Unit - 3
Higher order linear differential equations with constant and variable coefficients
Q1) Solve (4D² +4D -3)y = e2x
A1)
Auxiliary equation is 4m² +4m – 3 = 0
We get, (2m+3) (2m – 1) = 0
m = -3/2, 1/2
Complementary function: CF is A e-3x/2+ B e1 x/2
Now we will find particular integral,
P.I. = f(x)
General solution is y = CF + PI
= A e-3x/2+ B e1 x/2 + 1/21 . e2x
Q2) Solve (D2 + 6D + 9) = 0
A2)
Its auxiliary equation is-
D2 + 6D + 9 = 0
(D + 3)2 = 0
Where-
D = -3, -3
Therefore, the complete solution is-
x = (c1 + c2t)e-3t
Q3) Find the P.I. Of (D + 2)(D – 1)2 y = e-2x + 2 sin h x
A3)
Now we will evaluate each term separately-
And
Therefore-
Q4) Solve (D – D’ – 2) (D – D’ – 3) z =
A4)
The C.F. Will be given by-
Particular integral-
Therefore, the complete solution is-
z = C.F. + P.I. = e2x c1(y + x) + e3x c3(y+x) + 1/5 e3x – 2y
Q5) Find P.I. Of (D2 – 2D + 4) y = ex cos x
A5)
Put
D2 = - 12 = -1
Q6) Solve (D2 + 4D + 4)y = 3 sin x + 4 cos x
A6)
Here first we will find the C.F.-
Its auxiliary equation will be-
D2 + 4D + 4 or (D + 2)2 = 0
Here we get-
D = -2, -2
C.F. = (c1 + c2x)e-2x
Now we will find P.I.-
Now the complete solution is-
Complete solution = C.F. + P.I.
= (c1 + c2 x)e-2x + sin x
Q7) Solve-
A7)
The given equation can be written as-
(D2 – 3D + 2) y = xe3x + sin 2x
Its auxiliary equation is-
D2 – 3D + 2 = 0 or (D – 2)(D – 1) = 0
We get-
D = 1, 2
So that the C.F. Will be-
C. F. = c1ex + c2e2x
Now we will find P.I.-
Therefore, the complete solution is-
Q8) Solve the following simultaneous differential equations-
It is given that x = 0 and y = 1 when t = 0.
A8)
Given equations can be written as-
Dx + 2y = - sin t ………. (1) and -2x + Dy = cos t ……… (2)
Eliminate x by multiplying (1) by 2 and (2) by D then add-
Here A.E =
So that C.F. =
And P.I. =
So that- …………. (3)
And ………….. (4)
Substitute (3) in (2), we get-
2x = Dy – cos t =
………… (5)
When t = 0, x = 0, y = 1. (3) and (5) gives-
Hence
Q9) Solve the following DE by using variation of parameters-
A9)
We can write the given equation in symbolic form as-
(D2 + 4)y = tan 2x
To find CF-
It’s A.E. Is (D2 + 4) = 0 or D = ± 2
So that CF is- y = c1 cos 2x + c2 sin 2x
To find PI-
Here y1 = cos 2x, y2 = sin 2x and X = tan 2x
Now W =
Thus PI = -
= - ¼ cos 2x log ( sec 2x + tan 2x)
So that the complete solution is-
y = c1 cos 2x + c2 sin 2x – ¼ cos 2x log (sec 2x + tan 2x)
Q10) Solve the following by using the method of variation of parameters.
A10)
This can be written as-
(D2 – 2D + 1)y = ex log x
C.F.-
Auxiliary equation is- D2 – 2D + 1= 0 or (D – 1)2 so that D = 1, 1
So that the C.F. Will be- (c1 + c2x)ex
P.I.-
Here y1 = ex , y2 = xex and X = ex log x
Now W =
Thus PI = -
So that the complete solution is-
y = (c1 + c2x)ex + ¼ x2 ex(2 log x – 3)
Q11)
A11)
Putting,
AE is
CS = CF + PI
Q12) Solve
A12)
Let,
AE is
y= CF + PI
Q13) Solve
A13)
As we see that this is Legendre’s linear equation.
