Selected Exercises for the Feynman Lectures on Physics by Richard Feynman, Et Al. Chapter 27 Quantum Behavior: Waves, Particles, and Photons – Detailed Work by James Pate Williams, Jr. BA, BS, MSwE, PhD

Computerized solutions to Exercises 27.3 to 27.6:

Exercise 27.3 Main

Exercise 27.3

Exercise 27.4

Exercise 27.5

Exercise 27.6

Partial source code for the preceding C# application:

Exercise 27.3

Detailed solutions to Exercises 27.3 to 27.7 in a Portable Document File (PDF):

Feynman Exercises Chapter 27

 

Selected Exercises for the Feynman Lectures on Physics by Richard Feynman, Et Al. Chapter 4 Kinematics – Detailed Work by James Pate Williams, Jr. BA, BS, MSwE, PhD

Exercises 4.1 to 4.7:

Feynman Exercises Chapter 04

Computer solution output of Exercise 4.6:

Exercise 4.6

C# source code for the computer solution of Exercise 4.6, sorry about the naming confusion in the file:

Exercise 4.6

Computer solution of Exercise 4.7 using a velocity square drag function (velocity retardation function is the term used in exterior ballistics). I wrote a baseball ballistics program based on my numeric work (Runge-Kutta Fifth Order) and analytic solutions found in the paper:

Click to access 04-LAJPE-782_Chudinov.pdf

The first picture is the main form interface for the program with the parameters initial velocity in meters per second and the initial angle which is in degrees. We use a velocity of 25 meters per second which is approximately 56 miles per hour and the angle is 90 degrees to the horizontal which is throwing the ball straight up into the air.

BB Main Exercise 4.7

First we show the classical ballistics without atmospheric drag:

BB CB Exercise 4.7

Next we show the invalid (due to a singularity in one of the equations) analytic and numeric solutions:

BB AN Exercise 4.7

The analytic solution is not valid for theta0 = 90 degrees. The numeric solution shows a time to apogee of 2.28 seconds and time of flight 4.66 seconds. The difference is 4.66 – 2.28 seconds = 2.38 seconds so the time to return from apogee is greater than the time to reach apogee. The analytic solution becomes valid at 88 degrees of inclination.

BB AN 88 Exercise 4.7

Next we move onto an inclination of 15 degrees:

BB CB 15 Exercise 4.7

BB AN 15 Exercise 4.7

Finally for the maximum distance traveled by the ball classically we select 45 degrees:

BB CB 45 Exercise 4.7

BB AN 45 Exercise 4.7

We find that with drag the maximum distance traveled (range) is achieved around 43 degrees:

BB CB 43 Exercise 4.7

BB AN 43 Exercise 4.7

 

 

Exercises for the Feynman Lectures on Physics by Richard Feynman, Et Al. Chapter 38 Differential Calculus of Vector Fields – Detailed Work by James Pate Williams, Jr. BA, BS, MSwE, PhD

Feynman Exercises Chapter 38

Exercises for the Feynman Lectures on Physics by Richard Feynman, Et Al. Chapter 36 Fourier Analysis of Waves– Detailed Computer Work by James Pate Williams, Jr. BA, BS, MSwE, PhD

Exercise 36.1 (a) Graph
f(x) = 1 for all x contained in the interval [0, 6.28]
Exercise 36.1 (a) Coefficients
Fourier coefficients for a constant function f(x) = 1

 

 

Exercise 36.1 (b) Graph
f(x) = sin x for all x in the interval [0, 6.28]
Exercise 36.1 (b) Coefficients
Fourier coefficients for f(x) = sin x for all x in [0, 6.28]
Exercise 36.2 Graph
Graph of the Fourier Series Approximation to the Square Wave with the Gibb’s Overshoot Phenomena Clearly Present

 

Exercise 36.2 Coefficients
Fourier Series Coefficients for the Square Wave

Exercise 36.2 (a)

Exercise 36.2 (b)

Exercise 36.2 (c)

 

 

Exercise 36.3 Graph
Graph of the Fourier Series Approximation to the Triangle Wave

 

Exercise 36.3 Coefficients
Fourier Coefficients for the Triangle Wave

Exercise 36.3 (b) (1)

Exercise 36.3 (b) (2)

 

Exercise 36.4

 

Exercise 36.6 Graph
Graph of the Fourier Series Approximation to a Saw-Tooth Wave

 

Exercise 36.6 Coefficients
Fourier Coefficients for the Saw-Tooth Wave

 

Exercise 36.8 Graph
Graph of the Fourier Approximation to the Rectified Sine Wave

 

Exercise 36.8 Coefficients
Fourier Series Coefficients for the Rectified Sine Wave