Concise statement of the rules and geometric remarks as given above.
Right-end rule: choose sample points ξ_i = x_i (right endpoints); then ∫_a^b f(x) dx = lim_{n→∞} Σ_{i=1}^n f(x_i)Δx_i when limit exists. Mid-point rule: choose ξ_i = (x_{i-1}+x_i)/2; then ∫_a^b f(x) dx = lim_{n→∞} Σ f(midpoint)Δx_i. Remarks: (1) F(x)=∫_a^x f(u) du defines an antiderivative. (2) If f≥0 on [a,b], the integral equals the geometric area under the curve. (3) If f≤0 the integral equals negative of the geometric area. (4) If f changes sign, split [a,b] into subintervals where f has constant sign and add/subtract areas accordingly.
Repeated integration by parts produces the series u v − u' v_1 + u'' v_2 − … until derivatives vanish; this is called Bernoulli's formula for products.
Bernoulli's formula: ∫ u dv = uv − ∫ v du; applying repeatedly gives ∫ u dv = uv − u'v_1 + u''v_2 − ... alternating signs, where v_k are successive antiderivatives of v.
Δx =1. Left endpoints: 1,2,3,4. Left Riemann sum = (1+2+3+4)·1 = 10.
10
Δx =1. Right endpoints: 2,3,4,5. Right Riemann sum = (2+3+4+5)·1 = 14.
14
Δx =1. Midpoints: 1.5,2.5,3.5,4.5. Sum = (1.5+2.5+3.5+4.5)·1 = 12, which equals the exact value ∫_1^5 x dx = (25−1)/2 =12.
12
(i) ∫_4^5 (x+5) dx = [x^2/2 +5x]_4^5 = (25/2+25)−(16/2+20) = 19/2. (ii) ∫_1^4 (2−x) dx = [2x − x^2/2]_1^4 = (8−8)−(2−1/2) = −3/2.
(i) 19/2 (ii) −3/2
(i) $\int_{3}^{4}$ $\frac{dx}{x^2-4}$v
(ii) $\int_{-1}^{1}$ $\frac{dx}{x^2+2x+5}$
(iii) $\int_{0}^{1}$ $\frac{\sqrt{1-x}}{\sqrt{1+x}}$ dx
(iv) $\int_{0}^{\pi / 2}$ ($\frac{1+sin}{1+cosx}$)dx
(v) $\int_{0}^{\pi / 2}$ $\sqrt{cos θ}$ sin³θ dθ
(vi) $\int_{0}^{1}$ $\frac{1-x^2}{(1+x^2)^2}$ dx
(iv) $\int_{0}^{\pi / 2}$ ($\frac{1+sin}{1+cosx}$)dx (v) $\int_{0}^{\pi / 2}$ $\sqrt{cos θ}$ sin³θ dθ (vi) $\int_{0}^{1}$ $\frac{1-x^2}{(1+x^2)^2}$ dx
(i) $\int_{-5}^{5}$ x cos ($\frac{e^x-1}{e^x+1}$) dxv
(ii) $\int_{-\pi / 2}^{\pi / 2}$ (x 5 + x cos x + tan³ x) dx
$\int_{-\pi / 2}^{\pi / 2}$ (x 5 + x cos x + tan³ x) dx
= $\int_{-\pi / 2}^{\pi / 2}$ (x 5 + x cos x + tan³ x) dx + $\int_{-\pi / 2}^{\pi / 2}$
Let f(x) = x 5 + x cos x + tan³x
f(-x) = -x 5 – x cos x – tan³x
f(x) = -f(-x)
f(x) is an odd function
(iii) $\int_{-\pi / 4}^{\pi / 4}$ sin² x dx
I = $\int_{-\pi / 4}^{\pi / 4}$ sin² x dx
f(x) = sin²x
f(-x) = sin²(-x) = sin²x
f(x) = f(-x)
f(x) is an even function
(iv) $\int_{0}^{2π}$ x log($\frac{3+cos x}{3-cos x}$)dx
(v) $\int_{0}^{π}$ sin 4 x cos³ x dx
$\int_{0}^{π}$ sin 4 x cos³ x dx