Now put
So that-
And
Then the equation becomes- D (D – 1)y+ Dy + y = 2 sin t
Its auxiliary equation is-
And particular integral-
P.I. =
Note -
Hence the solution is -
Q14) Solve the following simultaneous differential equations-
....(2)
A14)
Consider the given equations
....(2)
Consider eq(1),(2)
Dx+2y = et....(1)
Dx +2x =e-t....(2)
Eliminating ‘x’ from both the equations we get,
12 2Dx + 2y = 2et
D 2Dx +D2y = e-t
y = Ae2t + Be-2t +
Q15) Solve the following simultaneous differential equations-
Given that x(0)=1 and y(0)= 0
A15)
Consider the given equations,
Dy +2x = sin2t
Dx -2y = cos2t
By solving the above equations, we get,
(D2 +4)Y =0
X(0) = 1, y(0) = 0
A =0, B=-1
Q16) Solve
(D2 + 8D + 15)y = 0
A16)
Given, (D2 + 8D + 15)y = 0
Here Auxiliary equation is
m2 – 8m + 15 = 9
m2 – 3m – 5m + 15 = 0
m(m – 3) – 5(m -3) = 0
(m – 3) (m – 5) = 0
m = 3, 5
y = C1e3x + C2 e5x
Q17) Solve: (D2 + 4)y = Cos 2x
A17)
Auxiliary equation are m2 + 4 = 0
CF = A Cos 2x + B Sin 2x
PI =
Put , D2 = - a2 = -22 = -4
PI =
PI = x
= x/4 Sin 2x
CS = CF + PR
= A Cos 2x + B Sin 2x + x/4 Sin 2x
Q18) Prove that-
A18)
As we know that-
Jn(x) =
Now put n = 1/2 in equation (1), then we get-
J1/2(x) =
Hence proved.
Q19) Prove that-
A19)
Put n = -1/2 in equation (1) of the above question, we get-
J1/2(x) =
Q20) Show that-
By using recurrence relation.
A20)
We know that-
The recurrence formula-
On differentiating, we get-
Now replace n by n -1 and n by n+1 in (1), we have-
2 J’n – 1 = Jn – 2 – Jn or J’n – 1 = ½ Jn – 2 – ½ Jn
2 J’n+1 = Jn – Jn+2 or J’n+1 = ½ Jn – ½ Jn+2
Put the values of and from the above equations in (2), we get-
2J’’n = ½ [ Jn-2 – Jn] – ½ [ Jn – Jn + 2]
4J’’n = Jn – 2 – Jn – Jn + Jn+2
4J’’n = Jn – 2 – 2 Jn + Jn+2
Q21) Prove that-
A21)
We know that- from recurrence formula
On integrating we get-
On taking n = 2 in (1), we get-
Again-
Put the value of from equation (2) and (3), we get-
By equation (1), when n = 1
Q22) Express in terms of Legendre polynomials.
A22)
By equating the coefficients of like powers of x, we get-
Put these values in equation (1), we get-
Q23) Let be the Legendre’s polynomial of degree n, then show that for every function f(x) for which the n’th derivative is continuous-
A23)
We know that-
On integrating by parts, we get-
Now integrate (n – 2) times by parts, we get-
Q24) Show that-
P2n(0) = (-1)n
A24)
We know that
Equating the coefficients of both sides, we have-
Q25) Prove that-
A25)
By using Rodrigue formula for Legendre function.
On integrating by parts, we get-
Now integrating m – 2 times, we get-
Unit - 3
Higher order linear differential equations with constant and variable coefficients
Q1) Solve (4D² +4D -3)y = e2x
A1)
Auxiliary equation is 4m² +4m – 3 = 0
We get, (2m+3) (2m – 1) = 0
m = -3/2, 1/2
Complementary function: CF is A e-3x/2+ B e1 x/2
Now we will find particular integral,
P.I. = f(x)
General solution is y = CF + PI
= A e-3x/2+ B e1 x/2 + 1/21 . e2x
Q2) Solve (D2 + 6D + 9) = 0
A2)
Its auxiliary equation is-
D2 + 6D + 9 = 0
(D + 3)2 = 0
Where-
D = -3, -3
Therefore, the complete solution is-
x = (c1 + c2t)e-3t
Q3) Find the P.I. Of (D + 2)(D – 1)2 y = e-2x + 2 sin h x
A3)
Now we will evaluate each term separately-
And
Therefore-
Q4) Solve (D – D’ – 2) (D – D’ – 3) z =
A4)
The C.F. Will be given by-
Particular integral-
Therefore, the complete solution is-
z = C.F. + P.I. = e2x c1(y + x) + e3x c3(y+x) + 1/5 e3x – 2y
Q5) Find P.I. Of (D2 – 2D + 4) y = ex cos x
A5)
Put
D2 = - 12 = -1
Q6) Solve (D2 + 4D + 4)y = 3 sin x + 4 cos x
A6)
Here first we will find the C.F.-
Its auxiliary equation will be-
D2 + 4D + 4 or (D + 2)2 = 0
Here we get-
D = -2, -2
C.F. = (c1 + c2x)e-2x
Now we will find P.I.-
Now the complete solution is-
Complete solution = C.F. + P.I.
