Fundamentals of Calculus
By Notes Vandar
2.1 Limits and continuity of a function
Limits of a Function
A limit describes the behavior of a function as its input approaches a particular value. It allows us to understand what value a function is approaching, even if it does not actually reach that value.
Formal Definition of a Limit:
limx→cf(x)=L\lim_{{x \to c}} f(x) = L
This means that as xx approaches cc, the function f(x)f(x) approaches the value LL. The limit exists if and only if f(x)f(x) approaches the same value LL from both the left-hand side and right-hand side of cc.
- Left-hand limit: limx→c−f(x)=L\lim_{{x \to c^-}} f(x) = L
- Right-hand limit: limx→c+f(x)=L\lim_{{x \to c^+}} f(x) = L
If limx→c−f(x)=limx→c+f(x)=L\lim_{{x \to c^-}} f(x) = \lim_{{x \to c^+}} f(x) = L, the limit exists and equals LL.
Example: Consider f(x)=x2−1x−1f(x) = \frac{x^2 – 1}{x – 1}. At x=1x = 1, the function is undefined (division by zero), but we can compute the limit as xx approaches 1:
limx→1×2−1x−1=limx→1(x−1)(x+1)x−1=limx→1(x+1)=2\lim_{{x \to 1}} \frac{x^2 – 1}{x – 1} = \lim_{{x \to 1}} \frac{(x – 1)(x + 1)}{x – 1} = \lim_{{x \to 1}} (x + 1) = 2
Even though f(x)f(x) is not defined at x=1x = 1, the limit exists and equals 2.
Continuity of a Function
A function is continuous at a point x=cx = c if the following three conditions are satisfied:
- The function is defined at cc: f(c)f(c) exists.
- The limit exists at cc: limx→cf(x)\lim_{{x \to c}} f(x) exists.
- The limit equals the function value: limx→cf(x)=f(c)\lim_{{x \to c}} f(x) = f(c).
If a function is continuous at every point in its domain, it is said to be continuous on its domain.
Example: Consider f(x)=x2f(x) = x^2.
- The function is defined for all xx.
- The limit as xx approaches any value cc is: limx→cx2=c2\lim_{{x \to c}} x^2 = c^2
- The function value is f(c)=c2f(c) = c^2.
Since limx→cx2=c2=f(c)\lim_{{x \to c}} x^2 = c^2 = f(c), the function is continuous for all real values of xx.
Types of Discontinuities
- Removable Discontinuity: Occurs when the limit exists, but the function is either undefined at that point or the function’s value does not match the limit. It can often be “fixed” by redefining the function at that point.
- Jump Discontinuity: Occurs when the left-hand and right-hand limits exist but are not equal.
- Infinite Discontinuity: Occurs when the function approaches infinity as xx approaches a particular point.
2.1.1 ε − δ definition of limit and continuity.
Definition of Limit and Continuity
The ε−δ\varepsilon – \delta (epsilon-delta) definition is a formal and rigorous way to define the limit of a function. This method gives a precise description of what it means for a function to approach a particular value as its input gets close to some point.
ε−δ\varepsilon – \delta Definition of a Limit
Let f(x)f(x) be a function, and let LL be a real number. We say that the limit of f(x)f(x) as xx approaches cc is LL, written as:
limx→cf(x)=L\lim_{x \to c} f(x) = L
If for every ε>0\varepsilon > 0 (no matter how small), there exists a δ>0\delta > 0 such that whenever 0<∣x−c∣<δ0 < |x – c| < \delta, it follows that ∣f(x)−L∣<ε|f(x) – L| < \varepsilon.
- ε\varepsilon represents how close we want f(x)f(x) to be to LL.
- δ\delta represents how close xx needs to be to cc to ensure f(x)f(x) is within ε\varepsilon of LL.
In simpler terms:
- For every small tolerance ε\varepsilon, we can find a small distance δ\delta such that when xx is within δ\delta units of cc (but not equal to cc), the value of f(x)f(x) is within ε\varepsilon units of LL.
Formal Statement:
∀ε>0, ∃δ>0 such that if 0<∣x−c∣<δ, then ∣f(x)−L∣<ε.\forall \varepsilon > 0, \, \exists \delta > 0 \text{ such that if } 0 < |x – c| < \delta, \text{ then } |f(x) – L| < \varepsilon.
Example:
Let’s prove that:
limx→2(3x+1)=7\lim_{x \to 2} (3x + 1) = 7
We need to show that for any ε>0\varepsilon > 0, there exists a δ>0\delta > 0 such that if 0<∣x−2∣<δ0 < |x – 2| < \delta, then ∣(3x+1)−7∣<ε|(3x + 1) – 7| < \varepsilon.
- Start with ∣(3x+1)−7∣|(3x + 1) – 7|:
∣(3x+1)−7∣=∣3x−6∣=3∣x−2∣|(3x + 1) – 7| = |3x – 6| = 3|x – 2|
- We want 3∣x−2∣<ε3|x – 2| < \varepsilon, so divide both sides by 3:
∣x−2∣<ε3|x – 2| < \frac{\varepsilon}{3}
Thus, we can choose δ=ε3\delta = \frac{\varepsilon}{3}. Therefore, for any ε>0\varepsilon > 0, if ∣x−2∣<δ=ε3|x – 2| < \delta = \frac{\varepsilon}{3}, it follows that ∣(3x+1)−7∣<ε|(3x + 1) – 7| < \varepsilon. This proves that limx→2(3x+1)=7\lim_{x \to 2} (3x + 1) = 7.
