/kg |
Boiling point (°C) |
kJ/kg |
kcal/kg |

Helium | −269.7 | 5.23 | 1.25 | −268.9 | 20.9 | 4.99 |

Hydrogen | −259.3 | 58.6 | 14.0 | −252.9 | 452 | 108 |

Nitrogen | −210.0 | 25.5 | 6.09 | −195.8 | 201 | 48.0 |

Oxygen | −218.8 | 13.8 | 3.30 | −183.0 | 213 | 50.9 |

Ethanol | −114 | 104 | 24.9 | 78.3 | 854 | 204 |

Ammonia | −75 | 108 | −33.4 | 1370 | 327 | |

Mercury | −38.9 | 11.8 | 2.82 | 357 | 272 | 65.0 |

Water | 0.00 | 334 | 79.8 | 100.0 | 2256 At $\text{37}\text{.}\mathrm{0\xba}\text{C}$ (body temperature), the heat of vaporization ${L}_{\mathrm{v}}$ for water is 2430 kJ/kg or 580 kcal/kg |
539 At $\text{37.}\mathrm{0\xba}\text{C}$ (body temperature), the heat of vaporization ${L}_{\mathrm{v}}$ for water is 2430 kJ/kg or 580 kcal/kg |

Sulfur | 119 | 38.1 | 9.10 | 444.6 | 326 | 77.9 |

Lead | 327 | 24.5 | 5.85 | 1750 | 871 | 208 |

Antimony | 631 | 165 | 39.4 | 1440 | 561 | 134 |

Aluminum | 660 | 380 | 90 | 2450 | 11400 | 2720 |

Silver | 961 | 88.3 | 21.1 | 2193 | 2336 | 558 |

Gold | 1063 | 64.5 | 15.4 | 2660 | 1578 | 377 |

Copper | 1083 | 134 | 32.0 | 2595 | 5069 | 1211 |

Uranium | 1133 | 84 | 20 | 3900 | 1900 | 454 |

Tungsten | 3410 | 184 | 44 | 5900 | 4810 | 1150 |

Phase changes can have a tremendous stabilizing effect even on temperatures that are not near the melting and boiling points, because evaporation and condensation (conversion of a gas into a liquid state) occur even at temperatures below the boiling point. Take, for example, the fact that air temperatures in humid climates rarely go above $\text{35}\text{.}\mathrm{0\xba}\text{C}$, which is because most heat transfer goes into evaporating water into the air. Similarly, temperatures in humid weather rarely fall below the dew point because enormous heat is released when water vapor condenses.

We examine the effects of phase change more precisely by considering adding heat into a sample of ice at $-\text{20\xba}\text{C}$ ([link]). The temperature of the ice rises linearly, absorbing heat at a constant rate of $0\text{.}\text{50cal/g}\cdot \xba\text{C}$ until it reaches $\mathrm{0\xba}\text{C}$. Once at this temperature, the ice begins to melt until all the ice has melted, absorbing 79.8 cal/g of heat. The temperature remains constant at $\mathrm{0\xba}\text{C}$ during this phase change. Once all the ice has melted, the temperature of the liquid water rises, absorbing heat at a new constant rate of $1\text{.}\text{00cal/g}\cdot \xba\text{C}$. At $\text{100\xba}\text{C}$, the water begins to boil and the temperature again remains constant while the water absorbs 539 cal/g of heat during this phase change. When all the liquid has become steam vapor, the temperature rises again, absorbing heat at a rate of $0\text{.}\text{482cal/g}\cdot \xba\text{C}$.

Water can evaporate at temperatures below the boiling point. More energy is required than at the boiling point, because the kinetic energy of water molecules at temperatures below $\text{100\xba}\text{C}$ is less than that at $\text{100\xba}\text{C}$, hence less energy is available from random thermal motions. Take, for example, the fact that, at body temperature, perspiration from the skin requires a heat input of 2428 kJ/kg, which is about 10 percent higher than the latent heat of vaporization at $\text{100\xba}\text{C}$. This heat comes from the skin, and thus provides an effective cooling mechanism in hot weather. High humidity inhibits evaporation, so that body temperature might rise, leaving unevaporated sweat on your brow.

