Question #42602

determine the response of the damped vibrating system given by the below mentioned differential equation using laplace transform

d2y/dt2+3dy/dt+2y=2(t^2+t+1) ;y(0)=2 ,y'(0)=0

Expert's answer

Answer on Question #42602– Math – Differential Calculus | Equation

Question:

Using laplace transforms solve the following ordinary differential equation


d2ydt2+3dydt+2y=2(t2+t+1);y(0)=2,y(0)=0\frac {\mathrm {d} ^ {2} \mathrm {y}}{\mathrm {d t} ^ {2}} + 3 \frac {\mathrm {d y}}{\mathrm {d t}} + 2 \mathrm {y} = 2 (\mathrm {t} ^ {2} + \mathrm {t} + 1); \mathrm {y} (0) = 2, \mathrm {y} ^ {\prime} (0) = 0


Solution:

Let Y(s)=L[y(t)](s)Y(s) = L[y(t)](s) . Instead of solving directly for y(t)y(t) , we derive a new equation for Y(s)Y(s) . Once we find Y(s)Y(s) , we inverse transform to determine y(t)y(t) .

The first step is to take the Laplace transform of both sides of the original differential equation. We have


L[y+3y+2y](s)=L[2(t2+t+1)](s)L [ y ^ {\prime \prime} + 3 y ^ {\prime} + 2 y ] (s) = L [ 2 (t ^ {2} + t + 1) ] (s)


If we look at the left-hand side, we have


L[y+3y+2y](s)=L[y](s)+3L[y](s)+2L[y](s)L [ y ^ {\prime \prime} + 3 y ^ {\prime} + 2 y ] (s) = L [ y ^ {\prime \prime} ] (s) + 3 L [ y ^ {\prime} ] (s) + 2 L [ y ] (s)


Now use the formulas for the L[y]L[y''] , L[y]L[y'] and L[y]L[y'] :


L[y]=sL[y]y(0)=sY(s)1;L [ y ^ {\prime} ] = s L [ y ] - y (0) = s Y (s) - 1;L[y]=s2L[y]sy(0)y(0)=s2Y(s)s2;L [ y ^ {\prime \prime} ] = s ^ {2} L [ y ] - s y (0) - y ^ {\prime} (0) = s ^ {2} Y (s) - s - 2;


Hence, we have


L[y+3y+2y](s)=s2Y(s)s2+3(sY(s)1)+2Y(s).L [ y ^ {\prime \prime} + 3 y ^ {\prime} + 2 y ] (s) = s ^ {2} Y (s) - s - 2 + 3 (s Y (s) - 1) + 2 Y (s).


If we look at the right-hand side, we have


L[2(t2+t+1)](s)=2L[t2](s)+2L[t](s)+2L[1](s)L [ 2 (t ^ {2} + t + 1) ] (s) = 2 L [ t ^ {2} ] (s) + 2 L [ t ] (s) + 2 L [ 1 ] (s)


Now use the formulas for the L[t2]L[t^2] , L[t]L[t] and L[1]L[1] :


L[t2]=2s3,L[t]=1s2,L[1]=1s.L [ t ^ {2} ] = \frac {2}{s ^ {3}}, \qquad L [ t ] = \frac {1}{s ^ {2}}, \quad L [ 1 ] = \frac {1}{s}.


The Laplace-transformed differential equation is


s2Y(s)s2+3(sY(s)1)+2Y(s)=4s3+2s2+2ss ^ {2} Y (s) - s - 2 + 3 (s Y (s) - 1) + 2 Y (s) = \frac {4}{s ^ {3}} + \frac {2}{s ^ {2}} + \frac {2}{s}(s2+3s+2)Y(s)=s+5+4s3+2s2+2s(s ^ {2} + 3 s + 2) Y (s) = s + 5 + \frac {4}{s ^ {3}} + \frac {2}{s ^ {2}} + \frac {2}{s}


Or


(s2+3s+2)Y(s)=(s+1)(s3+4s22s+4)s3(s^2 + 3s + 2)Y(s) = \frac{(s + 1)(s^3 + 4s^2 - 2s + 4)}{s^3}


This is a linear algebraic equation for Y(s)Y(s)! We have converted a differential equation into a algebraic equation! Solving for Y(s)Y(s), we have


Y(s)=(s+1)(s3+4s22s+4)s3(s2+3s+2)Y(s) = \frac{(s + 1)(s^3 + 4s^2 - 2s + 4)}{s^3(s^2 + 3s + 2)}


We can simplify this expression using the method of partial fractions:


Y(s)=2s32s22s+2+3s(for s1)Y(s) = \frac{2}{s^3} - \frac{2}{s^2} - \frac{2}{s + 2} + \frac{3}{s} \quad (for\ s \neq -1)


Recall the inverse transforms:


L1[1s3](t)=12t2,L1[1s2](t)=t,L1[1s+2](t)=e2t,L1[1s](t)=1L^{-1}\left[\frac{1}{s^3}\right](t) = \frac{1}{2t^2}, \quad L^{-1}\left[\frac{1}{s^2}\right](t) = t, \quad L^{-1}\left[\frac{1}{s + 2}\right](t) = e^{-2t}, \quad L^{-1}\left[\frac{1}{s}\right](t) = 1


Using linearity of the inverse transform, we have


y(t)=L1[2s32s22s+2+3s]=212t22te2t+31==t22te2t+3;\begin{array}{l} y(t) = L^{-1}\left[\frac{2}{s^3} - \frac{2}{s^2} - \frac{2}{s + 2} + \frac{3}{s}\right] = 2 * \frac{1}{2}t^2 - 2 * t - e^{-2t} + 3 * 1 = \\ = t^2 - 2t - e^{-2t} + 3; \end{array}


Answer. y(t)=t22te2t+3y(t) = t^2 - 2t - e^{-2t} + 3;

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