4.3 MCQs-Indefinite and Definite Integration
Indefinite and Definite Integration MCQs
Antiderivatives and Indefinite Integrals
1. The indefinite integral ∫f(x)dx represents:
The area under the curve f(x)
The derivative of f(x)
The family of all antiderivatives of f(x)
The slope of the tangent line to f(x)
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Answer: 3. The family of all antiderivatives of f(x)
Explanation:
If F′(x)=f(x), then F(x) is an antiderivative of f(x).
The indefinite integral ∫f(x)dx=F(x)+C, where C is the constant of integration, represents the entire family of antiderivatives.
Each member of this family differs by a constant.
2. The Power Rule for integration states that for n=−1, ∫xndx=
n+1xn+1+C
n−1xn−1+C
nxn−1+C
xn+1+C
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Answer: 1. n+1xn+1+C
Explanation:
This is the reverse of the Power Rule for differentiation: dxd(n+1xn+1)=xn.
The condition n=−1 is important because it leads to the integral ∫x−1dx=∫x1dx=ln∣x∣+C.
Example: ∫x3dx=4x4+C.
3. ∫exdx=
lnx+C
xex−1+C
ex+C
x+1ex+1+C
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Answer: 3. ex+C
Explanation:
Since the derivative of ex is ex, its antiderivative is also ex, plus the constant of integration.
This is a unique and important property of the exponential function with base e.
4. ∫x1dx=
lnx+C
ln∣x∣+C
x21+C
x−1+C
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Answer: 2. ln∣x∣+C
Explanation:
The absolute value is crucial because the domain of x1 excludes x=0, and the antiderivative lnx is only defined for x>0.
For x<0, the derivative of ln(−x) is also x1.
Therefore, the general antiderivative is ln∣x∣+C, valid for all x=0.
Basic Integration Rules and Substitution
5. The Constant Multiple Rule for integration states: ∫k⋅f(x)dx=
k+∫f(x)dx
k⋅∫f(x)dx
∫kdx⋅∫f(x)dx
f(kx)+C
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Answer: 2. k⋅∫f(x)dx
Explanation:
Constants can be factored out of the integral. Formally, ∫kf(x)dx=k∫f(x)dx, where k is any constant.
This follows directly from the linearity of the derivative: the derivative of kF(x) is kf(x).
6. The Sum Rule for integration states: ∫[f(x)+g(x)]dx=
∫f(x)dx⋅∫g(x)dx
∫f(x)dx+∫g(x)dx
f(x)+g(x)+C
21∫f(x)dx+21∫g(x)dx
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Answer: 2. ∫f(x)dx+∫g(x)dx
Explanation:
The integral of a sum is the sum of the integrals. Formally, ∫[f(x)+g(x)]dx=∫f(x)dx+∫g(x)dx.
Combined with the Constant Multiple Rule, this makes integration a linear operation.
Example: ∫(3x2+2cosx)dx=∫3x2dx+∫2cosxdx=x3+2sinx+C.
7. The Substitution Rule (u-substitution) for integration is essentially:
The Power Rule in reverse
The Chain Rule in reverse
The Product Rule in reverse
The Quotient Rule in reverse
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Answer: 2. The Chain Rule in reverse
Explanation:
If an integral is of the form ∫f(g(x))g′(x)dx, we can set u=g(x), then du=g′(x)dx.
The integral then simplifies to ∫f(u)du, which is hopefully easier to evaluate.
This method "undoes" the Chain Rule for differentiation.
Example: ∫2xcos(x2)dx. Let u=x2, du=2xdx. The integral becomes ∫cosudu=sinu+C=sin(x2)+C.
Definite Integrals and The Fundamental Theorem
8. The definite integral ∫abf(x)dx geometrically represents:
The slope of the secant line from (a,f(a)) to (b,f(b))
The average value of f(x) on [a,b]
The net signed area between the curve y=f(x), the x-axis, and the lines x=a and x=b
The derivative of f(x) at x=b
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Answer: 3. The net signed area between the curve y=f(x), the x-axis, and the lines x=a and x=b
Explanation:
Area above the x-axis is counted positively.