ε−δ\varepsilon – \delta Definition of Continuity
A function f(x)f(x) is continuous at a point x=cx = c if the following three conditions are satisfied:
- f(c)f(c) is defined (i.e., the function has a value at cc).
- limx→cf(x)\lim_{x \to c} f(x) exists.
- The limit equals the function value, limx→cf(x)=f(c)\lim_{x \to c} f(x) = f(c).
Using the ε−δ\varepsilon – \delta definition, the function f(x)f(x) is continuous at cc if for every ε>0\varepsilon > 0, there exists a δ>0\delta > 0 such that:
∀ε>0, ∃δ>0 such that if ∣x−c∣<δ, then ∣f(x)−f(c)∣<ε.\forall \varepsilon > 0, \, \exists \delta > 0 \text{ such that if } |x – c| < \delta, \text{ then } |f(x) – f(c)| < \varepsilon.
This means that the values of f(x)f(x) get arbitrarily close to f(c)f(c) as xx gets arbitrarily close to cc, ensuring the function is smooth and without jumps at that point.
Example of Continuity:
Let’s check if the function f(x)=x2f(x) = x^2 is continuous at x=1x = 1.
- The value of the function at x=1x = 1 is f(1)=12=1f(1) = 1^2 = 1.
- The limit of f(x)f(x) as xx approaches 1 is: limx→1×2=1\lim_{x \to 1} x^2 = 1
Now, for any ε>0\varepsilon > 0, we want to find δ\delta such that if ∣x−1∣<δ|x – 1| < \delta, then ∣x2−1∣<ε|x^2 – 1| < \varepsilon.
∣x2−1∣=∣(x−1)(x+1)∣|x^2 – 1| = |(x – 1)(x + 1)|
We want:
∣(x−1)(x+1)∣<ε|(x – 1)(x + 1)| < \varepsilon
To control ∣x+1∣|x + 1|, note that if ∣x−1∣<1|x – 1| < 1, then 0<x<20 < x < 2, and thus ∣x+1∣<3|x + 1| < 3. So, we can require:
∣x−1∣⋅3<ε⇒∣x−1∣<ε3|x – 1| \cdot 3 < \varepsilon \quad \Rightarrow \quad |x – 1| < \frac{\varepsilon}{3}
Thus, we can choose δ=ε3\delta = \frac{\varepsilon}{3}. Therefore, f(x)=x2f(x) = x^2 is continuous at x=1x = 1.
2.1.2 Evaluate the limit of the function
It seems like you want to evaluate the limit of a function but haven’t specified which function. Here are a few common examples of how to evaluate limits:
Example 1: Polynomial Limit
Evaluate the limit:
limx→3(2×2+5)\lim_{{x \to 3}} (2x^2 + 5)
Solution: Substituting x=3x = 3:
=2(3)2+5=2⋅9+5=18+5=23= 2(3)^2 + 5 = 2 \cdot 9 + 5 = 18 + 5 = 23
So,
limx→3(2×2+5)=23\lim_{{x \to 3}} (2x^2 + 5) = 23
Example 2: Rational Function Limit
Evaluate the limit:
limx→2×2−4x−2\lim_{{x \to 2}} \frac{x^2 – 4}{x – 2}
Solution: First, substitute x=2x = 2:
=22−42−2=00 (indeterminate form)= \frac{2^2 – 4}{2 – 2} = \frac{0}{0} \text{ (indeterminate form)}
Factor the numerator:
=(x−2)(x+2)x−2= \frac{(x – 2)(x + 2)}{x – 2}
Now cancel x−2x – 2 (valid for x≠2x \neq 2):
=x+2= x + 2
Now evaluate the limit:
limx→2(x+2)=2+2=4\lim_{{x \to 2}} (x + 2) = 2 + 2 = 4
So,
limx→2×2−4x−2=4\lim_{{x \to 2}} \frac{x^2 – 4}{x – 2} = 4
Example 3: Trigonometric Limit
Evaluate the limit:
limx→0sinxx\lim_{{x \to 0}} \frac{\sin x}{x}
Solution: This is a well-known limit:
limx→0sinxx=1\lim_{{x \to 0}} \frac{\sin x}{x} = 1
2.1.3 Continuity of the function
2.1.3 Continuity of the Function
To determine the continuity of a function at a specific point, we need to check the following three conditions for the function f(x)f(x) at the point x=cx = c:
- The function is defined at cc: f(c)f(c) exists.
- The limit exists at cc: limx→cf(x)\lim_{{x \to c}} f(x) exists.
- The limit equals the function value: limx→cf(x)=f(c)\lim_{{x \to c}} f(x) = f(c).
If all these conditions are met, the function is continuous at x=cx = c. If the function is continuous at every point in its domain, it is said to be continuous on that domain.
Example: Analyzing Continuity of a Function
Let’s consider the function f(x)f(x):
f(x)={x2if x<12if x=13−xif x>1f(x) = \begin{cases} x^2 & \text{if } x < 1 \\ 2 & \text{if } x = 1 \\ 3 – x & \text{if } x > 1 \end{cases}
Step 1: Check Continuity at x=1x = 1
- Is f(1)f(1) defined?
f(1)=2(function is defined)f(1) = 2 \quad (\text{function is defined})
- Does the limit exist at x=1x = 1?
