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MATH-182 (Calculus II) Curriculum

Session 04 - U Substitution

Handout Worksheet
Fall Semester 2026
Session Objectives & Overview
  • Algebraic Flexibility Rewriting and Variable Manipulation
  • Pattern Recognition Spotting the Inner Function and its Derivative
  • Precision in Mechanics Handling Constants, Limits, and Core Rules

Micro-Lecture

Engineering Context: Engineering Calculus II Application

In engineering, mastering the substitution rule is essential for modeling and controlling the physical world, as it translates complex mathematical systems into simpler, solvable forms. For example, electrical engineers use the mechanics of introducing constants to evaluate dynamic AC power and exponential capacitor charging integrals , while civil and mechanical engineers rely on pattern recognition to isolate trapped "inner functions" when mapping hydrostatic fluid pressure and structural stress. Additionally, aerospace engineers and roboticists employ variable manipulation to transform complex three-dimensional paths into simpler coordinate systems , while chemical and nuclear engineers depend on absolute precision when transforming definite integration limits to ensure thermal safety systems deploy at the exact correct physical thresholds. Ultimately, the ability to successfully substitute a complex expression with a single manageable variable allows engineers to efficiently calculate the critical, real-time equations that keep modern infrastructure, flight guidance software, and power grids operating safely.

Skill Block 1

Worked Example

∫(2x+1)x2+x5 dx\int (2x+1)\sqrt[5]{x^{2}+x} \, dx∫(2x+1)5x2+x​dx

Worked Solution:

We want to evaluate the following indefinite integral:

∫(2x+1)x2+x5 dx\int (2x+1)\sqrt[5]{x^2+x} \, dx∫(2x+1)5x2+x​dx

This problem is a perfect candidate for uuu-substitution because the derivative of the expression inside the radical, x2+xx^2 + xx2+x, is exactly the other term in the integrand, 2x+12x + 12x+1.

Step 1: Choose uuu and find dududu

Let's define our substitute variable uuu as the inside function:

u=x2+xu = x^2 + xu=x2+x

Now, take the derivative of uuu with respect to xxx to find dududu:

du=(2x+1) dxdu = (2x + 1) \, dxdu=(2x+1)dx

Step 2: Substitute uuu and dududu into the original integral

Notice how the pieces of our original integral perfectly match our substitution components:

  • x2+x5\sqrt[5]{x^2+x}5x2+x​ becomes u5\sqrt[5]{u}5u​ (or u1/5u^{1/5}u1/5)
  • (2x+1) dx(2x + 1) \, dx(2x+1)dx becomes dududu

Rewriting the integral gives:

∫u1/5 du\int u^{1/5} \, du∫u1/5du

Step 3: Integrate with respect to uuu

Using the power rule for integration, ∫un du=un+1n+1+C\int u^n \, du = \frac{u^{n+1}}{n+1} + C∫undu=n+1un+1​+C:

∫u1/5 du=u15+115+1+C\int u^{1/5} \, du = \frac{u^{\frac{1}{5} + 1}}{\frac{1}{5} + 1} + C∫u1/5du=51​+1u51​+1​+C

=u6/565+C\quad = \frac{u^{6/5}}{\frac{6}{5}} + C=56​u6/5​+C

=56u6/5+C\quad = \frac{5}{6}u^{6/5} + C=65​u6/5+C

Step 4: Substitute the original expression back in

Finally, replace uuu with our original expression x2+xx^2 + xx2+x to get the final answer in terms of xxx:

56(x2+x)6/5+C\frac{5}{6}(x^2 + x)^{6/5} + C65​(x2+x)6/5+C

56(x2+x)65+C\frac{5}{6}\sqrt[5]{(x^2 + x)^6} + C65​5(x2+x)6​+C
(Note: CCC represents the constant of integration.)

Active Practice Problem

∫xx2+1 dx\int \frac{x}{x^{2}+1} \, dx∫x2+1x​dx

Solution Key:

We want to evaluate the following indefinite integral:

∫xx2+1 dx\int \frac{x}{x^2+1} \, dx∫x2+1x​dx

This is another classic uuu-substitution problem. The degree of the polynomial in the denominator (x2+1x^2+1x2+1) is 2, and the degree of the numerator (xxx) is 1. Since the numerator is a scalar multiple of the derivative of the denominator, uuu-substitution is the perfect tool.