Three ice cubes are used to chill a soda at $\text{20\xba}\text{C}$ with mass ${m}_{\mathrm{soda}}=\text{0.25}\text{kg}$. The ice is at $\mathrm{0\xba}\text{C}$ and each ice cube has a mass of 6.0 g. Assume that the soda is kept in a foam container so that heat loss can be ignored. Assume the soda has the same heat capacity as water. Find the final temperature when all ice has melted.

**Strategy**

The ice cubes are at the melting temperature of $\mathrm{0\xba}\text{C}$. Heat is transferred from the soda to the ice for melting. Melting of ice occurs in two steps: first the phase change occurs and solid (ice) transforms into liquid water at the melting temperature, then the temperature of this water rises. Melting yields water at $\mathrm{0\xba}\text{C}$, so more heat is transferred from the soda to this water until the water plus soda system reaches thermal equilibrium,

The heat transferred to the ice is ${Q}_{\text{ice}}={m}_{\text{ice}}{L}_{\text{f}}+{m}_{\text{ice}}{c}_{\text{W}}({T}_{\text{f}}-\mathrm{0\xba}\text{C})$. The heat given off by the soda is ${Q}_{\text{soda}}={m}_{\text{soda}}{c}_{\text{W}}({T}_{\text{f}}-\text{20\xba}\text{C})$. Since no heat is lost, ${Q}_{\text{ice}}=-{Q}_{\text{soda}}$, so that

Bring all terms involving ${T}_{\text{f}}$ on the left-hand-side and all other terms on the right-hand-side. Solve for the unknown quantity ${T}_{\text{f}}$:

**Solution**

- Identify the known quantities. The mass of ice is ${m}_{\text{ice}}=3\text{\xd7}6.0\text{g}=0\text{.}\text{018}\text{kg}$ and the mass of soda is ${m}_{\text{soda}}=0\text{.}\text{25}\text{kg}$.
- Calculate the terms in the numerator:
${m}_{\text{soda}}{c}_{\mathrm{W}}\left(\text{20\xba}\text{C}\right)=\left(0\text{.25kg}\right)\left(\text{4186J/kg}\cdot \xba\text{C}\right)\left(\text{20\xba}\text{C}\right)=\text{20,930J}$
and

${m}_{\text{ice}}{L}_{\text{f}}=\left(0\text{.}\text{018}\text{kg}\right)\left(\text{334,000}\text{J/kg}\right)\text{=6012}\text{J.}$ - Calculate the denominator:
$\left({m}_{\text{soda}}+{m}_{\text{ice}}\right){c}_{\text{W}}=\left(0\text{.}\text{25}\text{kg+0}\text{.}\text{018 kg}\right)\left(\text{4186 K/}(\text{kg}\cdot \xba\text{C}\right)\text{=1122 J/\xba}\text{C}\text{.}$
- Calculate the final temperature:
${T}_{\text{f}}=\frac{\text{20},\text{930J}-\text{6012J}}{\text{1122J/\xba}\text{C}}=\text{13\xba}\text{C.}$

**Discussion**

This example illustrates the enormous energies involved during a phase change. The mass of ice is about 7 percent the mass of water but leads to a noticeable change in the temperature of soda. Although we assumed that the ice was at the freezing temperature, this is incorrect: the typical temperature is $-\mathrm{6\xba}\text{C}$. However, this correction gives a final temperature that is essentially identical to the result we found. Can you explain why?

We have seen that vaporization requires heat transfer to a liquid from the surroundings, so that energy is released by the surroundings. Condensation is the reverse process, increasing the temperature of the surroundings. This increase may seem surprising, since we associate condensation with cold objects—the glass in the figure, for example. However, energy must be removed from the condensing molecules to make a vapor condense. The energy is exactly the same as that required to make the phase change in the other direction, from liquid to vapor, and so it can be calculated from $Q={\text{mL}}_{\text{v}}$.