- Left-hand limit:
limx→1−f(x)=limx→1−x2=12=1\lim_{{x \to 1^-}} f(x) = \lim_{{x \to 1^-}} x^2 = 1^2 = 1
- Right-hand limit:
limx→1+f(x)=limx→1+(3−x)=3−1=2\lim_{{x \to 1^+}} f(x) = \lim_{{x \to 1^+}} (3 – x) = 3 – 1 = 2Since the left-hand limit (1) does not equal the right-hand limit (2), the overall limit does not exist at x=1x = 1:
limx→1f(x) does not exist.\lim_{{x \to 1}} f(x) \text{ does not exist.}
- Does the limit equal the function value?
- Since the limit does not exist, we cannot satisfy the third condition.
Conclusion: The function f(x)f(x) is not continuous at x=1x = 1 because the limit does not exist at that point.
Checking Continuity at Another Point
Let’s check the continuity of the same function at x=0x = 0.
- Is f(0)f(0) defined?
f(0)=02=0f(0) = 0^2 = 0
- Does the limit exist at x=0x = 0?
- Left-hand limit:
limx→0−f(x)=limx→0−x2=02=0\lim_{{x \to 0^-}} f(x) = \lim_{{x \to 0^-}} x^2 = 0^2 = 0
- Right-hand limit:
limx→0+f(x)=limx→0+x2=02=0\lim_{{x \to 0^+}} f(x) = \lim_{{x \to 0^+}} x^2 = 0^2 = 0Thus,
limx→0f(x)=0.\lim_{{x \to 0}} f(x) = 0.
- Does the limit equal the function value?
limx→0f(x)=0=f(0).\lim_{{x \to 0}} f(x) = 0 = f(0).
Conclusion: The function f(x)f(x) is continuous at x=0x = 0.
2.2 Derivatives of function
2.2.1 Definition and Geometrical Interpretation of Derivatives
Definition of the Derivative
The derivative of a function f(x)f(x) at a point x=ax = a is defined as the limit of the average rate of change of the function over an interval as the interval approaches zero. Mathematically, the derivative f′(a)f'(a) is given by:
f′(a)=limh→0f(a+h)−f(a)hf'(a) = \lim_{{h \to 0}} \frac{f(a + h) – f(a)}{h}
- f′(a)f'(a) is the derivative of the function f(x)f(x) at the point aa.
- hh is a small increment in xx.
- The expression f(a+h)−f(a)h\frac{f(a + h) – f(a)}{h} represents the average rate of change of the function between the points aa and a+ha + h.
Interpretation of the Derivative
- Slope of the Tangent Line: The derivative at a point gives the slope of the tangent line to the graph of the function at that point. If you think of the function as a curve, the derivative tells us how steep the curve is at any given point.
- Rate of Change: The derivative represents how much the function f(x)f(x) changes as xx changes. If f(x)f(x) describes a physical quantity (like position), then the derivative f′(x)f'(x) describes the rate of change of that quantity (like velocity).
Geometrical Interpretation
To visualize the concept of the derivative, consider the following:
- Graph of the Function: Imagine a curve representing the function f(x)f(x).
- Point of Interest: Pick a point (a,f(a))(a, f(a)) on the curve.
- Secant Line: Draw a secant line connecting two points (a,f(a))(a, f(a)) and (a+h,f(a+h))(a + h, f(a + h)). The slope of this secant line is given by the average rate of change:
slope of secant=f(a+h)−f(a)h\text{slope of secant} = \frac{f(a + h) – f(a)}{h}
- Tangent Line: As hh approaches 0 (i.e., as the second point approaches the point (a,f(a))(a, f(a))), the secant line approaches the tangent line at (a,f(a))(a, f(a)). The slope of the tangent line is the derivative f′(a)f'(a).
In this image, the blue secant line represents the average rate of change between two points on the curve, while the red tangent line represents the instantaneous rate of change at point aa.
Example:
Consider the function f(x)=x2f(x) = x^2.
- Calculate the Derivative:
f′(x)=limh→0(x+h)2−x2h=limh→0x2+2xh+h2−x2h=limh→02xh+h2h=limh→0(2x+h)=2xf'(x) = \lim_{{h \to 0}} \frac{(x + h)^2 – x^2}{h} = \lim_{{h \to 0}} \frac{x^2 + 2xh + h^2 – x^2}{h} = \lim_{{h \to 0}} \frac{2xh + h^2}{h} = \lim_{{h \to 0}} (2x + h) = 2x
- Interpret the Derivative:
- At any point xx, the derivative f′(x)=2xf'(x) = 2x gives the slope of the tangent line to the curve y=x2y = x^2 at that point. For example:
- At x=1x = 1, f′(1)=2f'(1) = 2, which means the slope of the tangent line at (1,1)(1, 1) is 2.
- At x=2x = 2, f′(2)=4f'(2) = 4, which means the slope of the tangent line at (2,4)(2, 4) is 4.
- At any point xx, the derivative f′(x)=2xf'(x) = 2x gives the slope of the tangent line to the curve y=x2y = x^2 at that point. For example:
2.2.2 Derivatives of the functions (Algebraic only)
The derivative of a function describes how the function changes as its input changes. Below are the basic rules and formulas for finding the derivatives of common algebraic functions.
