Answer to Question #267485 in Differential Equations for Ran

Question #267485

A tightly stretched string of length"l"has it's ends fastened at x=0andx=l. The midpoint of the string is taken the height h and released. find the initial displacement function at timet=0?


1
Expert's answer
2021-11-18T06:22:21-0500

Solution;

Displacement of a string y(x,t) given by;

"\\frac{\\partial^2y}{\\partial t^2}=a^2\\frac{\\partial^2y}{\\partial x^2}" .....(1)

A suitable solution of (1) is given by;

"y(x,t)=(Acoslx+Bsinlx)(Ccoslat+Dsinlat).....(2)"

The boundary conditions are;

"(i)y(0,t)=0"

"(ii)y(l,t)=0"

"(iii)(\\frac{\\partial y}{\\partial t})_{t=0}=0"

(iv)

"(y(x,0) = \\begin{cases}\n \\frac{2hx}{l} &\\text{if } 0\\leq x\\leq\\frac l2 \\\\\n \\frac{2h(l-x)}{l} &\\text{if } \\frac l2\\leq x\\leq l\n\\end{cases}"

Using conditions (i) and (ii) in (2),we get;

A=0

"\\lambda=\\frac{n\u03c0}{l}"

Therefore;

"y(x,t)=Bsin\\frac{n\u03c0x}{l}[Ccos\\frac{n\u03c0at}{l}+Dsin\\frac{n\u03c0at}{l}]"

Differentiate to obtain;

"\\frac{\\partial y}{\\partial t}=Bsin\\frac{n\u03c0x}{l}(-Csin\\frac{n\u03c0at}{l}.\\frac{n\u03c0t}{l}+Dcos\\frac{n\u03c0at}{l}.\\frac{n\u03c0a}{l})"

Using conditions (iii) in the above equation we get;

"0=Bsin\\frac{n\u03c0x}{l}Dsin\\frac{n\u03c0a}{l}"

Since "B\\neq0" ,then D=0

Equation (2) reduces to;

"y(x,t)=Bsin\\frac{n\u03c0x}{l}Ccos\\frac{n\u03c0at}{l}"

Rewrite;

"y(x,t)=B_1sin\\frac{n\u03c0x}{l}cos\\frac{n\u03c0at}{l}....(4)"

(Note that B1=BC )

Using condition (iv) ,we get that;

"y(x,0)=\\displaystyle\\sum_{n=0}^{\\infin}B_nsin\\frac{n\u03c0x}{l}..\u2026(5)"

The RHS of equation (5) is the half range Fourier sine series of the LHS function, therefore;

"B_n=\\frac 2l\\int_0^lf(x)sin\\frac{n\u03c0x}{l}dx"

"=\\frac2l[\\int_0^{\\frac L2}\\frac{2hx}{l}sin\\frac{n\u03c0x}{l}dx+\\int_{\\frac l2}^0\\frac{2h(l-x)}{l}sin\\frac{n\u03c0x}{l}dx]"

Rewrite;

"=\\frac{4h}{l^2}[\\int_0^{\\frac L2}xsin\\frac{n\u03c0x}{l}dx+\\int_{\\frac L2}^0(l-x)sin\\frac{n\u03c0x}{l}dx]"

Integrating on the given limits;

"=\\frac{4h}{l^2}[[\\frac{-xcos\\frac{n\u03c0x}{l}}{\\frac{n\u03c0}{l}}+\\frac{sin \\frac{n\u03c0x}{l}}{\\frac{n^2\u03c0^2}{l^2}}]_0^{\\frac L2}+[\\frac{(x-l)cos\\frac{n\u03c0x}{l}}{\\frac{n\u03c0}{l}}+\\frac{sin\\frac{n\u03c0x}{l}}{\\frac{n^2\u03c0^2}{l^2}}]_{\\frac l2}^l]"

Applying the limits ;

"\\frac{4h}{l^2}[\\frac{sin\\frac{n\u03c0}{2}}{\\frac{n^2\u03c0^2}{l^2}}]=\\frac{4hsin\\frac{n\u03c0}{2}}{n^2\u03c0^2}"

Hence,the solution is;

"y(x)=\\displaystyle\\sum_{n=1}^{\\infin}\\frac{4hsin\\frac{n\u03c0}{2}}{n^2\u03c0^2}cos\\frac{n\u03c0at}{l}sin\\frac{n\u03c0x}{l}"




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