f(x) = sin 4 x cos³x
f(2π – x) = sin 4 (2π – x) cos³ (2π – x)
= sin 4 x cos³x
f(2π – x) = f(x)
Limit from 0 to π tends to 0 to 0
∴ Integral value = 0
∴ $\int_{0}^{π}$ sin 4 x cos³ x dx = 0
(vi) $\int_{0}^{1}$ |5x – 3|dx
(vii) $\int_{0}^{sin^2x}$ sin -1 √t dt + $\int_{0}^{cos^2x}$ cos -1 √t dt
I 1 = $\int_{0}^{sin^2x}$ sin -1 √t dt
Put sin -1 √t = θ
√t = sin θ
$\frac{1}{2√t}$ dt = cos θ dθ
dt = 2√t cos θ dθ
= 2 sin θ cos θ dθ
dt = sin 2θ dθ
I 1 = $\int_{0}^{cos^2x}$ cos -1 √t dt
Put cos -1 √t = θ
√t = cos θ
$\frac{1}{2√t}$ dt = -sin θ dθ
dt = -2√t sin θ dθ
= -2 cos θ sin θ dθ
dt = -sin 2θ dθ
(viii) $\int_{0}^{1}$ $\frac{log(1+x)}{1+x^2}$ dx
(ix) $\int_{0}^{π}$ $\frac{x sin x}{1+sin x}$ dx
(x) $\int_{π/8}^{3π/8}$ $\frac{1}{1+\sqrt{tan x}}$ dx
(xi) $\int_{0}^{π}$ x[sin²(sin x) + cos² (cos x)] dx
Let I = $\int_{0}^{π}$ x[sin²(sin x) + cos² (cos x)] dx
f(x) = sin² (sin x) + cos² (cos x)
f(π – x) = sin² (sin π – x)) + cos² (cos(π – x))
= sin² (sin x) + cos² (cos x)
f(x) = f(π – x)
f(π – x) = sin² (sin π – x)) + cos² (cos(π – x)) = sin² (sin x) + cos² (cos x) f(x) = f(π – x)
$\int_{0}^{1}$ x³e -2x dxv
Bernoulli’s formula,
∫uv dx = uv 1 – u 1 v 2 + u 2 v 3 – u 3 v 4 + ….
Bernoulli’s formula, ∫uv dx = uv 1 – u 1 v 2 + u 2 v 3 – u 3 v 4 + ….
Let I=∫_0^π x^2 cos2x dx. Integrate by parts: u=x^2, dv=cos2x dx ⇒ v=½ sin2x. So I = [½ x^2 sin2x]_0^π − ∫_0^π x sin2x dx. The boundary term is 0. For J=∫_0^π x sin2x dx use parts: u=x, dv=sin2x dx ⇒ v=−½ cos2x, so J = [−½ x cos2x]_0^π + ½ ∫_0^π cos2x dx = −(π/2)·1 + 0 = −π/2. Hence I = −J = π/2.
π/2
(i) $\int_{0}^{π/2}$ $\frac{dx}{1+5cos^2x}$v
(ii) $\int_{0}^{π/2}$ $\frac{dx}{5+4sin^2x}$
(ii) $\int_{0}^{π/2}$ $\frac{dx}{5+4sin^2x}$
(i) $\int_{0}^{π/2}$ sin 10 x dxv
Here n = 10, which is even
(ii) $\int_{0}^{π/2}$ cos 7 x dx
Here n = 7, which is odd
(iii) $\int_{0}^{π/4}$ sin 6 2x dx
put t = 2x
dt = 2 dx
(iv) $\int_{0}^{π/6}$ sin 5 3x dx
put t = 3x
dt = 3 dx
(v) $\int_{0}^{π/2}$ sin 2 x cos 4 x dx
Here m = 2, which is even and n = 4, which is even
(vi) $\int_{0}^{2π}$ sin 7 $\frac{x}{4}$ dx
(vii) $\int_{0}^{π/2}$ sin 3 θ cos 5 θ dθ
Aliter Method
(viii) $\int_{1}^{0}$ x² (1 – x)³ dx
By applying reduction formula
Aliter Method (viii) $\int_{1}^{0}$ x² (1 – x)³ dx By applying reduction formula
(i) $\int_{0}^{∞}$ x 5 e -3x dxv
(ii) $\int_{0}^{π/2}$ $\frac{e^{-tanx}}{cos^6 x}$ dx
(ii) $\int_{0}^{π/2}$ $\frac{e^{-tanx}}{cos^6 x}$ dx
See the worked solution above.