1. Power Rule
For any function of the form f(x)=xnf(x) = x^n, where nn is a real number, the derivative is given by:
f′(x)=nxn−1f'(x) = nx^{n-1}
Example:
f(x)=x3 ⟹ f′(x)=3x2f(x) = x^3 \implies f'(x) = 3x^{2}
2. Constant Rule
The derivative of a constant cc is zero:
f(x)=c ⟹ f′(x)=0f(x) = c \implies f'(x) = 0
Example:
f(x)=5 ⟹ f′(x)=0f(x) = 5 \implies f'(x) = 0
3. Sum Rule
If f(x)f(x) and g(x)g(x) are differentiable functions, then the derivative of their sum is:
(f+g)′(x)=f′(x)+g′(x)(f + g)'(x) = f'(x) + g'(x)
Example:
f(x)=x2+3x ⟹ f′(x)=2x+3f(x) = x^2 + 3x \implies f'(x) = 2x + 3
4. Difference Rule
If f(x)f(x) and g(x)g(x) are differentiable functions, then the derivative of their difference is:
(f−g)′(x)=f′(x)−g′(x)(f – g)'(x) = f'(x) – g'(x)
Example:
f(x)=x2−4x ⟹ f′(x)=2x−4f(x) = x^2 – 4x \implies f'(x) = 2x – 4
5. Product Rule
If u(x)u(x) and v(x)v(x) are differentiable functions, then the derivative of their product is:
(uv)′=u′v+uv′(uv)’ = u’v + uv’
Example:
f(x)=x2(3x) ⟹ u=x2, v=3xf(x) = x^2(3x) \implies u = x^2, \, v = 3x u′=2x, v′=3 ⟹ f′(x)=(2x)(3x)+(x2)(3)=6×2+3×2=9x2u’ = 2x, \, v’ = 3 \implies f'(x) = (2x)(3x) + (x^2)(3) = 6x^2 + 3x^2 = 9x^2
6. Quotient Rule
If u(x)u(x) and v(x)v(x) are differentiable functions, then the derivative of their quotient is:
(uv)′=u′v−uv′v2\left(\frac{u}{v}\right)’ = \frac{u’v – uv’}{v^2}
Example:
f(x)=x23x ⟹ u=x2, v=3xf(x) = \frac{x^2}{3x} \implies u = x^2, \, v = 3x u′=2x, v′=3 ⟹ f′(x)=(2x)(3x)−(x2)(3)(3x)2=6×2−3x29x2=3x29x2=13u’ = 2x, \, v’ = 3 \implies f'(x) = \frac{(2x)(3x) – (x^2)(3)}{(3x)^2} = \frac{6x^2 – 3x^2}{9x^2} = \frac{3x^2}{9x^2} = \frac{1}{3}
7. Chain Rule
If g(x)g(x) is a differentiable function and f(x)=g(h(x))f(x) = g(h(x)) is a composite function, then the derivative is given by:
f′(x)=g′(h(x))⋅h′(x)f'(x) = g'(h(x)) \cdot h'(x)
Example:
f(x)=(x2+1)3f(x) = (x^2 + 1)^3
Let g(u)=u3g(u) = u^3 and h(x)=x2+1h(x) = x^2 + 1:
g′(u)=3u2, h′(x)=2x ⟹ f′(x)=3(h(x))2⋅h′(x)=3(x2+1)2⋅(2x)=6x(x2+1)2g'(u) = 3u^2, \, h'(x) = 2x \implies f'(x) = 3(h(x))^2 \cdot h'(x) = 3(x^2 + 1)^2 \cdot (2x) = 6x(x^2 + 1)^2
2.2.3 Maxima and Minima of Functions
Maxima and minima refer to the highest and lowest points on a function’s graph, respectively. These points are critical for understanding the behavior of functions, especially in optimization problems.
1. Definition
- Maximum: A function f(x)f(x) has a local maximum at x=cx = c if f(c)≥f(x)f(c) \geq f(x) for all xx in some neighborhood of cc.
- Minimum: A function f(x)f(x) has a local minimum at x=cx = c if f(c)≤f(x)f(c) \leq f(x) for all xx in some neighborhood of cc.
Global Maximum/Minimum: A global maximum (or minimum) is the highest (or lowest) value of the function over its entire domain.
2. Finding Maxima and Minima
To find the local maxima and minima of a function, we typically follow these steps:
- Find the Derivative: Calculate the derivative f′(x)f'(x) of the function f(x)f(x).
- Set the Derivative to Zero: Solve f′(x)=0f'(x) = 0 to find the critical points. These points are where the function’s slope is zero and could potentially be maxima or minima.
- Test Critical Points: Use the second derivative test or the first derivative test to determine whether each critical point is a maximum, minimum, or neither.
- Second Derivative Test:
- If f′′(c)>0f”(c) > 0, then f(x)f(x) has a local minimum at x=cx = c.
- If f′′(c)<0f”(c) < 0, then f(x)f(x) has a local maximum at x=cx = c.
- If f′′(c)=0f”(c) = 0, the test is inconclusive.
- First Derivative Test:
- Analyze the sign of f′(x)f'(x) on intervals around the critical points.
- If f′(x)f'(x) changes from positive to negative at cc, cc is a local maximum.
- If f′(x)f'(x) changes from negative to positive at cc, cc is a local minimum.