Step 1: Choose uuu and find dududu

Let's set uuu equal to the entire denominator:

u=x2+1u = x^2 + 1u=x2+1

Now, take the derivative of uuu with respect to xxx:

du=2x dxdu = 2x \, dxdu=2xdx

Step 2: Adjust for the coefficients

Looking at our original integral, the numerator only has x dxx \, dxxdx, not 2x dx2x \, dx2xdx. We can adjust our dududu equation by dividing both sides by 2:

12 du=x dx\frac{1}{2} \, du = x \, dx21​du=xdx

Step 3: Substitute into the original integral

Now replace the terms in the original integral with uuu and dududu:

  • The denominator x2+1x^2 + 1x2+1 becomes uuu.
  • The numerator and differential x dxx \, dxxdx become 12 du\frac{1}{2} \, du21​du.

∫xx2+1 dx=∫1u⋅(12 du)\int \frac{x}{x^2+1} \, dx = \int \frac{1}{u} \cdot \left(\frac{1}{2} \, du\right)∫x2+1x​dx=∫u1​⋅(21​du)

Pull the constant factor 12\frac{1}{2}21​ outside the integral:

12∫1u du\frac{1}{2} \int \frac{1}{u} \, du21​∫u1​du

Step 4: Integrate with respect to uuu

The integral of 1u\frac{1}{u}u1​ is a standard rule: ∫1u du=ln⁡∣u∣+C\int \frac{1}{u} \, du = \ln|u| + C∫u1​du=ln∣u∣+C.

12∫1u du=12ln⁡∣u∣+C\frac{1}{2} \int \frac{1}{u} \, du = \frac{1}{2} \ln|u| + C21​∫u1​du=21​ln∣u∣+C

Step 5: Substitute the original expression back in

Replace uuu with x2+1x^2 + 1x2+1:

12ln⁡(x2+1)+C\frac{1}{2} \ln(x^2 + 1) + C21​ln(x2+1)+C
(Note: Because x2+1x^2 + 1x2+1 is always positive for any real number xxx, you can safely drop the absolute value bars and use parentheses instead).

12ln⁡(x2+1)+C\frac{1}{2} \ln(x^2 + 1) + C21​ln(x2+1)+C

Show your steps and calculations here.

Regroup 1

  • Review common misconceptions and clarify key notations.

Skill Block 2

Worked Example

∫0π/4tan⁡(x)sec⁡2(x) dx\int_{0}^{\pi/4} \tan(x)\sec^{2}(x) \, dx∫0π/4​tan(x)sec2(x)dx

Worked Solution:

We want to evaluate the following definite integral:

∫0π/4tan⁡(x)sec⁡2(x) dx\int_{0}^{\pi/4} \tan(x)\sec^2(x) \, dx∫0π/4​tan(x)sec2(x)dx

This problem is a classic trigonometry-based uuu-substitution. Since the derivative of tan⁡(x)\tan(x)tan(x) is exactly sec⁡2(x)\sec^2(x)sec2(x), we have a perfect pairing ready to go. Because this is a definite integral (it has upper and lower limits), we also need to update our limits of integration when we switch from xxx to uuu.

Step 1: Choose uuu and find dududu

Let's choose our substitution variable:

u=tan⁡(x)u = \tan(x)u=tan(x)

Now, take the derivative of uuu with respect to xxx:

du=sec⁡2(x) dxdu = \sec^2(x) \, dxdu=sec2(x)dx

Step 2: Convert the limits of integration

Since we are changing variables from xxx to uuu, we must plug the original xxx limits into our substitution equation (u=tan⁡(x)u = \tan(x)u=tan(x)) to find the new uuu limits.

  • Lower limit (x=0x = 0x=0):
    u=tan⁡(0)=0u = \tan(0) = 0u=tan(0)=0
  • Upper limit (x=π4x = \frac{\pi}{4}x=4π​):
    u=tan⁡(π4)=1u = \tan\left(\frac{\pi}{4}\right) = 1u=tan(4π​)=1
Step 3: Substitute into the integral

Now, swap out all the xxx components for their uuu equivalents:

  • The limits change from 0→π40 \to \frac{\pi}{4}0→4π​ to 0→10 \to 10→1.
  • tan⁡(x)\tan(x)tan(x) becomes uuu.
  • sec⁡2(x) dx\sec^2(x) \, dxsec2(x)dx becomes dududu.

