Solve $frac{d^2y}{dx^2}+2frac{dy}{dx}+y=x sin^2x$
Solve the differential equation Solve $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=x sin^2x$$
i used the substitution $frac{dy}{dx}+y=t$ we get
$$frac{dt}{dx}+t=xsin^2x$$ which is linear first order, using integrating factor method we get the solution
$$te^x=int xe^xsin^2xdx+C$$
$$te^x=frac{1}{2} left(int xe^xdx-int xe^xcos 2xdxright)+C=frac{1}{2}left(P-Qright)+C tag{1}$$
we have $$P=int xe^x=(x-1)e^x+C'$$
now using integration by parts we have
$$Q=int xe^x cos2xdx=xint e^xcos 2xdx-int left(int e^xcos 2xdxright)dx$$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}int e^x(cos 2x+2sin 2x)dx $$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}left(frac{e^x}{5}(cos 2x+2sin 2x)right)-left(frac{2e^x}{5}(sin 2x-2 cos 2x)right)$$
finally we need to solve another linear differential equation viz:
$$e^xleft(frac{dy}{dx}+yright)=frac{1}{2}left(P-Qright)+C$$
which is very tedious.
is there a good approach?
integration algebra-precalculus differential-equations
add a comment |
Solve the differential equation Solve $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=x sin^2x$$
i used the substitution $frac{dy}{dx}+y=t$ we get
$$frac{dt}{dx}+t=xsin^2x$$ which is linear first order, using integrating factor method we get the solution
$$te^x=int xe^xsin^2xdx+C$$
$$te^x=frac{1}{2} left(int xe^xdx-int xe^xcos 2xdxright)+C=frac{1}{2}left(P-Qright)+C tag{1}$$
we have $$P=int xe^x=(x-1)e^x+C'$$
now using integration by parts we have
$$Q=int xe^x cos2xdx=xint e^xcos 2xdx-int left(int e^xcos 2xdxright)dx$$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}int e^x(cos 2x+2sin 2x)dx $$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}left(frac{e^x}{5}(cos 2x+2sin 2x)right)-left(frac{2e^x}{5}(sin 2x-2 cos 2x)right)$$
finally we need to solve another linear differential equation viz:
$$e^xleft(frac{dy}{dx}+yright)=frac{1}{2}left(P-Qright)+C$$
which is very tedious.
is there a good approach?
integration algebra-precalculus differential-equations
math.psu.edu/tseng/class/Math251/…
– Hussain-Alqatari
Dec 2 '18 at 6:58
Look up Method of Variation of Parameters and Method of Undetermined Coefficients
– Shubham Johri
Dec 2 '18 at 7:08
add a comment |
Solve the differential equation Solve $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=x sin^2x$$
i used the substitution $frac{dy}{dx}+y=t$ we get
$$frac{dt}{dx}+t=xsin^2x$$ which is linear first order, using integrating factor method we get the solution
$$te^x=int xe^xsin^2xdx+C$$
$$te^x=frac{1}{2} left(int xe^xdx-int xe^xcos 2xdxright)+C=frac{1}{2}left(P-Qright)+C tag{1}$$
we have $$P=int xe^x=(x-1)e^x+C'$$
now using integration by parts we have
$$Q=int xe^x cos2xdx=xint e^xcos 2xdx-int left(int e^xcos 2xdxright)dx$$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}int e^x(cos 2x+2sin 2x)dx $$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}left(frac{e^x}{5}(cos 2x+2sin 2x)right)-left(frac{2e^x}{5}(sin 2x-2 cos 2x)right)$$
finally we need to solve another linear differential equation viz:
$$e^xleft(frac{dy}{dx}+yright)=frac{1}{2}left(P-Qright)+C$$
which is very tedious.
is there a good approach?
