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Introduction
1. Limits
2. Derivative basics
3. Advanced differentiation
4. Contextual uses
5. Analytical uses
6. Integration
7. Differential equations
7.1 Modeling & verifying solutions
7.2 Slope fields
7.3 Separation of variables
7.4 Exponential models
8. Applications of integrals
9. Testing details tag
Wrapping up
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7.3 Separation of variables
Achievable AP Calculus AB
7. Differential equations
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Separation of variables

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What you’ll learn:

  • How to solve first-order differential equations using separation of variables
  • How to apply initial conditions to find a particular solution

So far, you’ve seen differential equations like

dxdy​=2x

which can be solved by integrating both sides with respect to x. When the right-hand side depends on both x and y, a common method is separation of variables.

The idea is to rewrite the equation so that:

  • all y-terms (and dy) are on one side
  • all x-terms (and dx) are on the other side

This works when the differential equation can be written in the form

dxdy​=f(x)⋅g(y)

If the equation can’t be rewritten as a product of a function of x and a function of y, then separation of variables won’t apply.

Examples

Find the particular solution to the differential equation

dxdy​=ex−y

given the initial condition y(0)=ln(5).

Step 1: Rewrite the equation to separate the variables

Start by rewriting the exponential so the x and y parts are separated:

dxdy​=ex−y=eyex​

A reliable way to separate variables is:

  • multiply both sides by dx
  • move the expression with y to the side with dy

In this case, multiplying both sides by dx and ey gives:

eydy=exdx

Step 2: Integrate both sides

∫eydy=∫exdx

ey=ex+C

Because the integral is indefinite, add the constant of integration C.

Conventionally, it’s added to the side with the independent variable (in this case, x), or the right hand-side.

Step 3: Apply the initial condition if given

If no initial condition is given, solve for y to get the general solution.

However, in this case the initial condition is y(0)=ln(5), meaning we substitute x=0 and y=ln(5) to find C:

eln(5)=e0+C

5=1+C

C=4

So the equation becomes

ey=ex+4

Now solve for y by taking the natural log of both sides:

ln(ey)=ln(ex+4)

y=ln(ex+4)​

This is the specific solution that satisfies the differential equation.

Next is an example to find the general solution using separation of variables. The answer will include C.

Find the general solution to

dxdy​=y+yx2

Solution

(spoiler)

First, factor the right-hand side so it’s written as a product:

dxdy​=y(1+x2)

Now separate the variables. Multiply by dx, then divide by y:

y1​dy=(1+x2)dx

Integrate both sides:

∫y1​dy=∫(1+x2)dx

ln∣y∣=x+3x3​+C

Solve for y by exponentiating both sides:

eln∣y∣=ex+3x3​+C

∣y∣=ex+3x3​+C

Using the product rule of exponents, rewrite the equation as:

∣y∣=ex+3x3​⋅eC

Since eC>0, we can absorb the sign from the absolute value into the constant and redefine it as an arbitrary nonzero real constant C. This gives the general solution:

y=Cex+3x3​​

Note: Exponential solutions are typically written in this form, with the constant multiplied in front of the exponential, for clarity and simplicity.

Find the particular solution to

dxdy​=xy2

with the initial condition y(0)=1.

Solution

(spoiler)

Separate the variables:

y21​dy=xdx

Integrate both sides:

∫y21​dy=∫xdx

−y1​=2x2​+C

Use the initial condition (x,y)=(0,1) to find C:

−11​=202​+C

C=−1

Substitute C=−1 and solve for y:

−y1​=2x2​−1

Multiply both sides by y:

−1=(2x2​−1)y

Divide to isolate y:

y=2x2​−1−1​=2x2−2​−1​

y=−x2−22​​

Find the particular solution to

dxdy​=y+1

with the initial condition y(2)=0

Solution

(spoiler)

Separate the variables:

y+11​dy=dx

Integrate both sides. On the left, u-substitution with u=y+1 is used.

∫y+11​dy=∫1dx

ln∣y+1∣=x+C

Use the initial condition (x,y)=(2,0) to find C:

ln(0+1)0C​=2+C=2+C=−2​

Substitute C=−2 and solve for y:

ln∣y+1∣eln∣y+1∣y+1​=x−2=ex−2=ex−2​

y=ex−2−1​

If

dtdy​=y2t+1​

and y=2 when t=0, find y when t=1.

Solution

(spoiler)

Even though the variables are y and t (instead of y and x), the separation steps are the same.