Sublimation is the transition from solid to vapor phase. You may have noticed that snow can disappear into thin air without a trace of liquid water, or the disappearance of ice cubes in a freezer. The reverse is also true: Frost can form on very cold windows without going through the liquid stage. A popular effect is the making of “smoke” from dry ice, which is solid carbon dioxide. Sublimation occurs because the equilibrium vapor pressure of solids is not zero. Certain air fresheners use the sublimation of a solid to inject a perfume into the room. Moth balls are a slightly toxic example of a phenol (an organic compound) that sublimates, while some solids, such as osmium tetroxide, are so toxic that they must be kept in sealed containers to prevent human exposure to their sublimation-produced vapors.

All phase transitions involve heat. In the case of direct solid-vapor transitions, the energy required is given by the equation $Q={\mathrm{mL}}_{\text{s}}$, where ${L}_{\text{s}}$ is the heat of sublimation, which is the energy required to change 1.00 kg of a substance from the solid phase to the vapor phase. ${L}_{\text{s}}$ is analogous to ${L}_{\text{f}}$ and ${L}_{\text{v}}$, and its value depends on the substance. Sublimation requires energy input, so that dry ice is an effective coolant, whereas the reverse process (i.e., frosting) releases energy. The amount of energy required for sublimation is of the same order of magnitude as that for other phase transitions.

The material presented in this section and the preceding section allows us to calculate any number of effects related to temperature and phase change. In each case, it is necessary to identify which temperature and phase changes are taking place and then to apply the appropriate equation. Keep in mind that heat transfer and work can cause both temperature and phase changes.

# Problem-Solving Strategies for the Effects of Heat Transfer

*Examine the situation to determine that there is a change in the temperature or phase. Is there heat transfer into or out of the system?*When the presence or absence of a phase change is not obvious, you may wish to first solve the problem as if there were no phase changes, and examine the temperature change obtained. If it is sufficient to take you past a boiling or melting point, you should then go back and do the problem in steps—temperature change, phase change, subsequent temperature change, and so on.*Identify and list all objects that change temperature and phase.**Identify exactly what needs to be determined in the problem (identify the unknowns).*A written list is useful.*Make a list of what is given or what can be inferred from the problem as stated (identify the knowns).**Solve the appropriate equation for the quantity to be determined (the unknown).*If there is a temperature change, the transferred heat depends on the specific heat (see [link]) whereas, for a phase change, the transferred heat depends on the latent heat. See [link].*Substitute the knowns along with their units into the appropriate equation and obtain numerical solutions complete with units.*You will need to do this in steps if there is more than one stage to the process (such as a temperature change followed by a phase change).*Check the answer to see if it is reasonable: Does it make sense?*As an example, be certain that the temperature change does not also cause a phase change that you have not taken into account.

# Summary

- Most substances can exist either in solid, liquid, and gas forms, which are referred to as “phases.”
- Phase changes occur at fixed temperatures for a given substance at a given pressure, and these temperatures are called boiling and freezing (or melting) points.
- During phase changes, heat absorbed or released is given by:
$Q=\text{mL,}$
where $L$ is the latent heat coefficient.

# Conceptual Questions

Heat transfer can cause temperature and phase changes. What else can cause these changes?

How does the latent heat of fusion of water help slow the decrease of air temperatures, perhaps preventing temperatures from falling significantly below $\text{0\xbaC}$, in the vicinity of large bodies of water?

What is the temperature of ice right after it is formed by freezing water?

If you place $\text{0\xbaC}$ ice into $\text{0\xbaC}$ water in an insulated container, what will happen? Will some ice melt, will more water freeze, or will neither take place?

What effect does condensation on a glass of ice water have on the rate at which the ice melts? Will the condensation speed up the melting process or slow it down?

In very humid climates where there are numerous bodies of water, such as in Florida, it is unusual for temperatures to rise above about $\text{35\xba}\text{C}(\text{95\xba}\text{F})$. In deserts, however, temperatures can rise far above this. Explain how the evaporation of water helps limit high temperatures in humid climates.

In winters, it is often warmer in San Francisco than in nearby Sacramento, 150 km inland. In summers, it is nearly always hotter in Sacramento. Explain how the bodies of water surrounding San Francisco moderate its extreme temperatures.

Putting a lid on a boiling pot greatly reduces the heat transfer necessary to keep it boiling. Explain why.