- Second Derivative Test:
3. Example: Finding Maxima and Minima
Example Function: Let’s analyze the function f(x)=−x2+4xf(x) = -x^2 + 4x.
- Find the Derivative:
f′(x)=−2x+4f'(x) = -2x + 4
- Set the Derivative to Zero:
−2x+4=0 ⟹ 2x=4 ⟹ x=2-2x + 4 = 0 \implies 2x = 4 \implies x = 2
- Test Critical Points:
- Second Derivative Test: f′′(x)=−2f”(x) = -2 Since f′′(x)<0f”(x) < 0, f(x)f(x) has a local maximum at x=2x = 2.
- Find the Maximum Value:
f(2)=−(2)2+4(2)=−4+8=4f(2) = -(2)^2 + 4(2) = -4 + 8 = 4Thus, the function has a local (and global) maximum at the point (2,4)(2, 4).
2.3 Indefinite and Definite Integral
Integration is a fundamental concept in calculus that is essentially the reverse process of differentiation. It is used to calculate areas under curves, among many other applications.
1. Indefinite Integrals
An indefinite integral represents a family of functions whose derivative is the integrand. It is written in the form:
∫f(x) dx=F(x)+C\int f(x) \, dx = F(x) + C
where:
- ∫\int denotes the integral sign.
- f(x)f(x) is the integrand (the function being integrated).
- F(x)F(x) is the antiderivative of f(x)f(x) (the function whose derivative is f(x)f(x)).
- CC is the constant of integration, representing any constant value, since the derivative of a constant is zero.
Example: To find the indefinite integral of f(x)=3x2f(x) = 3x^2:
∫3×2 dx=x3+C\int 3x^2 \, dx = x^3 + C
2. Definite Integrals
A definite integral computes the accumulation of a quantity over a specified interval [a,b][a, b]. It is represented as:
∫abf(x) dx=F(b)−F(a)\int_a^b f(x) \, dx = F(b) – F(a)
where:
- F(x)F(x) is any antiderivative of f(x)f(x).
- aa and bb are the limits of integration, with a<ba < b.
- The result represents the net area under the curve of f(x)f(x) from x=ax = a to x=bx = b.
Example: To evaluate the definite integral of f(x)=3x2f(x) = 3x^2 from x=1x = 1 to x=2x = 2:
- Find the antiderivative:
F(x)=x3F(x) = x^3
- Apply the Fundamental Theorem of Calculus:
∫123×2 dx=F(2)−F(1)=23−13=8−1=7\int_1^2 3x^2 \, dx = F(2) – F(1) = 2^3 – 1^3 = 8 – 1 = 7
3. Fundamental Theorem of Calculus
This theorem connects differentiation and integration, stating that:
- If FF is an antiderivative of ff on an interval [a,b][a, b], then:
∫abf(x) dx=F(b)−F(a)\int_a^b f(x) \, dx = F(b) – F(a)
- If ff is continuous on [a,b][a, b], then the function F(x)=∫axf(t) dtF(x) = \int_a^x f(t) \, dt is continuous on [a,b][a, b] and differentiable on (a,b)(a, b), and:
F′(x)=f(x)F'(x) = f(x)
4. Techniques of Integration
Common techniques for evaluating integrals include:
- Substitution: A method used to simplify the integrand by substituting a part of the expression with a new variable.
Example:
∫(2x)ex2 dx(let u=x2, du=2x dx)\int (2x) e^{x^2} \, dx \quad \text{(let } u = x^2, \, du = 2x \, dx\text{)} =∫eu du=ex2+C= \int e^u \, du = e^{x^2} + C
- Integration by Parts: A method based on the product rule for differentiation:
∫u dv=uv−∫v du\int u \, dv = uv – \int v \, du
- Partial Fractions: Used to integrate rational functions by breaking them down into simpler fractions.
2.3.1 Meanings of Integrals
Integrals have several interpretations and meanings in mathematics and applied fields. Here are the primary meanings of integrals:
1. Area Under a Curve
The most common interpretation of the definite integral is as the area under a curve defined by a function f(x)f(x) between two points aa and bb:
∫abf(x) dx\int_a^b f(x) \, dx
- Geometric Interpretation: If f(x)f(x) is positive over the interval [a,b][a, b], the definite integral gives the exact area between the curve y=f(x)y = f(x) and the x-axis from x=ax = a to x=bx = b. If f(x)f(x) is negative, the integral represents the area below the x-axis, which is considered negative.
2. Accumulation Function
The definite integral can be viewed as an accumulation function. It quantifies the total accumulation of a quantity represented by f(x)f(x) over the interval [a,b][a, b].
- Example: If f(t)f(t) represents the rate of water flow into a tank over time, then ∫abf(t) dt\int_a^b f(t) \, dt gives the total amount of water that has flowed into the tank between times aa and bb.
3. Average Value of a Function
The integral can also be used to find the average value of a continuous function f(x)f(x) over the interval [a,b][a, b]:
Average value=1b−a∫abf(x) dx\text{Average value} = \frac{1}{b – a} \int_a^b f(x) \, dx
- This formula gives the average height of the function over the specified interval, which can be particularly useful in various applications, such as determining the average temperature over a period.
4. Solution to Differential Equations
Integrals play a crucial role in solving ordinary differential equations (ODEs). Many physical phenomena are modeled by ODEs, and integrating these equations can help find solutions.