integration algebra-precalculus differential-equations
Solve the differential equation Solve $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=x sin^2x$$
i used the substitution $frac{dy}{dx}+y=t$ we get
$$frac{dt}{dx}+t=xsin^2x$$ which is linear first order, using integrating factor method we get the solution
$$te^x=int xe^xsin^2xdx+C$$
$$te^x=frac{1}{2} left(int xe^xdx-int xe^xcos 2xdxright)+C=frac{1}{2}left(P-Qright)+C tag{1}$$
we have $$P=int xe^x=(x-1)e^x+C'$$
now using integration by parts we have
$$Q=int xe^x cos2xdx=xint e^xcos 2xdx-int left(int e^xcos 2xdxright)dx$$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}int e^x(cos 2x+2sin 2x)dx $$
$$int xe^x cos2xdx=frac{xe^x}{5}left(cos 2x+2sin 2xright)-frac{1}{5}left(frac{e^x}{5}(cos 2x+2sin 2x)right)-left(frac{2e^x}{5}(sin 2x-2 cos 2x)right)$$
finally we need to solve another linear differential equation viz:
$$e^xleft(frac{dy}{dx}+yright)=frac{1}{2}left(P-Qright)+C$$
which is very tedious.
is there a good approach?
integration algebra-precalculus differential-equations
integration algebra-precalculus differential-equations
asked Dec 2 '18 at 6:55
Umesh shankar
2,56631219
2,56631219
math.psu.edu/tseng/class/Math251/…
– Hussain-Alqatari
Dec 2 '18 at 6:58
Look up Method of Variation of Parameters and Method of Undetermined Coefficients
– Shubham Johri
Dec 2 '18 at 7:08
add a comment |
math.psu.edu/tseng/class/Math251/…
– Hussain-Alqatari
Dec 2 '18 at 6:58
Look up Method of Variation of Parameters and Method of Undetermined Coefficients
– Shubham Johri
Dec 2 '18 at 7:08
math.psu.edu/tseng/class/Math251/…
– Hussain-Alqatari
Dec 2 '18 at 6:58
math.psu.edu/tseng/class/Math251/…
– Hussain-Alqatari
Dec 2 '18 at 6:58
Look up Method of Variation of Parameters and Method of Undetermined Coefficients
– Shubham Johri
Dec 2 '18 at 7:08
Look up Method of Variation of Parameters and Method of Undetermined Coefficients
– Shubham Johri
Dec 2 '18 at 7:08
add a comment |
3 Answers
3
active
oldest
votes
Hint
If you are as lazy as I am, considering $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=frac{x}{2}(1-cos(2x))$$ assume
$$y_p=a+b x+csin(2x)+dcos(2x)+e xsin(2x)+f xcos(2x)$$ Replace and identify $a,b,c,d,e,f$. This should be simple.
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
add a comment |
Write the differential equation as $$(D^2+2D+1)y=xsin^2(x)=frac{x}{2}(1-cos(2x))$$ then a complete solution can be written as $$y=y_r+y_p$$ where $y_r$ is the most general solution of the reduced equation $(D^2+2D+1)y=(D+1)^2y=0$ i.e. $y_r=ae^{-x}+bxe^{-x}$ , where $a,b$ are two arbitrary constants.
And $y_p$ is a one particular integral given by $$y_p=frac{1}{(D^2+2D+1)}frac{x}{2}(1-cos(2x))$$ i.e. $2y_p=(D+1)^{-2}(x)-(D+1)^{-2}(xcos(2x))$. Now $$(1+D)^{-2}(x)={1+frac{(-2)}{1!}D+frac{(-2)(-2-1)}{2!}+....}=(1-2D)x=x-2.$$ Since $D^2x=0,D^3x=0,....$
Next $(1+D)^{-2}(xcos(2x))=Re((1+D)^{-2}(xe^{iota 2x}))$. So that $$(1+D)^{-2}(xe^{iota 2x})=e^{iota 2x}frac{1}{1+2(D+2iota)+(D+2iota)^2} x.$$ Again expanding as bi-nomial series as in pervious part and then considering real part you can find particular integral $y_p$.
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
add a comment |
The homogeneous part is classical, though the characteristic polynomial has a double root, giving terms $e^{-x}$ and $xe^{-x}$.
