Download presentation
Presentation is loading. Please wait.
Published byAron Bennett Modified over 9 years ago
1
Transient
2
Equation of motion resistance force is proportional to speed : For convenience: Also, k=m 0 2 Trial solution
3
Underdamped Two solutions with
5
The real solution of equation of motion
6
Damped cosine oscillation
7
Logarithmic decrement A1A1 A2A2 A3A3 A4A4
8
Phase difference between x and v is not simply /2.
9
To find E and F we choose the initial conditions with
10
High Damping
12
For very high damping
13
© SB For very high damping
14
Two different time scale involved in damped SHM
15
Critical Damping General Solution
17
Transient : Damped oscillation with no forcing Use the link: http://www.walter-fendt.de/ph14e/resonance.htm © Walter Fendt
18
PROBLEM A door shutter has a spring which, in the absence of damping, shuts the door in 0.5 seconds. The problem is that the door bangs shut with a speed 1 m/s. A damper with a damping coefficient is introduced to ensure that the door shuts gradually. What is the time required for the door to shut and the velocity at the instant it shuts, if = 0. 5 . Note that the spring is unstretched when the door is shut.
19
Transients Equation of motion For low damping
20
For high damping For critical damping
21
FEYNMAN LECTURES ON PHYSICS VOL I Author : RICHARD P FEYNMAN, IIT KGP Central Library : Class no. 530.4
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.