Separate the variables:

ydy=(2t+1)dt

Integrate both sides:

∫ydy=∫(2t+1)dt

2y2​=t2+t+C

Use the initial condition y=2 when t=0 to find C:

222​=02+0+C

2=C

So

2y2​=t2+t+2

y2=2t2+2t+4

y=±2t2+2t+4​

Note: The initial condition y(0)=2 tells you y is positive at t=0, so take the positive branch:

y=2t2+2t+4​

Now evaluate at t=1:

y=2(1)2+2(1)+4​

=2+2+4​

=22​

Lastly, here is a problem similar to a multi-part free-response question from the 2022 AB exam:

Consider the differential equation

dxdy​=πcos(πx)y​

Let y=f(x) be the particular solution to the differential equation with initial condition f(1)=4.

a) Write an equation for the line tangent to the solution curve at the point (1,4) and use it to approximate f(0.9).

b) Given f′′(x)<0 for −1≤x≤1, is the approximation from part a) an overestimate or underestimate for f(0.9)?

c) Use separation of variables to find the particular solution to the differential equation with initial condition f(1)=4.

Solutions

a) Equation of tangent line at (1,4)

(spoiler)

The equation of the tangent line to y=f(x) at (a,f(a)) is

y−f(a)=f′(a)(x−a)

Here, (a,f(a))=(1,4). To find f′(1), evaluate the differential equation at x=1 and y=4:

dxdy​​x=1,y=4​=πcos(π⋅1)4​

=π(−1)(2)

=−2π

So the tangent line is

y−4=−2π(x−1)​

To approximate f(0.9), plug x=0.9 into the tangent line:

y−4=−2π(0.9−1)

y=−2π(−0.1)+4

f(0.9)≈0.2π+4​

b) Underestimate or overestimate?

(spoiler)

Since f′′(x)<0 on −1≤x≤1, the graph is concave down on that interval.

For a concave down function, the tangent line lies above the curve. That means the tangent-line (linear) approximation from part (a) is an overestimate of the actual value f(0.9).

c) Particular solution with f(1)=4

(spoiler)

Separate the variables:

y​1​dy=πcos(πx)dx

Integrate both sides:

∫y​1​dy=∫πcos(πx)dx

Rewrite the left integrand as a power:

∫y−1/2dy=sin(πx)+C

2y1/2=sin(πx)+C

Use the initial condition (1,4) to find C:

24​=sin(π⋅1)+C

4=0+C

C=4

Now solve for y:

2y1/2=sin(πx)+4

y1/2=21​sin(πx)+2

y=(21​sin(πx)+2)2​

Separation of variables

  • Used for first-order differential equations of the form dxdy​=f(x)g(y)
  • Rearrange to isolate y-terms with dy and x-terms with dx
  • Integrate both sides to solve

Applying initial conditions

  • Substitute given (x,y) values after integrating to solve for the constant C
  • Plug C back into the general solution for the particular solution

Example 1: dxdy​=ex−y, y(0)=ln(5)

  • Separate: eydy=exdx
  • Integrate: ey=ex+C
  • Apply initial condition: C=4
  • Solution: y=ln(ex+4)

Example 2: dxdy​=y+yx2

  • Factor: y(1+x2)
  • Separate: y1​dy=(1+x2)dx
  • Integrate: ln∣y∣=x+3x3​+C
  • General solution: y=Cex+x3/3

Example 3: dxdy​=xy2, y(0)=1

  • Separate: y21​dy=xdx
  • Integrate: −y1​=2x2​+C
  • Apply initial condition: C=−1
  • Solution: y=−x2−22​

Example 4: dxdy​=y+1, y(2)=0

  • Separate: y+11​dy=dx
  • Integrate: ln(y+1)=x+C
  • Apply initial condition: C=−2
  • Solution: y=ex−2−1

Example 5: dtdy​=y2t+1​, y(0)=2

  • Separate: ydy=(2t+1)dt
  • Integrate: 2y2​=t2+t+C
  • Apply initial condition: C=2
  • Solution: y=2t2+2t+4​
  • At t=1: y=22​

Tangent line approximation and concavity

  • Tangent line at (x0​,y0​): y−y0​=f′(x0​)(x−x0​)
  • If f′′(x)<0, function is concave down
    • Tangent line overestimates function near x0​

Example 6: dxdy​=πcos(πx)y​, f(1)=4

  • Tangent line at (1,4): y−4=−2π(x−1)
  • Approximate f(0.9): f(0.9)≈0.2π+4
  • Concavity: f′′(x)<0 implies tangent overestimates f(0.9)
  • Separate: y​1​dy=πcos(πx)dx
  • Integrate: 2y1/2=sin(πx)+C
  • Apply initial condition: C=4
  • Solution: y=(21​sin(πx)+2)2

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Separation of variables

What you’ll learn:

  • How to solve first-order differential equations using separation of variables
  • How to apply initial conditions to find a particular solution

So far, you’ve seen differential equations like

dxdy​=2x

which can be solved by integrating both sides with respect to x. When the right-hand side depends on both x and y, a common method is separation of variables.