The non-homogeneous one is a little harder, though you are lucky that there is no overlap with the roots. Let us try a solution of the form $y=xz+w$. The equation turns to
$$(z''+2z'+z)x+2z'+z+w''+2w'+w=xfrac{1-cos 2x}2=xfrac{1-Re(e^{i2x)}}2.$$
The constant term is dealt with by $dfrac12$, while the other can be handled using complex numbers, giving
$$z=-frac12Releft(frac{e^{i2x}}{4+2i+1}right).$$
Next,
$$w''+2w'+w=frac12Releft(frac{(i4+1))e^{i2x}}{4+2i+1}right)$$ and
$$w=frac12Releft(frac{(i4+1))e^{i2x}}{(4+2i+1)^2}right).$$
add a comment |
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3 Answers
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votes
3 Answers
3
active
oldest
votes
active
oldest
votes
active
oldest
votes
Hint
If you are as lazy as I am, considering $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=frac{x}{2}(1-cos(2x))$$ assume
$$y_p=a+b x+csin(2x)+dcos(2x)+e xsin(2x)+f xcos(2x)$$ Replace and identify $a,b,c,d,e,f$. This should be simple.
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
add a comment |
Hint
If you are as lazy as I am, considering $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=frac{x}{2}(1-cos(2x))$$ assume
$$y_p=a+b x+csin(2x)+dcos(2x)+e xsin(2x)+f xcos(2x)$$ Replace and identify $a,b,c,d,e,f$. This should be simple.
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
add a comment |
Hint
If you are as lazy as I am, considering $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=frac{x}{2}(1-cos(2x))$$ assume
$$y_p=a+b x+csin(2x)+dcos(2x)+e xsin(2x)+f xcos(2x)$$ Replace and identify $a,b,c,d,e,f$. This should be simple.
Hint
If you are as lazy as I am, considering $$frac{d^2y}{dx^2}+2frac{dy}{dx}+y=frac{x}{2}(1-cos(2x))$$ assume
$$y_p=a+b x+csin(2x)+dcos(2x)+e xsin(2x)+f xcos(2x)$$ Replace and identify $a,b,c,d,e,f$. This should be simple.
answered Dec 2 '18 at 7:43
Claude Leibovici
119k1157132
119k1157132
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
add a comment |
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
Solving for those coefficients can be a nightmare to be fair :-) this is what CAS are for?
– DavidG
Dec 2 '18 at 7:54
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
@DavidG. It took me five minutes with pen and paper.
– Claude Leibovici
Dec 2 '18 at 8:39
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
So roughly the same time as the original post.
– DavidG
Dec 2 '18 at 8:43
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
@ClaudeLeibovici: lazyness can be a virtue. ;-)
– Yves Daoust
Dec 2 '18 at 11:45
add a comment |
Write the differential equation as $$(D^2+2D+1)y=xsin^2(x)=frac{x}{2}(1-cos(2x))$$ then a complete solution can be written as $$y=y_r+y_p$$ where $y_r$ is the most general solution of the reduced equation $(D^2+2D+1)y=(D+1)^2y=0$ i.e. $y_r=ae^{-x}+bxe^{-x}$ , where $a,b$ are two arbitrary constants.
And $y_p$ is a one particular integral given by $$y_p=frac{1}{(D^2+2D+1)}frac{x}{2}(1-cos(2x))$$ i.e. $2y_p=(D+1)^{-2}(x)-(D+1)^{-2}(xcos(2x))$. Now $$(1+D)^{-2}(x)={1+frac{(-2)}{1!}D+frac{(-2)(-2-1)}{2!}+....}=(1-2D)x=x-2.$$ Since $D^2x=0,D^3x=0,....$
Next $(1+D)^{-2}(xcos(2x))=Re((1+D)^{-2}(xe^{iota 2x}))$. So that $$(1+D)^{-2}(xe^{iota 2x})=e^{iota 2x}frac{1}{1+2(D+2iota)+(D+2iota)^2} x.$$ Again expanding as bi-nomial series as in pervious part and then considering real part you can find particular integral $y_p$.
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
add a comment |
Write the differential equation as $$(D^2+2D+1)y=xsin^2(x)=frac{x}{2}(1-cos(2x))$$ then a complete solution can be written as $$y=y_r+y_p$$ where $y_r$ is the most general solution of the reduced equation $(D^2+2D+1)y=(D+1)^2y=0$ i.e. $y_r=ae^{-x}+bxe^{-x}$ , where $a,b$ are two arbitrary constants.
