General Solution of a First Order Linear Differential Equation A first order linear differential equation is one that can be put in the form dy + P(z)y= Q(z) dr where Pand Q are continuous functions on a given interval. This form is called the standard form and is readily solved by multiplying both sides of the equation by an integrating factor, u(z) = eS P(z) dz_ In this problem, we want to find the general solution of the equation dy y = -(2x7 + 12z4) , x >0 dr Part 1. We will begin by finding an integrating factor using the formula above, µ(x) = eS P(z) dz H(z) Hint: you should first re-write the equation in standard form. Part 2. Next, we multiply both sides of the differential equation by µ(2) and re-write the left hand side as the derivative of a product giving us: dz Part 3. Finally, upon integrating both sides with respect to z and solving for y we have: NOTE: Type 'C'for the arbitrary constant in the general solution.
General Solution of a First Order Linear Differential Equation A first order linear differential equation is one that can be put in the form dy + P(z)y= Q(z) dr where Pand Q are continuous functions on a given interval. This form is called the standard form and is readily solved by multiplying both sides of the equation by an integrating factor, u(z) = eS P(z) dz_ In this problem, we want to find the general solution of the equation dy y = -(2x7 + 12z4) , x >0 dr Part 1. We will begin by finding an integrating factor using the formula above, µ(x) = eS P(z) dz H(z) Hint: you should first re-write the equation in standard form. Part 2. Next, we multiply both sides of the differential equation by µ(2) and re-write the left hand side as the derivative of a product giving us: dz Part 3. Finally, upon integrating both sides with respect to z and solving for y we have: NOTE: Type 'C'for the arbitrary constant in the general solution.
Calculus: Early Transcendentals
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ISBN:9781285741550
Author:James Stewart
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![General Solution of a First Order Linear Differential Equation
A first order linear differential equation is one that can be put in the form
dy
+ P(z)y= Q(z)
dr
where Pand Q are continuous functions on a given interval. This form is called the standard form and is readily solved by multiplying both sides of the equation by an
integrating factor, u(z) = eS P(z) dz_
In this problem, we want to find the general solution of the equation
dy
y = -(2x7 + 12z4) , x >0
dr
Part 1.
We will begin by finding an integrating factor using the formula above, µ(x) = eS P(z) dz
H(z)
Hint: you should first re-write the equation in standard form.
Part 2.
Next, we multiply both sides of the differential equation by µ(2) and re-write the left hand side as the derivative of a product giving us:
dz
Part 3.
Finally, upon integrating both sides with respect to z and solving for y we have:
NOTE: Type 'C'for the arbitrary constant in the general solution.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F2e521a1e-f4ee-4c02-af71-8dfc2cc184d3%2F5d8f75a6-15b6-494d-98d5-ccd05505dda9%2Ffr1fzei_processed.png&w=3840&q=75)
Transcribed Image Text:General Solution of a First Order Linear Differential Equation
A first order linear differential equation is one that can be put in the form
dy
+ P(z)y= Q(z)
dr
where Pand Q are continuous functions on a given interval. This form is called the standard form and is readily solved by multiplying both sides of the equation by an
integrating factor, u(z) = eS P(z) dz_
In this problem, we want to find the general solution of the equation
dy
y = -(2x7 + 12z4) , x >0
dr
Part 1.
We will begin by finding an integrating factor using the formula above, µ(x) = eS P(z) dz
H(z)
Hint: you should first re-write the equation in standard form.
Part 2.
Next, we multiply both sides of the differential equation by µ(2) and re-write the left hand side as the derivative of a product giving us:
dz
Part 3.
Finally, upon integrating both sides with respect to z and solving for y we have:
NOTE: Type 'C'for the arbitrary constant in the general solution.
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