John Taylor Classical Mechanics Chapter 5, Problem 29

In summary: Bt/2m(C1cos(w1t)+ C2sin(w1t))In summary, the problem involves an undamped oscillator with a period of 1 second. When weak damping is added, the amplitude of oscillation drops by 50 percent in one period. The period of the damped oscillations is defined as the time between successive maxima and is calculated as t1=2pi/w1, where w1 is the angular frequency. The equation for a damped oscillator is x(t)=e^-Bt/2m(C1cos(w1t)+ C2sin(w1t)). The values of B and t1 can be calculated as B=0.110
  • #1
karmonkey98k
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John Taylor "Classical Mechanics" Chapter 5, Problem 29

Homework Statement


An undamped oscillator has period t(0)=1 second. When weak damping is added, it is found that the amplitude of oscillation drops by 50 percent in one period r1. (the period of the damped oscillations defined as time between successive maxima t1=2pi/w1) (w1=angular frequency). How big is B (damping constant) compared to w(0)? What is t1?


Homework Equations


For undamped osc: x(t)=C1e^iw(o)t+C2e^-iw(o)t
For underdamping: w1=root(w(o)^2-B^2)
for weak damping: B<w(o)


The Attempt at a Solution


well, the answers are t1=1.006 sec and B=0.110w(o). But I don't know how they arrived at those specific answers. How could you get those two numbers? May sound too general, but I just don't know how you could get numerical answers in general in this prob, from what we have.
 
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  • #2
karmonkey98k said:

Homework Statement


An undamped oscillator has period t(0)=1 second. When weak damping is added, it is found that the amplitude of oscillation drops by 50 percent in one period r1. (the period of the damped oscillations defined as time between successive maxima t1=2pi/w1) (w1=angular frequency). How big is B (damping constant) compared to w(0)? What is t1?

Homework Equations


For undamped osc: x(t)=C1e^iw(o)t+C2e^-iw(o)t
For underdamping: w1=root(w(o)^2-B^2)
for weak damping: B<w(o)

What is the equation for x(t) in case of a damped oscillator?

ehild
 

1. What is the title of Chapter 5 in "John Taylor Classical Mechanics"?

The title of Chapter 5 is "Motion in a Non-inertial Frame".

2. What is the specific problem addressed in Problem 29 of Chapter 5?

Problem 29 deals with the Coriolis force and its effects on a ball thrown from a rotating platform.

3. Is this problem relevant to real-world situations?

Yes, the Coriolis force is a real phenomenon that can be observed in everyday situations, such as the rotation of the Earth and its effect on weather patterns.

4. What are the main concepts covered in Chapter 5?

The main concepts in Chapter 5 include non-inertial frames of reference, the Coriolis force, and the centrifugal force.

5. Can this chapter be understood without prior knowledge of classical mechanics?

No, Chapter 5 assumes a basic understanding of classical mechanics and builds upon concepts introduced in earlier chapters of the book.

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