Giải toán trực tuyến W | A




Vẽ đồ thị trong Oxyz plot3D(f(x,y),x=..,y=..)
Vẽ đồ thị trong Oxy plot(f(x),x=..,y=..)
Đạo hàm derivative(f(x))
Tích phân Integrate(f(x))


Giải toán trực tuyến W|A

MW

Hiển thị các bài đăng có nhãn Power Spectral Density. Hiển thị tất cả bài đăng
Hiển thị các bài đăng có nhãn Power Spectral Density. Hiển thị tất cả bài đăng

Chủ Nhật, 1 tháng 7, 2007

KHẢO SÁT HÀM MẬT ĐỘ PHỔ PHƯƠNG TRÌNH DUFFING BẰNG PHƯƠNG PHÁP TUYẾN TÍNH HÓA TƯƠNG ĐƯƠNG

Creative Commons License



This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivs 3.0 United States License.


Investigation of the Power Spectral Density of Duffing's Equation By Equivalent Linearization Method

Co. H. Tran.
Faculty of Mathematics, University of Natural Sciences - VNU-HCM

Abstract

We consider the non-linear random vibration model demonstrated by the Duffing's differential equation :

(*)

The stationary random process is f( t) which is satisfied <> = 0
with the spectral density function Sf ( w ) . To find the solution Sx ( w ) of (*) we use the equivalent linearization method .

1. Model Definition

The non-linear random vibration model includes the mass (m) - dashpot (c) -spring (k)
( fig.1 ) . This model moves on the rough surface which is described by the random variable y(s) with the constant velocity v . If we have the relation s = vt and the mass m is also influenced under the non-linear stimulating force , then the vibration differential equation of the mass m can be rewritten as :

( 1.0 )
( fig . 1)

2. The equivalent linearization method

The conditions of the stationary solution and equivalent approximation : ( 2.1 )
The linear operator : ( 2 2 )
Substitute D = iy1 into (2.2) we obtain the frequency response :
( 2.3 )
The impulse response : ( 2.4 )
The power spectral density :
( 2. 5 )
Assuming S f ( y1 ) = So : const ( white-noise) then we have :
( 2. 6 )
By altering : and choosing S f ( y1 ) = So = 1 ( to simplify the next algorithm ) , we take into account the integral expression :
( 2.7 )
The function h(z) :
: ( 2.14 )
Calculation in details : eq:=subs(psi=1,mu=0.1,beta=0.2,S[0]=1,Gamma=omega[0]^2+Delta,eqndelta);eq:=subs(omega[0]=0.5,eq);
> nodelta:=solve(eq,Delta);

The Duffing's equation can be approximated in the linear form with the values of nodelta : ( 2.15 )
The investigation on components of the Duffing's differential equation will be calculated by other methods of linear random vibration , and we can obtain the corresponding approximate values in the meaning of minimum variance .

3. Parameters - Solution of the equivalent differential equation
The graph of Duffing's differential equation ( non-linear random ) :
The comparison of two graphical solutions : non-linear and equivalent-linearization .

Legal Notice: The copyright for this application is owned by the author(s). Neither Maplesoft nor the author are responsible for any errors contained within and are not liable for any damages resulting from the use of this material. This application is intended for non-commercial, non-profit use only. Contact the author for permission if you wish to use this application in for-profit activities.


See more details at :
http://www.maplesoft.com/applications/app_center_view.aspx?AID=1993











Creative Commons License
This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivs 3.0 United States License.





-------------------------------------------------------------------------------------------
 Toán học thuần túy, theo cách của riêng nó, là thi ca của tư duy logic. 
Pure mathematics is, in its way, the poetry of logical ideas. 
Albert Einstein . 

*******

Blog Toán Cơ trích đăng các thông tin khoa học tự nhiên của tác giả và nhiều nguồn tham khảo trên Internet .
Blog cũng là nơi chia sẻ các suy nghĩ , ý tưởng về nhiều lĩnh vực khoa học khác nhau .


Chia xẻ

Bài viết được xem nhiều trong tuần

CÁC BÀI VIẾT MỚI VỀ CHỦ ĐỀ TOÁN HỌC

Danh sách Blog

Gặp Cơ tại Researchgate.net

Co Tran