= (c1 + c2 x)e-2x + sin x
Q7) Solve-
A7)
The given equation can be written as-
(D2 – 3D + 2) y = xe3x + sin 2x
Its auxiliary equation is-
D2 – 3D + 2 = 0 or (D – 2)(D – 1) = 0
We get-
D = 1, 2
So that the C.F. Will be-
C. F. = c1ex + c2e2x
Now we will find P.I.-
Therefore, the complete solution is-
Q8) Solve the following simultaneous differential equations-
It is given that x = 0 and y = 1 when t = 0.
A8)
Given equations can be written as-
Dx + 2y = - sin t ………. (1) and -2x + Dy = cos t ……… (2)
Eliminate x by multiplying (1) by 2 and (2) by D then add-
Here A.E =
So that C.F. =
And P.I. =
So that- …………. (3)
And ………….. (4)
Substitute (3) in (2), we get-
2x = Dy – cos t =
………… (5)
When t = 0, x = 0, y = 1. (3) and (5) gives-
Hence
Q9) Solve the following DE by using variation of parameters-
A9)
We can write the given equation in symbolic form as-
(D2 + 4)y = tan 2x
To find CF-
It’s A.E. Is (D2 + 4) = 0 or D = ± 2
So that CF is- y = c1 cos 2x + c2 sin 2x
To find PI-
Here y1 = cos 2x, y2 = sin 2x and X = tan 2x
Now W =
Thus PI = -
= - ¼ cos 2x log ( sec 2x + tan 2x)
So that the complete solution is-
y = c1 cos 2x + c2 sin 2x – ¼ cos 2x log (sec 2x + tan 2x)
Q10) Solve the following by using the method of variation of parameters.
A10)
This can be written as-
(D2 – 2D + 1)y = ex log x
C.F.-
Auxiliary equation is- D2 – 2D + 1= 0 or (D – 1)2 so that D = 1, 1
So that the C.F. Will be- (c1 + c2x)ex
P.I.-
Here y1 = ex , y2 = xex and X = ex log x
Now W =
Thus PI = -
So that the complete solution is-
y = (c1 + c2x)ex + ¼ x2 ex(2 log x – 3)
Q11)
A11)
Putting,
AE is
CS = CF + PI
Q12) Solve
A12)
Let,
AE is
y= CF + PI
Q13) Solve
A13)
As we see that this is Legendre’s linear equation.
Now put
So that-
And
Then the equation becomes- D (D – 1)y+ Dy + y = 2 sin t
Its auxiliary equation is-
And particular integral-
P.I. =
Note -
Hence the solution is -
Q14) Solve the following simultaneous differential equations-
....(2)
A14)
Consider the given equations
....(2)
Consider eq(1),(2)
Dx+2y = et....(1)
Dx +2x =e-t....(2)
Eliminating ‘x’ from both the equations we get,
12 2Dx + 2y = 2et
D 2Dx +D2y = e-t
y = Ae2t + Be-2t +
Q15) Solve the following simultaneous differential equations-
Given that x(0)=1 and y(0)= 0
A15)
Consider the given equations,
Dy +2x = sin2t
Dx -2y = cos2t
By solving the above equations, we get,
(D2 +4)Y =0
X(0) = 1, y(0) = 0
A =0, B=-1
Q16) Solve
(D2 + 8D + 15)y = 0
A16)
Given, (D2 + 8D + 15)y = 0
Here Auxiliary equation is
m2 – 8m + 15 = 9
m2 – 3m – 5m + 15 = 0
m(m – 3) – 5(m -3) = 0
(m – 3) (m – 5) = 0
m = 3, 5
y = C1e3x + C2 e5x
Q17) Solve: (D2 + 4)y = Cos 2x
A17)
Auxiliary equation are m2 + 4 = 0
CF = A Cos 2x + B Sin 2x
PI =
Put , D2 = - a2 = -22 = -4
PI =
PI = x
= x/4 Sin 2x
CS = CF + PR
= A Cos 2x + B Sin 2x + x/4 Sin 2x
Q18) Prove that-
A18)
As we know that-
Jn(x) =
Now put n = 1/2 in equation (1), then we get-
J1/2(x) =
Hence proved.
Q19) Prove that-
A19)
Put n = -1/2 in equation (1) of the above question, we get-
J1/2(x) =
Q20) Show that-
By using recurrence relation.