Area below the x-axis is counted negatively.
The result is the net signed area.
This is the primary geometric interpretation of the definite integral.
9. The First Fundamental Theorem of Calculus states that if f is continuous on [a,b] and F is an antiderivative of f (i.e., F′=f), then:
dxd∫axf(t)dt=f(x)
∫abf(x)dx=F(b)−F(a)
Both 1 and 2
∫abF(x)dx=f(b)−f(a)
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Answer: 3. Both 1 and 2
Explanation:
The First Fundamental Theorem of Calculus has two closely related parts.
Part 1: If g(x)=∫axf(t)dt, then g′(x)=f(x). This links differentiation and integration.
Part 2 (Evaluation Theorem): ∫abf(x)dx=F(b)−F(a). This provides a practical way to evaluate definite integrals using antiderivatives.
Notation: F(b)−F(a) is often written as [F(x)]ab or F(x)ab.
10. Using the Evaluation Theorem, ∫132xdx=
4
8
9
10
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Answer: 2. 8
Explanation:
Find an antiderivative: ∫2xdx=x2+C. We can use F(x)=x2.
Apply the theorem: ∫132xdx=F(3)−F(1)=(3)2−(1)2=9−1=8.
Geometrically, this is the area of a trapezoid: base from 1 to 3, with heights 2 and 6. Area = average height (4) × width (2) = 8.
Properties of Definite Integrals
11. The property ∫abf(x)dx=−∫baf(x)dx reflects that:
Reversing the limits of integration changes the sign of the integral.
The integral is symmetric.
The area is always positive.
The function is odd.
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Answer: 1. Reversing the limits of integration changes the sign of the integral.
Explanation:
This is a definition/convention that ensures consistency with the Evaluation Theorem.
If F is an antiderivative, then ∫abf(x)dx=F(b)−F(a).
Conversely, ∫baf(x)dx=F(a)−F(b)=−(F(b)−F(a))=−∫abf(x)dx.
12. The Additivity property for definite integrals states that for a<c<b:
∫abf(x)dx=∫acf(x)dx+∫cbf(x)dx
∫abf(x)dx=∫acf(x)dx⋅∫cbf(x)dx
∫abf(x)dx=∫ab[f(x)+g(x)]dx
∫abf(x)dx=∫cdf(x)dx
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Answer: 1. ∫abf(x)dx=∫acf(x)dx+∫cbf(x)dx
Explanation:
This property is intuitive from the area interpretation: The total area from a to b is the sum of the area from a to c and the area from c to b.
This property is very useful for splitting integrals, especially when a function is defined piecewise or has different behaviors on different intervals.
Integration by Parts
13. The formula for Integration by Parts is derived from:
The Chain Rule
The Product Rule
The Quotient Rule
The Power Rule
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Answer: 2. The Product Rule
Explanation:
Starting from the Product Rule: dxd[u(x)v(x)]=u′(x)v(x)+u(x)v′(x).
Integrate both sides: u(x)v(x)=∫u′(x)v(x)dx+∫u(x)v′(x)dx.
Rearrange: ∫u(x)v′(x)dx=u(x)v(x)−∫u′(x)v(x)dx.
In differential form (letting dv=v′(x)dx and du=u′(x)dx): ∫udv=uv−∫vdu.
14. Integration by Parts is most useful for integrals of the form:
∫sin(x2)dx
∫xexdx
∫ex2dx
∫xlnxdx
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Answer: 2. ∫xexdx
Explanation:
Integration by Parts is effective for integrals that are products of different types of functions, such as polynomial × exponential (xnex), polynomial × trigonometric (xnsinx), or logarithmic × polynomial (lnx⋅xn).
For ∫xexdx, a good choice is: u=x (so du=dx) and dv=exdx (so v=ex).
Then ∫xexdx=xex−∫exdx=xex−ex+C=ex(x−1)+C.
Options 1 and 3 do not have elementary antiderivatives. Option 4 is better solved by simple substitution (let u=lnx).
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