Single-Variable-Calculus Β· Unit 12 Β· Video 2 Β· Interactive Practice

Antiderivatives Differ Only by a Constant

IKey Formulas

FormulaNameMeaning
∫g(x) dx=G(x)+c\displaystyle\int g(x)\,dx = G(x) + cIndefinite integral (antiderivative)Gβ€²(x)=g(x)G'(x) = g(x), or dG=g(x) dxdG = g(x)\,dx
∫xa dx=xa+1a+1+c\displaystyle\int x^a\,dx = \frac{x^{a+1}}{a+1} + c, aβ‰ βˆ’1a \neq -1Power rule read backwardsFrom d(xa+1)=(a+1)xa dxd(x^{a+1}) = (a+1)x^a\,dx, divided by a+1a+1
∫dxx=ln⁑∣x∣+c\displaystyle\int \frac{dx}{x} = \ln|x| + cThe exception a=βˆ’1a = -1Holds for x>0x > 0 and for x<0x < 0, where ln⁑∣x∣=ln⁑(βˆ’x)\ln|x| = \ln(-x)
Fβ€²=Gβ€²F' = G' on an interval β‡’F=G+c\Rightarrow F = G + cUniqueness up to a constant(Fβˆ’G)β€²=0(F - G)' = 0, so Fβˆ’GF - G is constant by the Mean Value Theorem

Key Insight: Adding a constant never changes a derivative, since (c)β€²=0(c)' = 0. The Mean Value Theorem shows this is the only ambiguity: on an interval, the rate of change determines the function up to its starting value.

IIVisualization 1 β€” The Family βˆ’cos⁑x+c-\cos x + c

Every curve y=βˆ’cos⁑x+cy = -\cos x + c has slope sin⁑x\sin x at each xx; only the vertical shift cc differs.

πŸ’‘ Challenge: find the one antiderivative of sin⁑x\sin x whose graph passes through (0,1)(0, 1). Its starting value fixes cc.

IIIVisualization 2 β€” Reading the Table Backwards

For each pair, the slope of GG at xx equals the height of gg at xx: that is what ∫g dx=G+c\int g\,dx = G + c says.

IVVisualization 3 β€” One Constant per Interval

Both branches of ln⁑∣x∣+c\ln|x| + c have derivative 1/x1/x, but x=0x = 0 splits the domain into two intervals.

The theorem's proof compares points a<ba < b inside one interval: f(b)=f(a)+fβ€²(c)(bβˆ’a)f(b) = f(a) + f'(c)(b - a) with f=Fβˆ’Gf = F - G and f′≑0f' \equiv 0. No such comparison crosses x=0x = 0, so c1c_1 and c2c_2 are independent.

VQuiz Questions

Problem 1 Β· A Negative Power

Find ∫xβˆ’3 dx\displaystyle\int x^{-3}\,dx.

βœ… Correct! With a=βˆ’3a = -3: xβˆ’2βˆ’2+c\dfrac{x^{-2}}{-2} + c, and (βˆ’12xβˆ’2)β€²=xβˆ’3\big(-\tfrac{1}{2}x^{-2}\big)' = x^{-3}.
❌ That is the derivative. βˆ’3xβˆ’4-3x^{-4} is (xβˆ’3)β€²(x^{-3})'; integrating goes the other way, raising the power by one.
❌ Wrong direction for the power. The antiderivative of xax^a has power a+1=βˆ’2a + 1 = -2, not aβˆ’1=βˆ’4a - 1 = -4.
❌ Check the sign. The denominator is a+1=βˆ’2a + 1 = -2, so the coefficient is βˆ’12-\tfrac{1}{2}; differentiate 12xβˆ’2\tfrac{1}{2}x^{-2} and you get βˆ’xβˆ’3-x^{-3}.
❌ Not quite. Use ∫xa dx=xa+1a+1+c\int x^a\,dx = \dfrac{x^{a+1}}{a+1} + c with a=βˆ’3a = -3.
Show solution

Here a=βˆ’3β‰ βˆ’1a = -3 \neq -1, so the power rule applies:

∫xβˆ’3 dx=xβˆ’3+1βˆ’3+1+c=xβˆ’2βˆ’2+c=βˆ’12x2+c.\int x^{-3}\,dx = \frac{x^{-3+1}}{-3+1} + c = \frac{x^{-2}}{-2} + c = -\frac{1}{2x^{2}} + c.

