A string is stretched and fastened to two points at a distance 0
l
0 apart. Motion is started by
displacing the string in the form y = k sin πx
l
from which it is released at time t = 0. Show
that the displacement of any point on the string at a distance x from one end at time t is
given by k sin πx
l
cos πax
l
Solution
The displacement y(x,t) of the string at a distance X from end 0 at time t is give by the following equation;
"\\frac{d^2y}{dt^2}=a^2\\frac{d^2y}{dx^2}" ..........(a)
We establish the boundary conditions using the given information.
Since the ends of the spring ,x=0 and x=l are fixed,they undergo zero displacement at any time t;
y(0,t)=0 for t"\\geq" 0..........(1)
y(l,t)=0 for t"\\geq" 0...........(2)
Since the spring is released from rest,at t =0 ,the velocity of every point on the string in the y-direction is zero,hence;
"\\frac{dy}{dx}" (x,0)=0 for 0"\\leq" x"\\leq" l..............(3)
The initial displacement is in the form of y=ksin"\\frac{\u03c0x}{l}" ,where y(x,0) is the initial displacement of any point x in the y-direction ,hence
y(x,0)=ksin"\\frac{\u03c0x}{l}" for 0"\\leq" x"\\leq" l ..........(4)
(1),(2),(3) and (4) are the boundary conditions of the problem.
The general solutions of equation (a) with respect to the vibration of the string is
y(x,t)=(Acos px +Bsin px)(C cos pat +Dsin pat) ......(b)
A,B,C,D and p are arbitrary constants which can be found by applying the boundary conditions;
Using condition (1) in (b),we have
A(C cos pat + Dsin pat)=0 for all t"\\geq"0
A=0
Using condition (2) in (b) ,we have
Since A=0
B sin pl(C cos pat +Dsin pat)=0,for all
t"\\geq" 0;
Bsin pl=0
Either B or sin pl=0
If B = 0 ,y(x,t)=0 and the equation is meaningless,so
sin pl=0
pl=nπ
p="\\frac{n\u03c0}{l}"
Where n=0,1,2,3..."\\infin"
Differentiate both sides of (b) with respect to t:
"\\frac{dy}{dt}" (x,y)=(Bsin px)pa(-Csinpat+Dcos pat) ........(c)
Where p="\\frac{n\u03c0}{l}"
Using condition (3) on (c),we have
Bsin px.paD=0
But B"\\ne" 0 and p"\\ne" 0 ,we get D=0
With the found constants ,the equation (b) reduces to
y(x,t)=BC sin "\\frac{n\u03c0x}{l}" Cos"\\frac{n\u03c0at}{l}" where n=1,2,3....."\\infin"
Taking BC=k,
The most general solution would be
y(x,t)="\\displaystyle\\sum_{n=1}^\\infin" "\\lambda_n"Sin"\\frac{n\u03c0}{l}"Cos"\\frac{n\u03c0at}{l}" ....(d)
"\\lambda_n" can be found using condition (4) in (d)
ksin"\\frac{\u03c0x}{l}" ="\\lambda_nsin\\frac{n\u03c0x}{l}"
By comparison,
"\\lambda_n" =k
"\\frac{\u03c0x}{l}=\\frac{n\u03c0x}{l}"
n=1
Using this values,the equation of displacement at any time on the string will be
y(x,t)=ksin"\\frac{\u03c0x}{l}" Cos"\\frac{\u03c0ax}{l}"
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