3x – 2y + 6 = 0
2y = 3x + 6
y = $\frac { 1 }{ 2 }$(3x + 6)
3x – 2y + 6 = 0 2y = 3x + 6 y = $\frac { 1 }{ 2 }$(3x + 6)
Given straight line is 2x – y + 1 = 0
y = 2x + 1, x = $\frac { y-1 }{ 2 }$
= 1 + 1
= 2 sq. units
Area required = 2 sq. units
= 1 + 1 = 2 sq. units Area required = 2 sq. units
Given curve is y = (x – 2)² + 1
(i.e) (y – 1) = (x – 2)²
Vertex of the parabola is (2, 1)
Minimum point P is (2, 1)
Slope of PQ is 2.
Equation of PQ is y – 1 = 2 (x – 2)
y – 1 = 2x – 4
y = 2x – 3
Intersecting point of y = 2x – 3 and y = (x – 2)² + 1
2x – 3 = (x – 2)² + 1
2x – 4 = (x – 2)²
2(x – 2) = (x – 2)²
x – 2 = 2
x = 4
when x = 4, y = 5
Required Area = $\frac { 4 }{ 3 }$ sq. units
x = 4 when x = 4, y = 5 Required Area = $\frac { 4 }{ 3 }$ sq. units
Given curve is
2 + x – x² + y = 0
y = x² – x – 2
y = (x – 2)(x + 1)
2 + x – x² + y = 0 y = x² – x – 2 y = (x – 2)(x + 1)
The curves meet where $x^2-2x=2x+5$, i.e. $x^2-4x-5=0\Rightarrow(x-5)(x+1)=0$, so $x=-1$ and $x=5$. On $[-1,5]$ the line lies above the parabola, so the area is $\displaystyle\int_{-1}^{5}\big[(2x+5)-(x^2-2x)\big]dx=\int_{-1}^{5}(-x^2+4x+5)\,dx=\left[-\dfrac{x^3}{3}+2x^2+5x\right]_{-1}^{5}=\dfrac{100}{3}-\left(-\dfrac{8}{3}\right)=36.$
Area $=36$ square units.
Solve sin x = cos x ⇒ x = π/4 in [0,π]. Area = ∫_0^{π/4} (cos x − sin x) dx + ∫_{π/4}^{π} (sin x − cos x) dx = [sin x + cos x]_0^{π/4} + [−cos x − sin x]_{π/4}^{π} = (√2−1)+(1+√2)=2√2.
2√2
For 0 ≤ x ≤ π/4, the region above y=0 and below y=tan x contributes A1 = ∫_0^{π/4} tan x dx = [-ln|cos x|]_0^{π/4} = ln √2 = (1/2)ln2. For π/4 ≤ x ≤ π/2 the region below y=cot x contributes A2 = ∫_{π/4}^{π/2} cot x dx = [ln|sin x|]_{π/4}^{π/2} = ln √2 = (1/2)ln2. Total area = A1 + A2 = ln2.
ln 2
Solve x^2 = −x + 2 ⇒ x^2 + x −2 = 0 ⇒ x = −2, 1. Area = ∫_{−2}^{1} [ (−x+2) − x^2 ] dx = [−x^2/2 + 2x − x^3/3]_{−2}^{1} = 9/2.
9/2
Total area = 16. The region between the two parabolas is A = ∫_0^4 [2√x − x^2/4] dx = 32/3 − 16/3 = 16/3. By symmetry the two remaining regions are equal, so each of the three parts has area 16/3.
Yes. Each area = 16/3
Given curve is y = (x – 2)² + 1
(i.e) (y – 1) = (x – 2)²
Vertex of the parabola is (2, 1)
Minimum point P is (2, 1)
Slope of PQ is 2.
Equation of PQ is y – 1 = 2 (x – 2)
y – 1 = 2x – 4
y = 2x – 3
Intersecting point of y = 2x – 3 and y = (x – 2)² + 1
2x – 3 = (x – 2)² + 1
2x – 4 = (x – 2)²
2(x – 2) = (x – 2)²
x – 2 = 2
x = 4
when x = 4, y = 5
Required Area = $\frac { 4 }{ 3 }$ sq. units
x = 4 when x = 4, y = 5 Required Area = $\frac { 4 }{ 3 }$ sq. units
Intersections: substitute x = y^2/6 into circle ⇒ (y^2/6)^2 + y^2 = 16 ⇒ y^2 = 12 ⇒ y = ±2√3, x = 2. For 0 ≤ x ≤ 2 the points common satisfy |y| ≤ √(6x), while the circle gives larger |y|, so common area = ∫_0^2 2√(6x) dx = 2√6 * (2/3) x^{3/2}|_0^2 = (16√3)/3.