Check: ddx(βˆ’12xβˆ’2)=βˆ’12β‹…(βˆ’2)xβˆ’3=xβˆ’3\dfrac{d}{dx}\Big(-\tfrac{1}{2}x^{-2}\Big) = -\tfrac{1}{2}\cdot(-2)x^{-3} = x^{-3}.

Problem 2 Β· The Negative Side of 1/x

Which function is an antiderivative of 1x\dfrac{1}{x} on the interval x<0x < 0?

βœ… Correct! For x<0x < 0, ln⁑∣x∣=ln⁑(βˆ’x)\ln|x| = \ln(-x), and the two minus signs in 1βˆ’xβ‹…(βˆ’1)\dfrac{1}{-x}\cdot(-1) cancel to give 1x\dfrac{1}{x}.
❌ Not defined there. ln⁑x\ln x only exists for x>0x > 0; on x<0x < 0 the formula needs the absolute value, ln⁑∣x∣=ln⁑(βˆ’x)\ln|x| = \ln(-x).
❌ One minus sign too many. (βˆ’ln⁑(βˆ’x))β€²=βˆ’1βˆ’xβ‹…(βˆ’1)=βˆ’1x\big(-\ln(-x)\big)' = -\dfrac{1}{-x}\cdot(-1) = -\dfrac{1}{x}. The chain rule already supplies the second minus sign.
❌ That is the derivative of 1/x1/x. (xβˆ’1)β€²=βˆ’xβˆ’2\big(x^{-1}\big)' = -x^{-2}; the question asks for a function whose derivative is 1/x1/x.
❌ Not quite. Differentiate each option on x<0x < 0 and look for 1/x1/x.
Show solution

The power rule fails at a=βˆ’1a = -1 (it would divide by a+1=0a + 1 = 0), so use ∫dxx=ln⁑∣x∣+c\int \frac{dx}{x} = \ln|x| + c. For x<0x < 0, ∣x∣=βˆ’x|x| = -x. With u=βˆ’xu = -x, dudx=βˆ’1\frac{du}{dx} = -1:

ddxln⁑(βˆ’x)=1βˆ’xβ‹…(βˆ’1)=1x.\frac{d}{dx}\ln(-x) = \frac{1}{-x}\cdot(-1) = \frac{1}{x}.

So ln⁑(βˆ’x)\ln(-x) works. By contrast (βˆ’ln⁑(βˆ’x))β€²=βˆ’1x\big(-\ln(-x)\big)' = -\tfrac{1}{x}, and ln⁑x\ln x is undefined for x<0x < 0.

Problem 3 Β· Pinning Down the Constant

Given: Fβ€²(x)=sin⁑x+x2F'(x) = \sin x + x^2 for all xx and F(0)=2F(0) = 2. Find F(x)F(x).

βœ… Correct! F(0)=βˆ’cos⁑0+0+3=βˆ’1+3=2F(0) = -\cos 0 + 0 + 3 = -1 + 3 = 2, and Fβ€²(x)=sin⁑x+x2F'(x) = \sin x + x^2.
❌ Check the starting value. βˆ’cos⁑0=βˆ’1-\cos 0 = -1, so this gives F(0)=1F(0) = 1, not 22. The constant has to make up the βˆ’1-1.
❌ Sign of the cosine. F(0)=2F(0) = 2 holds, but (cos⁑x)β€²=βˆ’sin⁑x(\cos x)' = -\sin x. The antiderivative of sin⁑x\sin x is βˆ’cos⁑x-\cos x.
❌ 2x2x is the derivative of x2x^2. F(0)=2F(0) = 2 holds, but Fβ€²(x)=sin⁑x+2F'(x) = \sin x + 2. The antiderivative of x2x^2 is 13x3\tfrac{1}{3}x^3.
❌ Not quite. Antidifferentiate term by term, then choose cc so that F(0)=2F(0) = 2.
Show solution

Step 1: every antiderivative. Reading the table backwards, term by term:

F(x)=βˆ’cos⁑x+x33+c.F(x) = -\cos x + \frac{x^3}{3} + c.