And $y_p$ is a one particular integral given by $$y_p=frac{1}{(D^2+2D+1)}frac{x}{2}(1-cos(2x))$$ i.e. $2y_p=(D+1)^{-2}(x)-(D+1)^{-2}(xcos(2x))$. Now $$(1+D)^{-2}(x)={1+frac{(-2)}{1!}D+frac{(-2)(-2-1)}{2!}+....}=(1-2D)x=x-2.$$ Since $D^2x=0,D^3x=0,....$
Next $(1+D)^{-2}(xcos(2x))=Re((1+D)^{-2}(xe^{iota 2x}))$. So that $$(1+D)^{-2}(xe^{iota 2x})=e^{iota 2x}frac{1}{1+2(D+2iota)+(D+2iota)^2} x.$$ Again expanding as bi-nomial series as in pervious part and then considering real part you can find particular integral $y_p$.
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
add a comment |
Write the differential equation as $$(D^2+2D+1)y=xsin^2(x)=frac{x}{2}(1-cos(2x))$$ then a complete solution can be written as $$y=y_r+y_p$$ where $y_r$ is the most general solution of the reduced equation $(D^2+2D+1)y=(D+1)^2y=0$ i.e. $y_r=ae^{-x}+bxe^{-x}$ , where $a,b$ are two arbitrary constants.
And $y_p$ is a one particular integral given by $$y_p=frac{1}{(D^2+2D+1)}frac{x}{2}(1-cos(2x))$$ i.e. $2y_p=(D+1)^{-2}(x)-(D+1)^{-2}(xcos(2x))$. Now $$(1+D)^{-2}(x)={1+frac{(-2)}{1!}D+frac{(-2)(-2-1)}{2!}+....}=(1-2D)x=x-2.$$ Since $D^2x=0,D^3x=0,....$
Next $(1+D)^{-2}(xcos(2x))=Re((1+D)^{-2}(xe^{iota 2x}))$. So that $$(1+D)^{-2}(xe^{iota 2x})=e^{iota 2x}frac{1}{1+2(D+2iota)+(D+2iota)^2} x.$$ Again expanding as bi-nomial series as in pervious part and then considering real part you can find particular integral $y_p$.
Write the differential equation as $$(D^2+2D+1)y=xsin^2(x)=frac{x}{2}(1-cos(2x))$$ then a complete solution can be written as $$y=y_r+y_p$$ where $y_r$ is the most general solution of the reduced equation $(D^2+2D+1)y=(D+1)^2y=0$ i.e. $y_r=ae^{-x}+bxe^{-x}$ , where $a,b$ are two arbitrary constants.
And $y_p$ is a one particular integral given by $$y_p=frac{1}{(D^2+2D+1)}frac{x}{2}(1-cos(2x))$$ i.e. $2y_p=(D+1)^{-2}(x)-(D+1)^{-2}(xcos(2x))$. Now $$(1+D)^{-2}(x)={1+frac{(-2)}{1!}D+frac{(-2)(-2-1)}{2!}+....}=(1-2D)x=x-2.$$ Since $D^2x=0,D^3x=0,....$
Next $(1+D)^{-2}(xcos(2x))=Re((1+D)^{-2}(xe^{iota 2x}))$. So that $$(1+D)^{-2}(xe^{iota 2x})=e^{iota 2x}frac{1}{1+2(D+2iota)+(D+2iota)^2} x.$$ Again expanding as bi-nomial series as in pervious part and then considering real part you can find particular integral $y_p$.
edited Dec 2 '18 at 11:41
DavidG
1,729619
1,729619
answered Dec 2 '18 at 7:24
UserS
1,5371112
1,5371112
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
add a comment |
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
During my undergrad, I recall this being termed the ‘Linear D operator’ - is that correct? Also, do you know of any good textbooks on it?
– DavidG
Dec 2 '18 at 9:23
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
You are right. Here $D$ stands for $frac {d}{dx}$, $D^2$ stands for $frac{d^2}{dx^2}$.Schaum's Outline of Differential Equations-Frank Ayres-McGraw-Hill International Book.