16√3 / 3
Volume = π ∫_0^1 (x^2)^2 dx = π ∫_0^1 x^4 dx = π [x^5/5]_0^1 = π/5.
π/5
Revolve about x-axis: V = π ∫_0^1 (e^x − 2)^2 dx = π ∫_0^1 (e^{2x} − 4e^x + 4) dx = π[ (1/2)e^{2x} − 4e^x + 4x ]_0^1 = π( (e^2/2 − 4e + 4) − (1/2 − 4) ) = π/2 (e^2 − 8e + 15 ).
V = (π/2)(e^2 − 8e + 15)
Assume the region is 0 ≤ y ≤ 3, 0 ≤ x ≤ 1 + y^2. Revolving about the y-axis: V = π ∫_0^3 (1 + y^2)^2 dy = π ∫_0^3 (1 + 2y^2 + y^4) dy = π[ y + (2/3)y^3 + (1/5)y^5 ]_0^3 = π(3 + 18 + 243/5) = 348π/5.
348π / 5
Between x=0 and x=1 the upper curve is y=x and lower y=x^2. Revolve about x-axis: V = π ∫_0^1 (x^2 − x^4) dx = π[ x^3/3 − x^5/5 ]_0^1 = π(1/3 − 1/5) = 2π/15.
2π/15
Semi-axes: a = 10 (major/2), b = 5 (minor/2). Volume of revolution (ellipsoid) = (4/3)π a b^2 = (4/3)π ·10·5^2 = 1000π/3 cm^3.
1000π / 3 cm^3
(A) $\frac { π }{ 6 }$ (B) $\frac { π }{ 2 }$ (C) $\frac { π }{ 4 }$ (D) πv
(a) $\frac { π }{ 6 }$
Hint:
$\frac { π }{ 6 }$
(A) $\frac { 1 }{ 2 }$ (B) $\frac { 3 }{ 2 }$ (C) $\frac { 5 }{ 2 }$ (D) $\frac { 7 }{ 2 }$v
(c) $\frac { 5 }{ 2 }$
Hint:
|x| = x if x > 0
= -x if x < 0
$\frac { 5 }{ 2 }$
(A) $\frac { π }{ 2 }$ (B) π (C) 0 (D) 2v
(c) 0
Hint:
0
(A) $\frac { 3 }{ 2 }$ (B) $\frac { 1 }{ 2 }$ (C) 0 (D) $\frac { 2 }{ 3 }$v
(d) $\frac { 2 }{ 3 }$
Hint:
f(x) = sin²x cos x
f(-x) = sin²(-x) cos(-x) = sin²x cos x
f(x) = f(-x)
f is an even function
$\frac { 2 }{ 3 }$
(A) $pi$ (B) $2pi$ (C) $3pi$ (D) $4pi$v
(d) $4pi$
Hint:
For $x
e0$, $rac { x^2 }{ x^4+1 }>0$, so using $ an^{-1}u+ an^{-1}rac { 1 }{ u }=rac { pi }{ 2 }$ with $u=rac { x^2 }{ x^4+1 }$, the integrand $=rac { pi }{ 2 }$.