Freeze-dried foods have been dehydrated in a vacuum. During the process, the food freezes and must be heated to facilitate dehydration. Explain both how the vacuum speeds up dehydration and why the food freezes as a result.

When still air cools by radiating at night, it is unusual for temperatures to fall below the dew point. Explain why.

In a physics classroom demonstration, an instructor inflates a balloon by mouth and then cools it in liquid nitrogen. When cold, the shrunken balloon has a small amount of light blue liquid in it, as well as some snow-like crystals. As it warms up, the liquid boils, and part of the crystals sublimate, with some crystals lingering for awhile and then producing a liquid. Identify the blue liquid and the two solids in the cold balloon. Justify your identifications using data from [link].

# Problems & Exercises

How much heat transfer (in kilocalories) is required to thaw a 0.450-kg package of frozen vegetables originally at $\mathrm{0\xba}\text{C}$ if their heat of fusion is the same as that of water?

35.9 kcal

A bag containing $\mathrm{0\xba}\text{C}$ ice is much more effective in absorbing energy than one containing the same amount of $\mathrm{0\xba}\text{C}$ water.

- How much heat transfer is necessary to raise the temperature of 0.800 kg of water from $\mathrm{0\xba}\text{C}$ to $\text{30}\text{.}\mathrm{0\xba}\text{C?}$
- How much heat transfer is required to first melt 0.800 kg of $\mathrm{0\xba}\text{C}$ ice and then raise its temperature?
- Explain how your answer supports the contention that the ice is more effective.

(a) How much heat transfer is required to raise the temperature of a 0.750-kg aluminum pot containing 2.50 kg of water from $\text{30}\text{.}\mathrm{0\xba}\text{C}$ to the boiling point and then boil away 0.750 kg of water? (b) How long does this take if the rate of heat transfer is 500 W $1\text{watt=1}\text{joule/second}(\text{1W=1J/s})$?

(a) 591 kcal

(b) $4\text{.}\text{94}\times {\text{10}}^{3}\phantom{\rule{0.25em}{0ex}}\text{s}$

The formation of condensation on a glass of ice water causes the ice to melt faster than it would otherwise. If 8.00 g of condensation forms on a glass containing both water and 200 g of ice, how many grams of the ice will melt as a result? Assume no other heat transfer occurs.

On a trip, you notice that a 3.50-kg bag of ice lasts an average of one day in your cooler. What is the average power in watts entering the ice if it starts at $\mathrm{0\xba}\text{C}$ and completely melts to $\mathrm{0\xba}\text{C}$ water in exactly one day $\text{1watt=1joule/second}\phantom{\rule{0.25em}{0ex}}(\text{1W=1J/s})$?

13.5 W

On a certain dry sunny day, a swimming pool’s temperature would rise by $1\text{.}\text{50\xba}\text{C}$ if not for evaporation. What fraction of the water must evaporate to carry away precisely enough energy to keep the temperature constant?

(a) How much heat transfer is necessary to raise the temperature of a 0.200-kg piece of ice from $-\text{20.}\mathrm{0\xba}\text{C}$ to $\text{130\xba}\text{C}$, including the energy needed for phase changes?

(b) How much time is required for each stage, assuming a constant 20.0 kJ/s rate of heat transfer?

(c) Make a graph of temperature versus time for this process.

(a) 148 kcal

(b) 0.418 s, 3.34 s, 4.19 s, 22.6 s, 0.456 s

In 1986, a gargantuan iceberg broke away from the Ross Ice Shelf in Antarctica. It was approximately a rectangle 160 km long, 40.0 km wide, and 250 m thick.

(a) What is the mass of this iceberg, given that the density of ice is $\text{917}{\text{kg/m}}^{3}$?

(b) How much heat transfer (in joules) is needed to melt it?

(c) How many years would it take sunlight alone to melt ice this thick, if the ice absorbs an average of $\text{100}{\text{W/m}}^{2}$, 12.00 h per day?