- Example: The integral of a rate function can provide the original function describing the quantity of interest. For example, if dydt=k\frac{dy}{dt} = k, integrating both sides with respect to tt gives y(t)=kt+Cy(t) = kt + C, where CC is the constant of integration.
5. Probability and Statistics
In probability theory, integrals are used to calculate probabilities and expected values.
- Probability Density Function (PDF): For a continuous random variable with a PDF f(x)f(x), the probability that the variable falls within a certain interval [a,b][a, b] is given by the definite integral:
P(a≤X≤b)=∫abf(x) dxP(a \leq X \leq b) = \int_a^b f(x) \, dx
- Expected Value: The expected value E[X]E[X] of a continuous random variable can be computed using:
E[X]=∫−∞∞xf(x) dxE[X] = \int_{-\infty}^{\infty} x f(x) \, dx
2.3.2 Some Standard Integrals
In calculus, certain integrals frequently occur, and knowing their standard forms can greatly simplify the process of integration. Here’s a list of some common standard integrals:
1. Basic Power Functions
- Integral of a Power Function:
∫xn dx=xn+1n+1+C,n≠−1\int x^n \, dx = \frac{x^{n+1}}{n+1} + C, \quad n \neq -1
- Integral of x−1x^{-1}:
∫1x dx=ln∣x∣+C\int \frac{1}{x} \, dx = \ln |x| + C
2. Exponential Functions
- Integral of the Exponential Function:
∫eax dx=1aeax+C\int e^{ax} \, dx = \frac{1}{a} e^{ax} + C
- Integral of the Natural Exponential Function:
∫ax dx=axlna+C(a>0,a≠1)\int a^x \, dx = \frac{a^x}{\ln a} + C \quad (a > 0, a \neq 1)
3. Trigonometric Functions
- Integral of Sine and Cosine:
∫sinx dx=−cosx+C\int \sin x \, dx = -\cos x + C ∫cosx dx=sinx+C\int \cos x \, dx = \sin x + C
- Integral of Tangent:
∫tanx dx=−ln∣cosx∣+C=ln∣secx∣+C\int \tan x \, dx = -\ln |\cos x| + C = \ln |\sec x| + C
- Integral of Cosecant:
∫cscx dx=−ln∣cscx+cotx∣+C\int \csc x \, dx = -\ln |\csc x + \cot x| + C
- Integral of Secant:
∫secx dx=ln∣secx+tanx∣+C\int \sec x \, dx = \ln |\sec x + \tan x| + C
- Integral of Cotangent:
∫cotx dx=ln∣sinx∣+C\int \cot x \, dx = \ln |\sin x| + C
4. Hyperbolic Functions
- Integral of Hyperbolic Sine:
∫sinhx dx=coshx+C\int \sinh x \, dx = \cosh x + C
- Integral of Hyperbolic Cosine:
∫coshx dx=sinhx+C\int \cosh x \, dx = \sinh x + C
- Integral of Hyperbolic Tangent:
∫tanhx dx=ln∣coshx∣+C\int \tanh x \, dx = \ln |\cosh x| + C
5. Other Useful Integrals
- Integral of 1×2+a2\frac{1}{x^2 + a^2}:
∫1×2+a2 dx=1atan−1(xa)+C\int \frac{1}{x^2 + a^2} \, dx = \frac{1}{a} \tan^{-1} \left(\frac{x}{a}\right) + C
- Integral of 1a2−x2\frac{1}{\sqrt{a^2 – x^2}}:
∫1a2−x2 dx=sin−1(xa)+C\int \frac{1}{\sqrt{a^2 – x^2}} \, dx = \sin^{-1} \left(\frac{x}{a}\right) + C
- Integral of 1×2+a2\frac{1}{\sqrt{x^2 + a^2}}:
∫1×2+a2 dx=ln∣x+x2+a2∣+C\int \frac{1}{\sqrt{x^2 + a^2}} \, dx = \ln \left| x + \sqrt{x^2 + a^2} \right| + C
2.3.3 Meaning of ∫ f(x)dx
The notation ∫f(x) dx\int f(x) \, dx represents the process of integration of the function f(x)f(x) with respect to the variable xx. This expression has several interpretations and meanings, which are crucial for understanding its applications in mathematics and science. Here are the key meanings:
1. Antiderivative
The most fundamental meaning of ∫f(x) dx\int f(x) \, dx is that it represents the antiderivative or primitive of the function f(x)f(x). This means that:
∫f(x) dx=F(x)+C\int f(x) \, dx = F(x) + C
where:
- F(x)F(x) is a function such that F′(x)=f(x)F'(x) = f(x).
- CC is the constant of integration, accounting for the fact that there are infinitely many antiderivatives (differing by a constant).
Example: If f(x)=2xf(x) = 2x, then:
∫2x dx=x2+C\int 2x \, dx = x^2 + C
2. Area Under the Curve
For a definite integral (with limits), the expression can represent the area under the curve of f(x)f(x) from x=ax = a to x=bx = b:
∫abf(x) dx\int_a^b f(x) \, dx
This quantity is the net area between the graph of f(x)f(x) and the x-axis over the interval [a,b][a, b]. If f(x)f(x) is above the x-axis, the area is positive; if it is below, the area is negative.
3. Accumulation Function
The integral can also be viewed as an accumulation function. In this context, if f(x)f(x) represents a rate of change (e.g., velocity), then ∫f(x) dx\int f(x) \, dx represents the total accumulation of the quantity over the interval.
