string is stretched and fastened
to two points
l
cm apart. Motion is started by displacing the string into the form of the curve
l
x
l
x
y
2
cos
3
2sin
and then releasing it from this position at time
t 0.
Do not use the
symbol
l
but its actual value should be used in all of your calculations (steps). Find the
displacement function
y(x,t).
The displacement of the point of the string at a distance x from the left end 0 at
time t is given by the equation-
"\\dfrac{d^2y}{dt^2}=a^2\\dfrac{d^2y}{dx^2}"
Since the ends of the string x=0 and x=l are fixed, they do not undergo any displacement
at any time.
"\\text{ Hence } y(x,t)=0, for t\\ge 0 \u2026\u2026. (2)\\\\\n\n\\text{and }y(l,t)=0 for t\\ge 0\n\n \u2026\u2026. (3)"
Since the string is released from rest initially, that is , at t=0, the initial velocity of every
point of the string in the y-direction is zero.
"\\dfrac{dy}{dt}(x,0)=0 for 0\\le x\\le l"
Since the string is initially displaced in to the form of the curve , t0he coordinates
The solution to the above problem is-
"y(x,t)=(Acospx+Bsinpx)(Ccospat+Dsinpat)"
Where A, B, C, D and p are arbitrary constants that are to be found out by using the
boundary conditions.
Using Boundary condition we can calculate the values of Arbitary constant-
"A=0,B=0,D=0,p=\\dfrac{n\\pi}{l}"
The general solution is-
"y(x,t)=\\sum_{n=1}^{\\infty}(c_nk)sin\\dfrac{n\\pi}{l}cos\\dfrac{n\\pi at}{l}"
Again using Boundary condition we have-
"\\sum_{n=1}^{\\infty}\\lambda_n sin\\dfrac{n\\pi x}{l}=f(x) for 0\\le x\\le l"
As "f(x)=ksin^3\\dfrac{\\pi x}{l}"
Now calculating f(x) and equating with above equation we get-
"y(x,t)=\\dfrac{3k}{4}sin\\dfrac{\\pi x}{l}cos\\dfrac{\\pi at}{l}-\\dfrac{k}{4}sin\\dfrac{3\\pi x}{l}cos\\dfrac{3\\pi at}{l}"
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