How many grams of coffee must evaporate from 350 g of coffee in a 100-g glass cup to cool the coffee from $\text{95}\text{.}\mathrm{0\xba}\text{C}$ to $\text{45}\text{.}\mathrm{0\xba}\text{C}$? You may assume the coffee has the same thermal properties as water and that the average heat of vaporization is 2340 kJ/kg (560 cal/g). (You may neglect the change in mass of the coffee as it cools, which will give you an answer that is slightly larger than correct.)

33.0 g

(a) It is difficult to extinguish a fire on a crude oil tanker, because each liter of crude oil releases $2\text{.}\text{80}\times {\text{10}}^{7}\phantom{\rule{0.25em}{0ex}}\text{J}$ of energy when burned. To illustrate this difficulty, calculate the number of liters of water that must be expended to absorb the energy released by burning 1.00 L of crude oil, if the water has its temperature raised from $\text{20}\text{.}\mathrm{0\xba}\text{C}$ to $\text{100\xba}\text{C}$, it boils, and the resulting steam is raised to $\text{300\xba}\text{C}$. (b) Discuss additional complications caused by the fact that crude oil has a smaller density than water.

(a) 9.67 L

(b) Crude oil is less dense than water, so it floats on top of the water, thereby exposing it to the oxygen in the air, which it uses to burn. Also, if the water is under the oil, it is less efficient in absorbing the heat generated by the oil.

The energy released from condensation in thunderstorms can be very large. Calculate the energy released into the atmosphere for a small storm of radius 1 km, assuming that 1.0 cm of rain is precipitated uniformly over this area.

To help prevent frost damage, 4.00 kg of $\mathrm{0\xba}\text{C}$ water is sprayed onto a fruit tree.

(a) How much heat transfer occurs as the water freezes?

(b) How much would the temperature of the 200-kg tree decrease if this amount of heat transferred from the tree? Take the specific heat to be $3\text{.35kJ/kg}\cdot \xba\text{C}$, and assume that no phase change occurs.

a) 319 kcal

b) $2\text{.}\text{00\xba}\text{C}$

A 0.250-kg aluminum bowl holding 0.800 kg of soup at $\text{25}\text{.}\mathrm{0\xba}\text{C}$ is placed in a freezer. What is the final temperature if 377 kJ of energy is transferred from the bowl and soup, assuming the soup’s thermal properties are the same as that of water? Explicitly show how you follow the steps in Problem-Solving Strategies for the Effects of Heat Transfer.

A 0.0500-kg ice cube at $-\text{30}\text{.}\mathrm{0\xba}\text{C}$ is placed in 0.400 kg of $\text{35}\text{.}\mathrm{0\xba}\text{C}$ water in a very well-insulated container. What is the final temperature?

$\text{20.6\xba}\text{C}$

If you pour 0.0100 kg of $\text{20}\text{.}\mathrm{0\xba}\text{C}$ water onto a 1.20-kg block of ice (which is initially at $-\text{15}\text{.}\mathrm{0\xba}\text{C}$), what is the final temperature? You may assume that the water cools so rapidly that effects of the surroundings are negligible.

Indigenous people sometimes cook in watertight baskets by placing hot rocks into water to bring it to a boil. What mass of $\text{500\xba}\text{C}$ rock must be placed in 4.00 kg of $\text{15}\text{.}\mathrm{0\xba}\text{C}$ water to bring its temperature to $\text{100\xba}\text{C}$, if 0.0250 kg of water escapes as vapor from the initial sizzle? You may neglect the effects of the surroundings and take the average specific heat of the rocks to be that of granite.

4.38 kg

What would be the final temperature of the pan and water in Calculating the Final Temperature When Heat Is Transferred Between Two Bodies: Pouring Cold Water in a Hot Pan if 0.260 kg of water was placed in the pan and 0.0100 kg of the water evaporated immediately, leaving the remainder to come to a common temperature with the pan?

In some countries, liquid nitrogen is used on dairy trucks instead of mechanical refrigerators. A 3.00-hour delivery trip requires 200 L of liquid nitrogen, which has a density of $\text{808}{\text{kg/m}}^{3}$.

(a) Calculate the heat transfer necessary to evaporate this amount of liquid nitrogen and raise its temperature to $3\text{.}\text{00\xba}\text{C}$. (Use ${c}_{\mathrm{p}}$ and assume it is constant over the temperature range.) This value is the amount of cooling the liquid nitrogen supplies.

