What is the general solution of the differential equation # y'''-y''+44y'-4=0 #?

Answer 1

# y = A + e^(1/2x){Bcos(sqrt(15)/2x) + Csin(sqrt(15)/2x)} + x#

We have:

# y'''-y''+44y'-4=0 #

Alternatively, as an alternative:

# y'''-y''+4y' = 4 # ..... [A]
This is a third order linear non-Homogeneous Differentiation Equation with constant coefficients. The standard approach is to find a solution, #y_c# of the homogeneous equation by looking at the Auxiliary Equation, which is the polynomial equation with the coefficients of the derivatives., and then finding an independent particular solution, #y_p# of the non-homogeneous equation.

Complementary Role

The equation homogeneous linked to [A] is

# y'''-y''+4y' = 0 # ..... [B]

Additionally, the related auxiliary equation is:

# m^3-m^2+4m = 0#
The challenge with higher order Differential Equation is solving the associated higher order Auxiliary equation. By inspection we see #m# is a factor, so we get::
# m(m^2-m+4) = 0#

We can also finish the square by:

# m((m-1/2)^2-(1/2)^2+4) = 0# # :. m((m-1/2)^2+4-1/4) = 0# # :. m((m-1/2)^2+15/4) = 0#

Consequently, we have the answers:

# m=0 # # (m-1/2)^2 = -15/4 => m = 1/2+sqrt(15)/2-#

Parts of the solution are determined by the auxiliary equation's roots; if these parts are linearly independent, the solutions' superposition forms the complete general solution.

Thus, the homogeneous equation [B] has the following solution:

# y = Ae^(0x) + e^(1/2x){Bcos(sqrt(15)/2x) + Csin(sqrt(15)/2x)}# # \ \ = A + e^(1/2x){Bcos(sqrt(15)/2x) + Csin(sqrt(15)/2x)}#

Specific Resolution

To identify a specific non-homogeneous equation solution:

# y'''-y''+4y' = f(x) \ \ # with #f(x)=4 # ..... [C]
then as #f(x)# is a polynomial of degree #0#, we would look for a polynomial solution of the same degree, i.e. of the form #y = a#
However, such a solution already exists in the CF solution and so must consider a potential solution of the form #y=ax#, Where the constants #a# is to be determined by direct substitution and comparison:
Differentiating #y=ax# wrt #x# we get:
# y' = a # # y'' = 0 # # y''' = 0 #

When we enter these outcomes into the DE [A], we obtain:

# 0-0+4a = 4 => a=1 #

Thus, we arrive at the specific solution:

# y_p = x #

Overall Resolution

which ultimately results in the GS of [A}

# y(x) = y_c + y_p # # \ \ \ \ \ \ \ = A + e^(1/2x){Bcos(sqrt(15)/2x) + Csin(sqrt(15)/2x)} + x#
Note this solution has #3# constants of integration and #3# linearly independent solutions, hence by the Existence and Uniqueness Theorem their superposition is the General Solution
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Answer 2
#"Characteristic equation is : "# #z^3 - z^2 + 4 z = 0# #=> z(z^2 - z + 4) = 0# #=> z = 0 " OR " z^2 - z + 4 = 0# #"disc of the quad. eq. = 1 - 16 = -15 < 0"# #"so we have two complex solutions, they are"# #z = (1 pm sqrt(15) i)/2# #"So the general solution of the homogeneous equation is : "# #A + B' exp(x/2) exp((sqrt(15)/2) i x) +# #C' exp(x/2) exp(-(sqrt(15)/2) i x)# #= A + B exp(x/2) cos(sqrt(15)x /2) + C exp(x/2) sin(sqrt(15) x/2)# #"The particular solution to the complete equation is"# #"y=x ,"# #"That is easy to see."# #"So the complete solution is :"# #y(x) = x + A + B exp(x/2) cos(sqrt(15) x/2) + C exp(x/2) sin(sqrt(15) x/2)#
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Answer 3

The general solution of the differential equation (y''' - y'' + 44y' - 4 = 0) is:

[y(t) = C_1 e^{2t} + C_2 e^{-2t} + C_3 e^{-22t} + \frac{1}{11}]

where (C_1), (C_2), and (C_3) are arbitrary constants.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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