∫01u du\int_{0}^{1} u \, du∫01​udu

Step 4: Integrate and evaluate

Using the power rule for integration (∫u du=12u2\int u \, du = \frac{1}{2}u^2∫udu=21​u2), we evaluate from 000 to 111:

[12u2]01\left[ \frac{1}{2}u^2 \right]_{0}^{1}[21​u2]01​

Now, apply the Fundamental Theorem of Calculus:

(12(1)2)−(12(0)2)=12−0=12\left( \frac{1}{2}(1)^2 \right) - \left( \frac{1}{2}(0)^2 \right) = \frac{1}{2} - 0 = \frac{1}{2}(21​(1)2)−(21​(0)2)=21​−0=21​

12\frac{1}{2}21​
(Fun side note: You can solve this by picking u=sec⁡(x)u = \sec(x)u=sec(x) instead. If you try it that way, your new limits will be 111 to 2\sqrt{2}2​, but the math beautifully shakes out to give you the exact same answer!)

Active Practice Problem

∫13e1/xx2 dx\int_{1}^{3} \frac{e^{1/x}}{x^{2}} \, dx∫13​x2e1/x​dx

Solution Key:

We want to evaluate the following definite integral:

∫13e1/xx2 dx\int_{1}^{3} \frac{e^{1/x}}{x^2} \, dx∫13​x2e1/x​dx

This problem is a great candidate for uuu-substitution. If we rewrite the fraction slightly, it looks like ∫13e1/x⋅1x2 dx\int_{1}^{3} e^{1/x} \cdot \frac{1}{x^2} \, dx∫13​e1/x⋅x21​dx. Since the derivative of 1x\frac{1}{x}x1​ is closely related to 1x2\frac{1}{x^2}x21​, we can set up our substitution perfectly.

Step 1: Choose uuu and find dududu

Let's choose the exponent of eee as our substitute variable:

u=1x=x−1u = \frac{1}{x} = x^{-1}u=x1​=x−1

Now, take the derivative of uuu with respect to xxx using the power rule:

du=−1x−2 dx=−1x2 dxdu = -1x^{-2} \, dx = -\frac{1}{x^2} \, dxdu=−1x−2dx=−x21​dx

Since our original integral has a positive 1x2 dx\frac{1}{x^2} \, dxx21​dx, let's move the negative sign to the other side:

−du=1x2 dx-du = \frac{1}{x^2} \, dx−du=x21​dx

Step 2: Convert the limits of integration

Because this is a definite integral, we need to update our lower and upper limits from xxx-values to uuu-values using our formula u=1xu = \frac{1}{x}u=x1​.

  • Lower limit (x=1x = 1x=1):
    u=11=1u = \frac{1}{1} = 1u=11​=1
  • Upper limit (x=3x = 3x=3):
    u=13u = \frac{1}{3}u=31​
Step 3: Substitute into the integral

Now, swap the xxx variables and limits with their uuu counterparts:

  • The limits change from 1→31 \to 31→3 to 1→131 \to \frac{1}{3}1→31​.
  • e1/xe^{1/x}e1/x becomes eue^ueu.
  • 1x2 dx\frac{1}{x^2} \, dxx21​dx becomes −du-du−du.

∫11/3eu(−du)=−∫11/3eu du\int_{1}^{1/3} e^u (-du) = -\int_{1}^{1/3} e^u \, du∫11/3​eu(−du)=−∫11/3​eudu

Pro-Tip: You can use the negative sign outside the integral to flip the lower and upper limits of integration back into standard increasing order:

∫1/31eu du\int_{1/3}^{1} e^u \, du∫1/31​eudu

Step 4: Integrate and evaluate

The integral of eue^ueu is simply eue^ueu. Now we evaluate it from 13\frac{1}{3}31​ to 111:

[eu]1/31\left[ e^u \right]_{1/3}^{1}[eu]1/31​

Apply the Fundamental Theorem of Calculus:

e1−e1/3=e−e3e^1 - e^{1/3} = e - \sqrt[3]{e}e1−e1/3=e−3e​

e−e3e - \sqrt[3]{e}e−3e​

Show your steps and calculations here.

Regroup 2

  • Reflect on the physical modeling applications and mathematical setups.