A20)
We know that-
The recurrence formula-
On differentiating, we get-
Now replace n by n -1 and n by n+1 in (1), we have-
2 J’n – 1 = Jn – 2 – Jn or J’n – 1 = ½ Jn – 2 – ½ Jn
2 J’n+1 = Jn – Jn+2 or J’n+1 = ½ Jn – ½ Jn+2
Put the values of and from the above equations in (2), we get-
2J’’n = ½ [ Jn-2 – Jn] – ½ [ Jn – Jn + 2]
4J’’n = Jn – 2 – Jn – Jn + Jn+2
4J’’n = Jn – 2 – 2 Jn + Jn+2
Q21) Prove that-
A21)
We know that- from recurrence formula
On integrating we get-
On taking n = 2 in (1), we get-
Again-
Put the value of from equation (2) and (3), we get-
By equation (1), when n = 1
Q22) Express in terms of Legendre polynomials.
A22)
By equating the coefficients of like powers of x, we get-
Put these values in equation (1), we get-
Q23) Let be the Legendre’s polynomial of degree n, then show that for every function f(x) for which the n’th derivative is continuous-
A23)
We know that-
On integrating by parts, we get-
Now integrate (n – 2) times by parts, we get-
Q24) Show that-
P2n(0) = (-1)n
A24)
We know that
Equating the coefficients of both sides, we have-
Q25) Prove that-
A25)
By using Rodrigue formula for Legendre function.
On integrating by parts, we get-
Now integrating m – 2 times, we get-
Unit - 3
Unit - 3
Unit - 3
Higher order linear differential equations with constant and variable coefficients
Q1) Solve (4D² +4D -3)y = e2x
A1)
Auxiliary equation is 4m² +4m – 3 = 0
We get, (2m+3) (2m – 1) = 0
m = -3/2, 1/2
Complementary function: CF is A e-3x/2+ B e1 x/2
Now we will find particular integral,
P.I. = f(x)
General solution is y = CF + PI
= A e-3x/2+ B e1 x/2 + 1/21 . e2x
Q2) Solve (D2 + 6D + 9) = 0
A2)
Its auxiliary equation is-
D2 + 6D + 9 = 0
(D + 3)2 = 0
Where-
D = -3, -3
Therefore, the complete solution is-
x = (c1 + c2t)e-3t
Q3) Find the P.I. Of (D + 2)(D – 1)2 y = e-2x + 2 sin h x
A3)
Now we will evaluate each term separately-
And
Therefore-
Q4) Solve (D – D’ – 2) (D – D’ – 3) z =
A4)
The C.F. Will be given by-
Particular integral-
Therefore, the complete solution is-
z = C.F. + P.I. = e2x c1(y + x) + e3x c3(y+x) + 1/5 e3x – 2y
Q5) Find P.I. Of (D2 – 2D + 4) y = ex cos x
A5)
Put
D2 = - 12 = -1
Q6) Solve (D2 + 4D + 4)y = 3 sin x + 4 cos x
A6)
Here first we will find the C.F.-
Its auxiliary equation will be-
D2 + 4D + 4 or (D + 2)2 = 0
Here we get-
D = -2, -2
C.F. = (c1 + c2x)e-2x
Now we will find P.I.-
Now the complete solution is-
Complete solution = C.F. + P.I.
= (c1 + c2 x)e-2x + sin x
Q7) Solve-
A7)
The given equation can be written as-
(D2 – 3D + 2) y = xe3x + sin 2x
Its auxiliary equation is-
D2 – 3D + 2 = 0 or (D – 2)(D – 1) = 0
We get-
D = 1, 2
So that the C.F. Will be-
C. F. = c1ex + c2e2x
Now we will find P.I.-
Therefore, the complete solution is-
Q8) Solve the following simultaneous differential equations-
It is given that x = 0 and y = 1 when t = 0.
A8)
Given equations can be written as-
Dx + 2y = - sin t ………. (1) and -2x + Dy = cos t ……… (2)
Eliminate x by multiplying (1) by 2 and (2) by D then add-
Here A.E =
So that C.F. =
And P.I. =
So that- …………. (3)
And ………….. (4)
Substitute (3) in (2), we get-
2x = Dy – cos t =
………… (5)
When t = 0, x = 0, y = 1. (3) and (5) gives-
Hence
Q9) Solve the following DE by using variation of parameters-
A9)
We can write the given equation in symbolic form as-
(D2 + 4)y = tan 2x
To find CF-
It’s A.E. Is (D2 + 4) = 0 or D = ± 2
So that CF is- y = c1 cos 2x + c2 sin 2x
To find PI-
Here y1 = cos 2x, y2 = sin 2x and X = tan 2x
Now W =
Thus PI = -
= - ¼ cos 2x log ( sec 2x + tan 2x)
So that the complete solution is-
y = c1 cos 2x + c2 sin 2x – ¼ cos 2x log (sec 2x + tan 2x)
Q10) Solve the following by using the method of variation of parameters.