By the uniqueness theorem these are all the antiderivatives on (βˆ’βˆž,∞)(-\infty, \infty), so FF is one of them.

Step 2: the starting value.

F(0)=βˆ’cos⁑0+0+c=βˆ’1+c=2⟹c=3.F(0) = -\cos 0 + 0 + c = -1 + c = 2 \quad\Longrightarrow\quad c = 3. F(x)=βˆ’cos⁑x+13x3+3.F(x) = -\cos x + \tfrac{1}{3}x^3 + 3.

Check: Fβ€²(x)=sin⁑x+x2F'(x) = \sin x + x^2 and F(0)=βˆ’1+3=2F(0) = -1 + 3 = 2.

Problem 4 Β· Same Derivative, Two Intervals

Given: F(x)=tanβ‘βˆ’1xF(x) = \tan^{-1}x and G(x)=βˆ’tanβ‘βˆ’1 ⁣(1x)G(x) = -\tan^{-1}\!\big(\tfrac{1}{x}\big), defined for xβ‰ 0x \neq 0. Both have derivative 11+x2\dfrac{1}{1+x^2} wherever they are defined. What is F(x)βˆ’G(x)F(x) - G(x)?

βœ… Correct! Fβˆ’GF - G is constant on each interval, and the two constants differ: Ο€4+Ο€4=Ο€2\tfrac{\pi}{4} + \tfrac{\pi}{4} = \tfrac{\pi}{2} at x=1x = 1, βˆ’Ο€4βˆ’Ο€4=βˆ’Ο€2-\tfrac{\pi}{4} - \tfrac{\pi}{4} = -\tfrac{\pi}{2} at x=βˆ’1x = -1.
❌ Equal derivatives do not make equal functions. They make Fβˆ’GF - G constant on an interval. At x=1x = 1: Fβˆ’G=tanβ‘βˆ’11+tanβ‘βˆ’11=Ο€2β‰ 0F - G = \tan^{-1}1 + \tan^{-1}1 = \tfrac{\pi}{2} \neq 0.
❌ Right for x>0x > 0 only. The domain xβ‰ 0x \neq 0 is two intervals, so the constant may change across 00. Evaluate at x=βˆ’1x = -1.
❌ The theorem applies on each interval. (Fβˆ’G)β€²=0(F - G)' = 0 on x>0x > 0 and on x<0x < 0, so Fβˆ’GF - G is constant on each one.
❌ Not quite. Evaluate Fβˆ’GF - G at one point in each interval.
Show solution

Step 1: equal derivatives. By the chain rule,

Gβ€²(x)=βˆ’11+1/x2β‹…(βˆ’1x2)=1x2+1=Fβ€²(x).G'(x) = -\frac{1}{1 + 1/x^2}\cdot\Big(-\frac{1}{x^2}\Big) = \frac{1}{x^2 + 1} = F'(x).

Step 2: apply the theorem on each interval. (Fβˆ’G)β€²=0(F - G)' = 0 on (0,∞)(0, \infty) and on (βˆ’βˆž,0)(-\infty, 0), so Fβˆ’GF - G is a constant on each, possibly a different one.

Step 3: one point per interval.

x=1:tanβ‘βˆ’11+tanβ‘βˆ’11=Ο€4+Ο€4=Ο€2x = 1:\quad \tan^{-1}1 + \tan^{-1}1 = \tfrac{\pi}{4} + \tfrac{\pi}{4} = \tfrac{\pi}{2} x=βˆ’1:tanβ‘βˆ’1(βˆ’1)+tanβ‘βˆ’1(βˆ’1)=βˆ’Ο€4βˆ’Ο€4=βˆ’Ο€2x = -1:\quad \tan^{-1}(-1) + \tan^{-1}(-1) = -\tfrac{\pi}{4} - \tfrac{\pi}{4} = -\tfrac{\pi}{2}

So Fβˆ’G=Ο€2F - G = \tfrac{\pi}{2} for x>0x > 0 and βˆ’Ο€2-\tfrac{\pi}{2} for x<0x < 0. This is the same situation as ln⁑∣x∣+c\ln|x| + c: one constant per interval.

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