Skill Block 3

Standard Sample Problem

Solution Key:
  • Step 1: Choose uuu and calculate dududu . The inner function of the sine expression is 2x2x2x.

    u=2xu = 2xu=2x
    du=2 dxdu = 2 \, dxdu=2dx

  • Step 2: Balance the constant factor. The original integrand contains only dxdxdx, not 2 dx2 \, dx2dx. Divide both sides by 2 to balance the differential component:

    12 du=dx\frac{1}{2} \, du = dx21​du=dx

  • Step 3: Transform the integration limits . Use the boundary tracking formula u=2xu = 2xu=2x to convert the limits from xxx to uuu:

    • Lower limit: When x=0  ⟹  u=2(0)=0x = 0 \implies u = 2(0) = 0x=0⟹u=2(0)=0
    • Upper limit: When x=π2  ⟹  u=2(π2)=πx = \frac{\pi}{2} \implies u = 2\left(\frac{\pi}{2}\right) = \pix=2π​⟹u=2(2π​)=π
  • Step 4: Rewrite and integrate in terms of uuu . Substitute the updated limits (0→π0 \to \pi0→π), replace 2x2x2x with uuu, and swap dxdxdx for 12 du\frac{1}{2} \, du21​du:

    ∫0πsin⁡(u)⋅12 du=12∫0πsin⁡(u) du\int_{0}^{\pi} \sin(u) \cdot \frac{1}{2} \, du = \frac{1}{2} \int_{0}^{\pi} \sin(u) \, du∫0π​sin(u)⋅21​du=21​∫0π​sin(u)du

    The antiderivative of sin⁡(u)\sin(u)sin(u) is −cos⁡(u)-\cos(u)−cos(u):

    [−12cos⁡(u)]0π\left[ -\frac{1}{2}\cos(u) \right]_{0}^{\pi}[−21​cos(u)]0π​

  • Step 5: Numerically evaluate the boundaries . Apply the fundamental integration limits directly to the uuu terms without reverting back to xxx:

    (−12cos⁡(π))−(−12cos⁡(0))\left(-\frac{1}{2}\cos(\pi)\right) - \left(-\frac{1}{2}\cos(0)\right)(−21​cos(π))−(−21​cos(0))

    Knowing cos⁡(π)=−1\cos(\pi) = -1cos(π)=−1 and cos⁡(0)=1\cos(0) = 1cos(0)=1:

    (−12⋅(−1))+(12⋅1)=12+12=1\left(-\frac{1}{2} \cdot (-1)\right) + \left(\frac{1}{2} \cdot 1\right) = \frac{1}{2} + \frac{1}{2} = 1(−21​⋅(−1))+(21​⋅1)=21​+21​=1

Worked Example

∫x3−x dx\int x\sqrt{3-x} \, dx∫x3−x​dx

Worked Solution:

We want to evaluate the following indefinite integral:

∫x3−x dx\int x\sqrt{3-x} \, dx∫x3−x​dx

This problem uses a special twist on uuu-substitution often called back-substitution. Notice that if we set u=3−xu = 3-xu=3−x, its derivative is just −1-1−1, which doesn't automatically cancel out the xxx sitting outside the radical. To fix this, we will solve our substitution equation for xxx and substitute that in too!

Step 1: Choose uuu and find dududu

Let's choose the expression under the radical to be our uuu:

u=3−xu = 3 - xu=3−x

Now, find dududu:

du=−1 dx  ⟹  −du=dxdu = -1 \, dx \implies -du = dxdu=−1dx⟹−du=dx

Step 2: Solve for xxx in terms of uuu

Since we have an extra xxx left over in the integrand, let's rearrange our original uuu equation to isolate xxx:

u=3−xu = 3 - xu=3−x
x=3−ux = 3 - ux=3−u

Step 3: Substitute everything into the original integral

Now replace every single part of the original xxx-integral with its uuu equivalent:

  • xxx becomes (3−u)(3 - u)(3−u)
  • 3−x\sqrt{3-x}3−x​ becomes u\sqrt{u}u​ (or u1/2u^{1/2}u1/2)
  • dxdxdx becomes −du-du−du

∫(3−u)⋅u1/2⋅(−du)\int (3 - u) \cdot u^{1/2} \cdot (-du)∫(3−u)⋅u1/2⋅(−du)

Pull the negative sign out front:

−∫(3−u)u1/2 du-\int (3 - u)u^{1/2} \, du−∫(3−u)u1/2du

Step 4: Distribute and integrate

Before integrating, distribute u1/2u^{1/2}u1/2 into the parentheses:

−∫(3u1/2−u3/2) du-\int (3u^{1/2} - u^{3/2}) \, du−∫(3u1/2−u3/2)du

Distribute the negative sign to make the power rule cleaner:

∫(u3/2−3u1/2) du\int (u^{3/2} - 3u^{1/2}) \, du∫(u3/2−3u1/2)du

Now, apply the power rule to each term:

  • For u3/2u^{3/2}u3/2: 25u5/2\frac{2}{5}u^{5/2}52​u5/2
  • For 3u1/23u^{1/2}3u1/2: 2u3/22u^{3/2}2u3/2

Putting it together:

25u5/2−2u3/2+C\frac{2}{5}u^{5/2} - 2u^{3/2} + C52​u5/2−2u3/2+C

Step 5: Substitute the original expression back in

Finally, replace uuu with 3−x3-x3−x:

25(3−x)5/2−2(3−x)3/2+C\frac{2}{5}(3-x)^{5/2} - 2(3-x)^{3/2} + C52​(3−x)5/2−2(3−x)3/2+C

25(3−x)5/2−2(3−x)3/2+C\frac{2}{5}(3-x)^{5/2} - 2(3-x)^{3/2} + C52​(3−x)5/2−2(3−x)3/2+C

Active Practice Problem

∫0π4xcos⁡(x2) dx\int_{0}^{\sqrt{\pi}} 4x\cos(x^{2}) \, dx∫0π​​4xcos(x2)dx

Solution Key:

We want to evaluate the following definite integral:

∫0π4xcos⁡(x2) dx\int_{0}^{\sqrt{\pi}} 4x \cos(x^2) \, dx∫0π​​4xcos(x2)dx

This problem is a classic uuu-substitution involving trigonometric functions. The inside function is x2x^2x2, and its derivative is closely related to the 4x4x4x term sitting outside the cosine function. Because it is a definite integral, we will also update our limits of integration as we switch from xxx to uuu.

Step 1: Choose uuu and find dududu

Let's choose the inside function of the cosine term to be our uuu:

u=x2u = x^2u=x2

Now, take the derivative of uuu with respect to xxx:

du=2x dxdu = 2x \, dxdu=2xdx

Step 2: Adjust for the coefficients

Our original integral contains 4x dx4x \, dx4xdx, but our derivative gives us 2x dx2x \, dx2xdx. To match the integral perfectly, we can multiply both sides of our dududu equation by 2:

2 du=4x dx2 \, du = 4x \, dx2du=4xdx

Step 3: Convert the limits of integration

Since we are switching variables from xxx to uuu, we must transform the upper and lower boundaries using our substitution equation u=x2u = x^2u=x2.

  • Lower limit (x=0x = 0x=0):
    u=(0)2=0u = (0)^2 = 0u=(0)2=0
  • Upper limit (x=πx = \sqrt{\pi}x=π​):
    u=(π)2=πu = (\sqrt{\pi})^2 = \piu=(π​)2=π
Step 4: Substitute into the integral

Now, replace all components of the original integral with our new uuu terms:

  • The limits change from 0→π0 \to \sqrt{\pi}0→π​ to 0→π0 \to \pi0→π.
  • cos⁡(x2)\cos(x^2)cos(x2) becomes cos⁡(u)\cos(u)cos(u).
  • 4x dx4x \, dx4xdx becomes 2 du2 \, du2du.

∫0πcos⁡(u)⋅2 du\int_{0}^{\pi} \cos(u) \cdot 2 \, du∫0π​cos(u)⋅2du

Pull the constant factor 2 outside the integral:

2∫0πcos⁡(u) du2 \int_{0}^{\pi} \cos(u) \, du2∫0π​cos(u)du

Step 5: Integrate and evaluate

The antiderivative of cos⁡(u)\cos(u)cos(u) is sin⁡(u)\sin(u)sin(u). Now we evaluate this from 000 to π\piπ:

2[sin⁡(u)]0π2 \Big[ \sin(u) \Big]_{0}^{\pi}2[sin(u)]0π​

Apply the Fundamental Theorem of Calculus:

2(sin⁡(π)−sin⁡(0))=2(0−0)=02 \big( \sin(\pi) - \sin(0) \big) = 2 (0 - 0) = 02(sin(π)−sin(0))=2(0−0)=0

000
(Fun fact: The answer is exactly zero because the positive area under the curve cancels out the negative area under the curve!)

Show your steps and calculations here.

Regroup 3

  • Verify calculations and mathematical reasoning.

Synthesis Wrap-up

  • Core takeaways from Session 04 and overview of homework homework assignment.