The idea is to rewrite the equation so that:

  • all y-terms (and dy) are on one side
  • all x-terms (and dx) are on the other side

This works when the differential equation can be written in the form

dxdy​=f(x)⋅g(y)

If the equation can’t be rewritten as a product of a function of x and a function of y, then separation of variables won’t apply.

Examples

Find the particular solution to the differential equation

dxdy​=ex−y

given the initial condition y(0)=ln(5).

Step 1: Rewrite the equation to separate the variables

Start by rewriting the exponential so the x and y parts are separated:

dxdy​=ex−y=eyex​

A reliable way to separate variables is:

  • multiply both sides by dx
  • move the expression with y to the side with dy

In this case, multiplying both sides by dx and ey gives:

eydy=exdx

Step 2: Integrate both sides

∫eydy=∫exdx

ey=ex+C

Because the integral is indefinite, add the constant of integration C.

Conventionally, it’s added to the side with the independent variable (in this case, x), or the right hand-side.

Step 3: Apply the initial condition if given

If no initial condition is given, solve for y to get the general solution.

However, in this case the initial condition is y(0)=ln(5), meaning we substitute x=0 and y=ln(5) to find C:

eln(5)=e0+C

5=1+C

C=4

So the equation becomes

ey=ex+4

Now solve for y by taking the natural log of both sides:

ln(ey)=ln(ex+4)

y=ln(ex+4)​

This is the specific solution that satisfies the differential equation.

Next is an example to find the general solution using separation of variables. The answer will include C.

Find the general solution to

dxdy​=y+yx2

Solution

(spoiler)

First, factor the right-hand side so it’s written as a product:

dxdy​=y(1+x2)

Now separate the variables. Multiply by dx, then divide by y:

y1​dy=(1+x2)dx

Integrate both sides:

∫y1​dy=∫(1+x2)dx

ln∣y∣=x+3x3​+C

Solve for y by exponentiating both sides:

eln∣y∣=ex+3x3​+C

∣y∣=ex+3x3​+C

Using the product rule of exponents, rewrite the equation as:

∣y∣=ex+3x3​⋅eC

Since eC>0, we can absorb the sign from the absolute value into the constant and redefine it as an arbitrary nonzero real constant C. This gives the general solution:

y=Cex+3x3​​

Note: Exponential solutions are typically written in this form, with the constant multiplied in front of the exponential, for clarity and simplicity.

Find the particular solution to

dxdy​=xy2

with the initial condition y(0)=1.

Solution

(spoiler)

Separate the variables:

y21​dy=xdx

Integrate both sides:

∫y21​dy=∫xdx

−y1​=2x2​+C

Use the initial condition (x,y)=(0,1) to find C:

−11​=202​+C

C=−1

Substitute C=−1 and solve for y:

−y1​=2x2​−1

Multiply both sides by y:

−1=(2x2​−1)y

Divide to isolate y:

y=2x2​−1−1​=2x2−2​−1​

y=−x2−22​​

Find the particular solution to

dxdy​=y+1

with the initial condition y(2)=0

Solution

(spoiler)

Separate the variables:

y+11​dy=dx

Integrate both sides. On the left, u-substitution with u=y+1 is used.

∫y+11​dy=∫1dx

ln∣y+1∣=x+C

Use the initial condition (x,y)=(2,0) to find C:

ln(0+1)0C​=2+C=2+C=−2​

Substitute C=−2 and solve for y:

ln∣y+1∣eln∣y+1∣y+1​=x−2=ex−2=ex−2​

y=ex−2−1​

If

dtdy​=y2t+1​

and y=2 when t=0, find y when t=1.

Solution

(spoiler)

Even though the variables are y and t (instead of y and x), the separation steps are the same.