$int_{-4}^{4}rac { pi }{ 2 }$ dx $=rac { pi }{ 2 } imes8=4pi$
$4pi$
(A) 4 (B) 3 (C) 2 (D) 0v
(c) 2
Hint:
Odd function – 3 Odd function + 7 Odd function – Odd function + even function
= 0 + 2 $\int_{0}^{π/4}$ sec² x dx
= 2 [tan x]$_{0}^{π/4}$
= 2(1 – 0)
= 2
2
(A) cos x – x sin x (B) sin x + x cos x (C) x cos x (D) x sin xv
(c) x cos x
Hint:
f(x) = $\int_{0}^{x}$ cos t dt
u = t, dv = cos t dt
u’ = 1, v = sin t
v 1 = -cos t
f(x) = [t sin t + cos t]$_{0}^{x}$
f(x) = x sin x + cos x – 1
$\frac { df }{ dx }$ = x cos + sin x – sin x
$\frac { df }{ dx }$ = x cos x
x cos x
(A) $\frac { 2 }{ 3 }$ (B) $\frac { 4 }{ 3 }$ (C) $\frac { 8 }{ 3 }$ (D) $\frac { 5 }{ 3 }$v
(c) $\frac { 8 }{ 3 }$
Hint:
y² = 4x
y = 2√x
$\frac { 8 }{ 3 }$
(A) $\frac { 1 }{ 11000 }$ (B) $\frac { 1 }{ 10100}$ (C) $\frac { 1 }{ 10010 }$ (D) $\frac { 1 }{ 10001 }$v
(b) $\frac { 1 }{ 10100}$
Hint:
$\frac { 1 }{ 10100}$
(A) $\frac { 1 }{ 11000 }$ (B) $\frac { 1 }{ 10100}$ (C) $\frac { 1 }{ 10010 }$ (D) $\frac { 1 }{ 10001 }$v
(b) $\frac { 1 }{ 10100}$
Hint:
$\frac { 1 }{ 10100}$
(A) 10 (B) 5 (C) 8 (D) 9v
(d) 9
Hint:
n² + n = 90
n² + n – 90 = 0
(n + 10) (n – 9) = 0
n = 9
9
(A) $\frac { 2 }{ 3 }$ (B) $\frac { 2 }{ 9}$ (C) $\frac { 1 }{ 9 }$ (D) $\frac { 1 }{ 3 }$v
(b) $\frac { 1 }{ 10100}$
Hint:
$\int_{0}^{π/6}$ cos³ 3xdx = $\frac { 1 }{ 3 }$ × $\frac { 2 }{ 3 }$ × 1
= $\frac { 2 }{ 9 }$
$\frac { 2 }{ 9}$
(A) $\frac { 2 }{ 3 }$ (B) $\frac { 2 }{ 9}$ (C) $\frac { 1 }{ 9 }$ (D) $\frac { 1 }{ 3 }$v
(b) $\frac { 1 }{ 10100}$
Hint:
$\int_{0}^{π/6}$ cos³ 3xdx = $\frac { 1 }{ 3 }$ × $\frac { 2 }{ 3 }$ × 1
= $\frac { 2 }{ 9 }$
$\frac { 2 }{ 9}$
(A) $\frac { 3π }{ 10 }$ (B) $\frac { 3π }{ 8}$ (C) $\frac { 3π }{ 4 }$ (D) $\frac { 3π }{ 2 }$v
(b) $\frac { 3π }{ 8}$
Hint:
(x) = sin 4 x dx
f(π – x) = sin 4 (π – x) = sin 4 x
$\frac { 3π }{ 8}$
(A) $\frac { 7 }{ 27 }$ (B) $\frac { 5 }{ 27 }$ (C) $\frac { 4 }{ 27 }$ (D) $\frac { 2 }{ 27 }$v
(d) $\frac { 2 }{ 27 }$
Hint:
$\frac { 2 }{ 27 }$
(A) πa³ (B) $\frac { πa^3 }{ 4 }$ (C) $\frac { πa^3 }{ 5 }$ (D) $\frac { πa^3 }{ 6 }$v
(d) $\frac { πa^3 }{ 6 }$
Hint:
y² = x(a – x)
To find limit put y = 0
x (a – x) = 0
x = 0, x = a
$\frac { πa^3 }{ 6 }$
(A) 3 (B) 6 (C) 9 (D) 5v
(c) 9
Hint:
9
(A) $\frac { π^2 }{ 4 }$ – 1 (B) $\frac { π^2 }{ 4 }$ + 2 (C) $\frac { π^2 }{ 4 }$ + 1 (D) $\frac { π^2 }{ 4 }$ – 2v
(d) $\frac { π^2 }{ 4 }$ – 2
Hint:
$\frac { π^2 }{ 4 }$ – 2
(A) $\frac { π^2 }{ 4 }$ – 1 (B) $\frac { π^2 }{ 4 }$ + 2 (C) $\frac { π^2 }{ 4 }$ + 1 (D) $\frac { π^2 }{ 4 }$ – 2v
(d) $\frac { π^2 }{ 4 }$ – 2
Hint:
$\frac { π^2 }{ 4 }$ – 2
(A) $\frac { 1 }{ 2 }$ (B) 2 (C) 1 (D) $\frac { 3 }{ 4 }$v
(a) $\frac { 1 }{ 2 }$
Hint:
= 1 + 0 – x f(x)
f(x) + x f(x) = 1
f(x)[1 + x] = 1
when x = 1,
f(1)(2) = 1
f(1) = $\frac { 1 }{ 2 }$
$\frac { 1 }{ 2 }$