(b) What is this heat transfer rate in kilowatt-hours?

(c) Compare the amount of cooling obtained from melting an identical mass of $\mathrm{0\xba}\text{C}$ ice with that from evaporating the liquid nitrogen.

(a) $1\text{.}\text{57}\times {\text{10}}^{4}\phantom{\rule{0.25em}{0ex}}\text{kcal}$

(b) $\text{18}\text{.3 kW}\cdot \text{h}$

(c) $1\text{.}\text{29}\times {\text{10}}^{4}\phantom{\rule{0.25em}{0ex}}\text{kcal}$

Some gun fanciers make their own bullets, which involves melting and casting the lead slugs. How much heat transfer is needed to raise the temperature and melt 0.500 kg of lead, starting from $\text{25}\text{.}\mathrm{0\xba}\text{C}$?

- College Physics
- Preface
- Introduction: The Nature of Science and Physics
- Kinematics
- Introduction to One-Dimensional Kinematics
- Displacement
- Vectors, Scalars, and Coordinate Systems
- Time, Velocity, and Speed
- Acceleration
- Motion Equations for Constant Acceleration in One Dimension
- Problem-Solving Basics for One-Dimensional Kinematics
- Falling Objects
- Graphical Analysis of One-Dimensional Motion

- Two-Dimensional Kinematics
- Dynamics: Force and Newton's Laws of Motion
- Introduction to Dynamics: Newton’s Laws of Motion
- Development of Force Concept
- Newton’s First Law of Motion: Inertia
- Newton’s Second Law of Motion: Concept of a System
- Newton’s Third Law of Motion: Symmetry in Forces
- Normal, Tension, and Other Examples of Forces
- Problem-Solving Strategies
- Further Applications of Newton’s Laws of Motion
- Extended Topic: The Four Basic Forces—An Introduction

- Further Applications of Newton's Laws: Friction, Drag, and Elasticity
- Uniform Circular Motion and Gravitation
- Work, Energy, and Energy Resources
- Introduction to Work, Energy, and Energy Resources
- Work: The Scientific Definition
- Kinetic Energy and the Work-Energy Theorem
- Gravitational Potential Energy
- Conservative Forces and Potential Energy
- Nonconservative Forces
- Conservation of Energy
- Power
- Work, Energy, and Power in Humans
- World Energy Use

- Linear Momentum and Collisions
- Statics and Torque
- Rotational Motion and Angular Momentum
- Introduction to Rotational Motion and Angular Momentum
- Angular Acceleration
- Kinematics of Rotational Motion
- Dynamics of Rotational Motion: Rotational Inertia
- Rotational Kinetic Energy: Work and Energy Revisited
- Angular Momentum and Its Conservation
- Collisions of Extended Bodies in Two Dimensions
- Gyroscopic Effects: Vector Aspects of Angular Momentum

- Fluid Statics
- Introduction to Fluid Statics
- What Is a Fluid?
- Density
- Pressure
- Variation of Pressure with Depth in a Fluid
- Pascal’s Principle
- Gauge Pressure, Absolute Pressure, and Pressure Measurement
- Archimedes’ Principle
- Cohesion and Adhesion in Liquids: Surface Tension and Capillary Action
- Pressures in the Body

- Fluid Dynamics and Its Biological and Medical Applications
- Introduction to Fluid Dynamics and Its Biological and Medical Applications
- Flow Rate and Its Relation to Velocity
- Bernoulli’s Equation
- The Most General Applications of Bernoulli’s Equation
- Viscosity and Laminar Flow; Poiseuille’s Law
- The Onset of Turbulence
- Motion of an Object in a Viscous Fluid
- Molecular Transport Phenomena: Diffusion, Osmosis, and Related Processes

- Temperature, Kinetic Theory, and the Gas Laws
- Heat and Heat Transfer Methods
- Thermodynamics
- Introduction to Thermodynamics
- The First Law of Thermodynamics
- The First Law of Thermodynamics and Some Simple Processes
- Introduction to the Second Law of Thermodynamics: Heat Engines and Their Efficiency
- Carnot’s Perfect Heat Engine: The Second Law of Thermodynamics Restated
- Applications of Thermodynamics: Heat Pumps and Refrigerators
- Entropy and the Second Law of Thermodynamics: Disorder and the Unavailability of Energy
- Statistical Interpretation of Entropy and the Second Law of Thermodynamics: The Underlying Explanation