A10)
This can be written as-
(D2 – 2D + 1)y = ex log x
C.F.-
Auxiliary equation is- D2 – 2D + 1= 0 or (D – 1)2 so that D = 1, 1
So that the C.F. Will be- (c1 + c2x)ex
P.I.-
Here y1 = ex , y2 = xex and X = ex log x
Now W =
Thus PI = -
So that the complete solution is-
y = (c1 + c2x)ex + ¼ x2 ex(2 log x – 3)
Q11)
A11)
Putting,
AE is
CS = CF + PI
Q12) Solve
A12)
Let,
AE is
y= CF + PI
Q13) Solve
A13)
As we see that this is Legendre’s linear equation.
Now put
So that-
And
Then the equation becomes- D (D – 1)y+ Dy + y = 2 sin t
Its auxiliary equation is-
And particular integral-
P.I. =
Note -
Hence the solution is -
Q14) Solve the following simultaneous differential equations-
....(2)
A14)
Consider the given equations
....(2)
Consider eq(1),(2)
Dx+2y = et....(1)
Dx +2x =e-t....(2)
Eliminating ‘x’ from both the equations we get,
12 2Dx + 2y = 2et
D 2Dx +D2y = e-t
y = Ae2t + Be-2t +
Q15) Solve the following simultaneous differential equations-
Given that x(0)=1 and y(0)= 0
A15)
Consider the given equations,
Dy +2x = sin2t
Dx -2y = cos2t
By solving the above equations, we get,
(D2 +4)Y =0
X(0) = 1, y(0) = 0
A =0, B=-1
Q16) Solve
(D2 + 8D + 15)y = 0
A16)
Given, (D2 + 8D + 15)y = 0
Here Auxiliary equation is
m2 – 8m + 15 = 9
m2 – 3m – 5m + 15 = 0
m(m – 3) – 5(m -3) = 0
(m – 3) (m – 5) = 0
m = 3, 5
y = C1e3x + C2 e5x
Q17) Solve: (D2 + 4)y = Cos 2x
A17)
Auxiliary equation are m2 + 4 = 0
CF = A Cos 2x + B Sin 2x
PI =
Put , D2 = - a2 = -22 = -4
PI =
PI = x
= x/4 Sin 2x
CS = CF + PR
= A Cos 2x + B Sin 2x + x/4 Sin 2x
Q18) Prove that-
A18)
As we know that-
Jn(x) =
Now put n = 1/2 in equation (1), then we get-
J1/2(x) =
Hence proved.
Q19) Prove that-
A19)
Put n = -1/2 in equation (1) of the above question, we get-
J1/2(x) =
Q20) Show that-
By using recurrence relation.
A20)
We know that-
The recurrence formula-
On differentiating, we get-
Now replace n by n -1 and n by n+1 in (1), we have-
2 J’n – 1 = Jn – 2 – Jn or J’n – 1 = ½ Jn – 2 – ½ Jn
2 J’n+1 = Jn – Jn+2 or J’n+1 = ½ Jn – ½ Jn+2
Put the values of and from the above equations in (2), we get-
2J’’n = ½ [ Jn-2 – Jn] – ½ [ Jn – Jn + 2]
4J’’n = Jn – 2 – Jn – Jn + Jn+2
4J’’n = Jn – 2 – 2 Jn + Jn+2
Q21) Prove that-
A21)
We know that- from recurrence formula
On integrating we get-
On taking n = 2 in (1), we get-
Again-
Put the value of from equation (2) and (3), we get-
By equation (1), when n = 1
Q22) Express in terms of Legendre polynomials.
A22)
By equating the coefficients of like powers of x, we get-
Put these values in equation (1), we get-
Q23) Let be the Legendre’s polynomial of degree n, then show that for every function f(x) for which the n’th derivative is continuous-
A23)
We know that-
On integrating by parts, we get-
Now integrate (n – 2) times by parts, we get-
Q24) Show that-
P2n(0) = (-1)n
A24)
We know that
Equating the coefficients of both sides, we have-
Q25) Prove that-
A25)
By using Rodrigue formula for Legendre function.
On integrating by parts, we get-
Now integrating m – 2 times, we get-