For instance, if f(t)f(t) is the rate of water flowing into a tank, then:
∫f(t) dt\int f(t) \, dt
gives the total volume of water that has flowed into the tank over a time interval.
4. Mean Value of a Function
The integral can be used to find the average value of a function over a certain interval [a,b][a, b]:
Average value of f=1b−a∫abf(x) dx\text{Average value of } f = \frac{1}{b-a} \int_a^b f(x) \, dx
This formula gives the mean height of the function on the interval, which can be useful in various applications, including statistics and physics.
5. Connection to Differential Equations
In the context of differential equations, ∫f(x) dx\int f(x) \, dx is crucial in solving equations where f(x)f(x) represents a rate of change. The integral helps recover the original function from its derivative.
6. Probability and Statistics
In probability, if f(x)f(x) is a probability density function (PDF), then ∫f(x) dx\int f(x) \, dx over an interval gives the probability that a random variable falls within that interval.
2.3.4 Problems on finding definite integral
Finding definite integrals involves calculating the area under a curve between two specific points. Here are several problems with step-by-step solutions.
Problem 1: Basic Polynomial Function
Evaluate the definite integral:
∫13(2×3−4×2+3) dx\int_1^3 (2x^3 – 4x^2 + 3) \, dx
Solution:
- Find the Antiderivative:
- Integrate the function:
∫(2×3−4×2+3) dx=2×44−4×33+3x=x42−4×33+3x+C\int (2x^3 – 4x^2 + 3) \, dx = \frac{2x^4}{4} – \frac{4x^3}{3} + 3x = \frac{x^4}{2} – \frac{4x^3}{3} + 3x + C
- Evaluate from 1 to 3:
[x42−4×33+3x]13=(342−4(33)3+3(3))−(142−4(13)3+3(1))\left[ \frac{x^4}{2} – \frac{4x^3}{3} + 3x \right]_1^3 = \left( \frac{3^4}{2} – \frac{4(3^3)}{3} + 3(3) \right) – \left( \frac{1^4}{2} – \frac{4(1^3)}{3} + 3(1) \right) =(812−36+9)−(12−43+3)= \left( \frac{81}{2} – 36 + 9 \right) – \left( \frac{1}{2} – \frac{4}{3} + 3 \right) =(812−722+182)−(12−86+186)= \left( \frac{81}{2} – \frac{72}{2} + \frac{18}{2} \right) – \left( \frac{1}{2} – \frac{8}{6} + \frac{18}{6} \right) =(272)−(12+106)=272−(12+53)= \left( \frac{27}{2} \right) – \left( \frac{1}{2} + \frac{10}{6} \right) = \frac{27}{2} – \left( \frac{1}{2} + \frac{5}{3} \right) =272−36−106=272−136= \frac{27}{2} – \frac{3}{6} – \frac{10}{6} = \frac{27}{2} – \frac{13}{6}To combine:
=816−136=686=343= \frac{81}{6} – \frac{13}{6} = \frac{68}{6} = \frac{34}{3}
The final answer is:
∫13(2×3−4×2+3) dx=343\int_1^3 (2x^3 – 4x^2 + 3) \, dx = \frac{34}{3}
Problem 2: Trigonometric Function
Evaluate the definite integral:
∫0π2sinx dx\int_0^{\frac{\pi}{2}} \sin x \, dx
Solution:
- Find the Antiderivative:
∫sinx dx=−cosx+C\int \sin x \, dx = -\cos x + C
- Evaluate from 0 to π2\frac{\pi}{2}:
[−cosx]0π2=−cos(π2)−(−cos(0))\left[ -\cos x \right]_0^{\frac{\pi}{2}} = -\cos\left(\frac{\pi}{2}\right) – (-\cos(0)) =−0+1=1= -0 + 1 = 1
The final answer is:
∫0π2sinx dx=1\int_0^{\frac{\pi}{2}} \sin x \, dx = 1
Problem 3: Exponential Function
Evaluate the definite integral:
∫13e2x dx\int_1^3 e^{2x} \, dx
Solution:
- Find the Antiderivative:
∫e2x dx=12e2x+C\int e^{2x} \, dx = \frac{1}{2} e^{2x} + C
- Evaluate from 1 to 3:
[12e2x]13=12e2(3)−12e2(1)\left[ \frac{1}{2} e^{2x} \right]_1^3 = \frac{1}{2} e^{2(3)} – \frac{1}{2} e^{2(1)} =12e6−12e2= \frac{1}{2} e^6 – \frac{1}{2} e^2
The final answer is:
∫13e2x dx=12(e6−e2)\int_1^3 e^{2x} \, dx = \frac{1}{2}(e^6 – e^2)
Problem 4: Area Between Curves
Evaluate the definite integral representing the area between the curves y=x2y = x^2 and y=4y = 4 from x=0x = 0 to x=2x = 2.
Solution:
- Identify the Top and Bottom Functions: Here, y=4y = 4 is above y=x2y = x^2 on the interval [0,2][0, 2].