- Oscillatory Motion and Waves
- Introduction to Oscillatory Motion and Waves
- Hooke’s Law: Stress and Strain Revisited
- Period and Frequency in Oscillations
- Simple Harmonic Motion: A Special Periodic Motion
- The Simple Pendulum
- Energy and the Simple Harmonic Oscillator
- Uniform Circular Motion and Simple Harmonic Motion
- Damped Harmonic Motion
- Forced Oscillations and Resonance
- Waves
- Superposition and Interference
- Energy in Waves: Intensity

- Physics of Hearing
- Electric Charge and Electric Field
- Introduction to Electric Charge and Electric Field
- Static Electricity and Charge: Conservation of Charge
- Conductors and Insulators
- Coulomb’s Law
- Electric Field: Concept of a Field Revisited
- Electric Field Lines: Multiple Charges
- Electric Forces in Biology
- Conductors and Electric Fields in Static Equilibrium
- Applications of Electrostatics

- Electric Potential and Electric Field
- Introduction to Electric Potential and Electric Energy
- Electric Potential Energy: Potential Difference
- Electric Potential in a Uniform Electric Field
- Electrical Potential Due to a Point Charge
- Equipotential Lines
- Capacitors and Dielectrics
- Capacitors in Series and Parallel
- Energy Stored in Capacitors

- Electric Current, Resistance, and Ohm's Law
- Circuits, Bioelectricity, and DC Instruments
- Magnetism
- Introduction to Magnetism
- Magnets
- Ferromagnets and Electromagnets
- Magnetic Fields and Magnetic Field Lines
- Magnetic Field Strength: Force on a Moving Charge in a Magnetic Field
- Force on a Moving Charge in a Magnetic Field: Examples and Applications
- The Hall Effect
- Magnetic Force on a Current-Carrying Conductor
- Torque on a Current Loop: Motors and Meters
- Magnetic Fields Produced by Currents: Ampere’s Law
- Magnetic Force between Two Parallel Conductors
- More Applications of Magnetism

- Electromagnetic Induction, AC Circuits, and Electrical Technologies
- Introduction to Electromagnetic Induction, AC Circuits and Electrical Technologies
- Induced Emf and Magnetic Flux
- Faraday’s Law of Induction: Lenz’s Law
- Motional Emf
- Eddy Currents and Magnetic Damping
- Electric Generators
- Back Emf
- Transformers
- Electrical Safety: Systems and Devices
- Inductance
- RL Circuits
- Reactance, Inductive and Capacitive
- RLC Series AC Circuits

- Electromagnetic Waves
- Geometric Optics
- Vision and Optical Instruments
- Wave Optics
- Introduction to Wave Optics
- The Wave Aspect of Light: Interference
- Huygens's Principle: Diffraction
- Young’s Double Slit Experiment
- Multiple Slit Diffraction
- Single Slit Diffraction
- Limits of Resolution: The Rayleigh Criterion
- Thin Film Interference
- Polarization
- *Extended Topic* Microscopy Enhanced by the Wave Characteristics of Light

- Special Relativity
- Introduction to Quantum Physics
- Atomic Physics
- Introduction to Atomic Physics
- Discovery of the Atom
- Discovery of the Parts of the Atom: Electrons and Nuclei
- Bohr’s Theory of the Hydrogen Atom
- X Rays: Atomic Origins and Applications
- Applications of Atomic Excitations and De-Excitations
- The Wave Nature of Matter Causes Quantization
- Patterns in Spectra Reveal More Quantization
- Quantum Numbers and Rules
- The Pauli Exclusion Principle

- Radioactivity and Nuclear Physics
- Medical Applications of Nuclear Physics
- Particle Physics
- Frontiers of Physics
- Atomic Masses
- Selected Radioactive Isotopes
- Useful Information
- Glossary of Key Symbols and Notation