– UserS
Dec 2 '18 at 11:38
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
Thanks so much. Appreciate the reference.
– DavidG
Dec 2 '18 at 11:50
add a comment |
The homogeneous part is classical, though the characteristic polynomial has a double root, giving terms $e^{-x}$ and $xe^{-x}$.
The non-homogeneous one is a little harder, though you are lucky that there is no overlap with the roots. Let us try a solution of the form $y=xz+w$. The equation turns to
$$(z''+2z'+z)x+2z'+z+w''+2w'+w=xfrac{1-cos 2x}2=xfrac{1-Re(e^{i2x)}}2.$$
The constant term is dealt with by $dfrac12$, while the other can be handled using complex numbers, giving
$$z=-frac12Releft(frac{e^{i2x}}{4+2i+1}right).$$
Next,
$$w''+2w'+w=frac12Releft(frac{(i4+1))e^{i2x}}{4+2i+1}right)$$ and
$$w=frac12Releft(frac{(i4+1))e^{i2x}}{(4+2i+1)^2}right).$$
add a comment |
The homogeneous part is classical, though the characteristic polynomial has a double root, giving terms $e^{-x}$ and $xe^{-x}$.
The non-homogeneous one is a little harder, though you are lucky that there is no overlap with the roots. Let us try a solution of the form $y=xz+w$. The equation turns to
$$(z''+2z'+z)x+2z'+z+w''+2w'+w=xfrac{1-cos 2x}2=xfrac{1-Re(e^{i2x)}}2.$$
The constant term is dealt with by $dfrac12$, while the other can be handled using complex numbers, giving
$$z=-frac12Releft(frac{e^{i2x}}{4+2i+1}right).$$
Next,
$$w''+2w'+w=frac12Releft(frac{(i4+1))e^{i2x}}{4+2i+1}right)$$ and
$$w=frac12Releft(frac{(i4+1))e^{i2x}}{(4+2i+1)^2}right).$$
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The homogeneous part is classical, though the characteristic polynomial has a double root, giving terms $e^{-x}$ and $xe^{-x}$.
The non-homogeneous one is a little harder, though you are lucky that there is no overlap with the roots. Let us try a solution of the form $y=xz+w$. The equation turns to
$$(z''+2z'+z)x+2z'+z+w''+2w'+w=xfrac{1-cos 2x}2=xfrac{1-Re(e^{i2x)}}2.$$
The constant term is dealt with by $dfrac12$, while the other can be handled using complex numbers, giving
$$z=-frac12Releft(frac{e^{i2x}}{4+2i+1}right).$$
Next,
$$w''+2w'+w=frac12Releft(frac{(i4+1))e^{i2x}}{4+2i+1}right)$$ and
$$w=frac12Releft(frac{(i4+1))e^{i2x}}{(4+2i+1)^2}right).$$
The homogeneous part is classical, though the characteristic polynomial has a double root, giving terms $e^{-x}$ and $xe^{-x}$.
The non-homogeneous one is a little harder, though you are lucky that there is no overlap with the roots. Let us try a solution of the form $y=xz+w$. The equation turns to
$$(z''+2z'+z)x+2z'+z+w''+2w'+w=xfrac{1-cos 2x}2=xfrac{1-Re(e^{i2x)}}2.$$
The constant term is dealt with by $dfrac12$, while the other can be handled using complex numbers, giving
$$z=-frac12Releft(frac{e^{i2x}}{4+2i+1}right).$$
Next,
$$w''+2w'+w=frac12Releft(frac{(i4+1))e^{i2x}}{4+2i+1}right)$$ and
$$w=frac12Releft(frac{(i4+1))e^{i2x}}{(4+2i+1)^2}right).$$
answered Dec 2 '18 at 12:01
Yves Daoust
124k671221
124k671221
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add a comment |
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math.psu.edu/tseng/class/Math251/…
– Hussain-Alqatari
Dec 2 '18 at 6:58
Look up Method of Variation of Parameters and Method of Undetermined Coefficients
– Shubham Johri
Dec 2 '18 at 7:08