4.3** Do the same as in Problem 4.2, but for the force F = (-y, x) and for the three paths joining and Q shown in Figure 4.24(b) and defined as follows: (a) This path goes straight from P = (1, 0) the origin and then straight to Q = (0, 1). (b) This is a straight line from P to Q. (Write y as a funct of x and rewrite the integral as an integral over x.) (c) This is a quarter-circle centered on the orig (Write x and y in polar coordinates and rewrite the integral as an integral over p.)
4.3** Do the same as in Problem 4.2, but for the force F = (-y, x) and for the three paths joining and Q shown in Figure 4.24(b) and defined as follows: (a) This path goes straight from P = (1, 0) the origin and then straight to Q = (0, 1). (b) This is a straight line from P to Q. (Write y as a funct of x and rewrite the integral as an integral over x.) (c) This is a quarter-circle centered on the orig (Write x and y in polar coordinates and rewrite the integral as an integral over p.)
Algebra and Trigonometry (6th Edition)
6th Edition
ISBN:9780134463216
Author:Robert F. Blitzer
Publisher:Robert F. Blitzer
ChapterP: Prerequisites: Fundamental Concepts Of Algebra
Section: Chapter Questions
Problem 1MCCP: In Exercises 1-25, simplify the given expression or perform the indicated operation (and simplify,...
Related questions
Question
4.3

Transcribed Image Text:4.3** Do the same as in Problem 4.2, but for the force F = (-y, x) and for the three paths joining P
and Q shown in Figure 4.24(b) and defined as follows: (a) This path goes straight from P = (1, 0) to
the origin and then straight to Q = (0, 1). (b) This is a straight line from P to Q. (Write y as a function
of x and rewrite the integral as an integral over x.) (c) This is a quarter-circle centered on the origin.
(Write x and y in polar coordinates and rewrite the integral as an integral over p.)
4.4** A particle of mass m is moving on a frictionless horizontal table and is attached to a massless
string, whose other end passes through a hole in the table, where I am holding it. Initially the particle is
moving in a circle of radius ro with angular velocity wo, but I now pull the string down through the hole
until a length r remains between the hole and the particle. (a) What is the particle's angular velocity
now? (b) Assuming that I pull the string so slowly that we can approximate the particle's path by a
1
Q
(a)
a
a
0
b
(b)
Figure 4.24 (a) Problem 4.2. (b) Problem 4.3
P
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