Separate the variables:

ydy=(2t+1)dt

Integrate both sides:

∫ydy=∫(2t+1)dt

2y2​=t2+t+C

Use the initial condition y=2 when t=0 to find C:

222​=02+0+C

2=C

So

2y2​=t2+t+2

y2=2t2+2t+4

y=±2t2+2t+4​

Note: The initial condition y(0)=2 tells you y is positive at t=0, so take the positive branch:

y=2t2+2t+4​

Now evaluate at t=1:

y=2(1)2+2(1)+4​

=2+2+4​

=22​

Lastly, here is a problem similar to a multi-part free-response question from the 2022 AB exam:

Consider the differential equation

dxdy​=πcos(πx)y​

Let y=f(x) be the particular solution to the differential equation with initial condition f(1)=4.

a) Write an equation for the line tangent to the solution curve at the point (1,4) and use it to approximate f(0.9).

b) Given f′′(x)<0 for −1≤x≤1, is the approximation from part a) an overestimate or underestimate for f(0.9)?

c) Use separation of variables to find the particular solution to the differential equation with initial condition f(1)=4.

Solutions

a) Equation of tangent line at (1,4)

(spoiler)

The equation of the tangent line to y=f(x) at (a,f(a)) is

y−f(a)=f′(a)(x−a)

Here, (a,f(a))=(1,4). To find f′(1), evaluate the differential equation at x=1 and y=4:

dxdy​​x=1,y=4​=πcos(π⋅1)4​

=π(−1)(2)

=−2π

So the tangent line is

y−4=−2π(x−1)​

To approximate f(0.9), plug x=0.9 into the tangent line:

y−4=−2π(0.9−1)

y=−2π(−0.1)+4

f(0.9)≈0.2π+4​

b) Underestimate or overestimate?

(spoiler)

Since f′′(x)<0 on −1≤x≤1, the graph is concave down on that interval.

For a concave down function, the tangent line lies above the curve. That means the tangent-line (linear) approximation from part (a) is an overestimate of the actual value f(0.9).

c) Particular solution with f(1)=4

(spoiler)

Separate the variables:

y​1​dy=πcos(πx)dx

Integrate both sides:

∫y​1​dy=∫πcos(πx)dx

Rewrite the left integrand as a power:

∫y−1/2dy=sin(πx)+C

2y1/2=sin(πx)+C

Use the initial condition (1,4) to find C:

24​=sin(π⋅1)+C

4=0+C

C=4

Now solve for y:

2y1/2=sin(πx)+4

y1/2=21​sin(πx)+2

y=(21​sin(πx)+2)2​

Key points

Separation of variables

  • Used for first-order differential equations of the form dxdy​=f(x)g(y)
  • Rearrange to isolate y-terms with dy and x-terms with dx
  • Integrate both sides to solve

Applying initial conditions

  • Substitute given (x,y) values after integrating to solve for the constant C
  • Plug C back into the general solution for the particular solution

Example 1: dxdy​=ex−y, y(0)=ln(5)

  • Separate: eydy=exdx
  • Integrate: ey=ex+C
  • Apply initial condition: C=4
  • Solution: y=ln(ex+4)

Example 2: dxdy​=y+yx2

  • Factor: y(1+x2)
  • Separate: y1​dy=(1+x2)dx
  • Integrate: ln∣y∣=x+3x3​+C
  • General solution: y=Cex+x3/3

Example 3: dxdy​=xy2, y(0)=1

  • Separate: y21​dy=xdx
  • Integrate: −y1​=2x2​+C
  • Apply initial condition: C=−1
  • Solution: y=−x2−22​

Example 4: dxdy​=y+1, y(2)=0

  • Separate: y+11​dy=dx
  • Integrate: ln(y+1)=x+C
  • Apply initial condition: C=−2
  • Solution: y=ex−2−1

Example 5: dtdy​=y2t+1​, y(0)=2

  • Separate: ydy=(2t+1)dt
  • Integrate: 2y2​=t2+t+C
  • Apply initial condition: C=2
  • Solution: y=2t2+2t+4​
  • At t=1: y=22​

Tangent line approximation and concavity

  • Tangent line at (x0​,y0​): y−y0​=f′(x0​)(x−x0​)
  • If f′′(x)<0, function is concave down
    • Tangent line overestimates function near x0​

Example 6: dxdy​=πcos(πx)y​, f(1)=4

  • Tangent line at (1,4): y−4=−2π(x−1)
  • Approximate f(0.9): f(0.9)≈0.2π+4
  • Concavity: f′′(x)<0 implies tangent overestimates f(0.9)
  • Separate: y​1​dy=πcos(πx)dx
  • Integrate: 2y1/2=sin(πx)+C
  • Apply initial condition: C=4
  • Solution: y=(21​sin(πx)+2)2