- Set up the Integral:
Area=∫02(4−x2) dx\text{Area} = \int_0^2 (4 – x^2) \, dx
- Find the Antiderivative:
∫(4−x2) dx=4x−x33+C\int (4 – x^2) \, dx = 4x – \frac{x^3}{3} + C
- Evaluate from 0 to 2:
[4x−x33]02=(4(2)−(2)33)−(4(0)−(0)33)\left[ 4x – \frac{x^3}{3} \right]_0^2 = \left( 4(2) – \frac{(2)^3}{3} \right) – \left( 4(0) – \frac{(0)^3}{3} \right) =(8−83)−0=8−83=243−83=163= \left( 8 – \frac{8}{3} \right) – 0 = 8 – \frac{8}{3} = \frac{24}{3} – \frac{8}{3} = \frac{16}{3}
The final answer is:
Area=163\text{Area} = \frac{16}{3}
2.3.5 Area of plane regions
Calculating the area of plane regions involves finding the space enclosed by curves in a two-dimensional plane. The approach depends on the specific shapes and boundaries of the region. Here are several methods for finding areas of different plane regions.
1. Area Between Two Curves
To find the area between two curves, y=f(x)y = f(x) (the upper curve) and y=g(x)y = g(x) (the lower curve), from x=ax = a to x=bx = b, the area AA can be calculated using the integral:
A=∫ab(f(x)−g(x)) dxA = \int_a^b (f(x) – g(x)) \, dx
Example:
Find the area between the curves y=x2y = x^2 and y=x+2y = x + 2 from x=0x = 0 to x=2x = 2.
- Identify the curves:
- Upper curve: y=x+2y = x + 2
- Lower curve: y=x2y = x^2
- Set up the integral:
A=∫02((x+2)−x2) dxA = \int_0^2 ((x + 2) – x^2) \, dx
- Integrate:
A=∫02(x+2−x2) dx=∫02(−x2+x+2) dxA = \int_0^2 (x + 2 – x^2) \, dx = \int_0^2 (-x^2 + x + 2) \, dx
- Calculate the integral:
=[−x33+x22+2x]02= \left[ -\frac{x^3}{3} + \frac{x^2}{2} + 2x \right]_0^2 =(−(2)33+(2)22+2(2))−(0)= \left( -\frac{(2)^3}{3} + \frac{(2)^2}{2} + 2(2) \right) – \left( 0 \right) =(−83+2+4)=(−83+63+123)= \left( -\frac{8}{3} + 2 + 4 \right) = \left( -\frac{8}{3} + \frac{6}{3} + \frac{12}{3} \right) =103= \frac{10}{3}
The area between the curves is 103\frac{10}{3} square units.
2. Area of a Region Bounded by a Single Curve
To find the area under a curve y=f(x)y = f(x) from x=ax = a to x=bx = b:
A=∫abf(x) dxA = \int_a^b f(x) \, dx
Example:
Find the area under the curve y=x2y = x^2 from x=1x = 1 to x=3x = 3.
- Set up the integral:
A=∫13×2 dxA = \int_1^3 x^2 \, dx
- Integrate:
A=[x33]13A = \left[ \frac{x^3}{3} \right]_1^3
- Calculate the integral:
=((3)33−(1)33)=(273−13)=263= \left( \frac{(3)^3}{3} – \frac{(1)^3}{3} \right) = \left( \frac{27}{3} – \frac{1}{3} \right) = \frac{26}{3}
The area under the curve from x=1x = 1 to x=3x = 3 is 263\frac{26}{3} square units.
3. Area of a Region Bounded by Polar Curves
For regions defined in polar coordinates, the area AA can be calculated using the formula:
A=12∫θ1θ2r(θ)2 dθA = \frac{1}{2} \int_{\theta_1}^{\theta_2} r(\theta)^2 \, d\theta
where r(θ)r(\theta) is the polar function and θ1\theta_1 and θ2\theta_2 are the limits of integration.
Example:
Find the area of one loop of the rose curve defined by r(θ)=2sin(2θ)r(\theta) = 2 \sin(2\theta).
- Determine the limits:
- The loop occurs when r=0r = 0. Setting 2sin(2θ)=02 \sin(2\theta) = 0 gives θ=0\theta = 0 and θ=π2\theta = \frac{\pi}{2}.
- Set up the integral:
A=12∫0π2(2sin(2θ))2 dθA = \frac{1}{2} \int_0^{\frac{\pi}{2}} (2 \sin(2\theta))^2 \, d\theta =12∫0π24sin2(2θ) dθ=2∫0π2sin2(2θ) dθ= \frac{1}{2} \int_0^{\frac{\pi}{2}} 4 \sin^2(2\theta) \, d\theta = 2 \int_0^{\frac{\pi}{2}} \sin^2(2\theta) \, d\theta
- Use the identity sin2x=1−cos(2x)2\sin^2 x = \frac{1 – \cos(2x)}{2}:
=2∫0π21−cos(4θ)2 dθ=∫0π2(1−cos(4θ)) dθ= 2 \int_0^{\frac{\pi}{2}} \frac{1 – \cos(4\theta)}{2} \, d\theta = \int_0^{\frac{\pi}{2}} (1 – \cos(4\theta)) \, d\theta
- Calculate the integral:
=[θ−sin(4θ)4]0π2=(π2−0)−(0−0)=π2= \left[ \theta – \frac{\sin(4\theta)}{4} \right]_0^{\frac{\pi}{2}} = \left( \frac{\pi}{2} – 0 \right) – \left( 0 – 0 \right) = \frac{\pi}{2}
The area of one loop of the rose curve is π2\frac{\pi}{2} square units.