Before we begin, let’s review some key concepts:
Exercise 1: Basic Trigonometric Derivatives
Without referring to any formula, prove that:
d d x ( sin 2 x ) = sin 2 x \frac{d}{dx}(\sin^2 x) = \sin 2x d x d ( sin 2 x ) = sin 2 x
d d x ( tan x ) = sec 2 x \frac{d}{dx}(\tan x) = \sec^2 x d x d ( tan x ) = sec 2 x
Given that y = x 2 cos 3 x y = x^2 \cos 3x y = x 2 cos 3 x , find d y d x \frac{dy}{dx} d x d y
Exercise 2: Basic Hyperbolic Functions
Write down the definitions of the following functions:
sinh x , cosh x , tanh x , sech x , csch x , coth x \sinh x, \cosh x, \tanh x, \operatorname{sech} x, \operatorname{csch} x, \coth x sinh x , cosh x , tanh x , sech x , csch x , coth x
The derivative of a function at a point represents the gradient of the tangent line at that point. This can be understood as the limit of the gradient of secant lines.
Definition: Derivative as a Limit from First Principle
The derivative of a function f f f at a point x = a x = a x = a is defined as:
f ′ ( a ) = lim h → 0 f ( a + h ) − f ( a ) h f'(a) = \lim_{h \to 0} \frac{f(a+h) - f(a)}{h} f ′ ( a ) = lim h → 0 h f ( a + h ) − f ( a )
provided this limit exists.
From an algebraic perspective, differentiation can be viewed as finding the best linear approximation to a function near a point.
Theorem: Linear Approximation
Near x = a x = a x = a , a differentiable function f ( x ) f(x) f ( x ) can be approximated by:
f ( x ) ≈ f ( a ) + f ′ ( a ) ( x − a ) f(x) \approx f(a) + f'(a)(x - a) f ( x ) ≈ f ( a ) + f ′ ( a ) ( x − a )
This is called the linear approximation or tangent line approximation.
Example: Application to Error Analysis
Consider estimating 4.1 \sqrt{4.1} 4.1 using the linear approximation to f ( x ) = x f(x) = \sqrt{x} f ( x ) = x at x = 4 x = 4 x = 4 .
Since f ′ ( x ) = 1 2 x f'(x) = \frac{1}{2\sqrt{x}} f ′ ( x ) = 2 x 1 , we have:
4.1 ≈ 4 + 1 2 4 ( 4.1 − 4 ) = 2 + 0.1 4 = 2.025 \sqrt{4.1} \approx \sqrt{4} + \frac{1}{2\sqrt{4}}(4.1 - 4) = 2 + \frac{0.1}{4} = 2.025 4.1 ≈ 4 + 2 4 1 ( 4.1 − 4 ) = 2 + 4 0.1 = 2.025
Example: Derivative of arcsin
Show that d d x ( arcsin x ) = 1 1 − x 2 \frac{d}{dx}(\arcsin x) = \frac{1}{\sqrt{1 - x^2}} d x d ( arcsin x ) = 1 − x 2 1 .
Implicit Differentiation:
Let y = arcsin x y = \arcsin x y = arcsin x , then sin y = x \sin y = x sin y = x
Differentiate both sides: cos y d y d x = 1 \cos y \frac{dy}{dx} = 1 cos y d x d y = 1
Therefore d y d x = 1 cos y \frac{dy}{dx} = \frac{1}{\cos y} d x d y = c o s y 1
Since sin 2 y + cos 2 y = 1 \sin^2 y + \cos^2 y = 1 sin 2 y + cos 2 y = 1 , we have cos 2 y = 1 − sin 2 y = 1 − x 2 \cos^2 y = 1 - \sin^2 y = 1 - x^2 cos 2 y = 1 − sin 2 y = 1 − x 2
Thus d y d x = 1 1 − x 2 \frac{dy}{dx} = \frac{1}{\sqrt{1 - x^2}} d x d y = 1 − x 2 1
Guided Exercise: Derivative of arccos
Show that d d x ( arccos x ) = − 1 1 − x 2 \frac{d}{dx}(\arccos x) = -\frac{1}{\sqrt{1 - x^2}} d x d ( arccos x ) = − 1 − x 2 1 .
Method 1 (Using arccos x + arcsin x = π 2 \arccos x + \arcsin x = \frac{\pi}{2} arccos x + arcsin x = 2 π ):
Method 2 (Implicit Differentiation):
Try this yourself using y = arccos x ⟹ cos y = x y = \arccos x \implies \cos y = x y = arccos x ⟹ cos y = x .
Guided Exercise: Derivative of arctan
Show that d d x ( arctan x ) = 1 1 + x 2 \frac{d}{dx}(\arctan x) = \frac{1}{1 + x^2} d x d ( arctan x ) = 1 + x 2 1 .
Guided Exercise: Basic Hyperbolic Derivatives
Using the definitions:
sinh x = e x − e − x 2 , cosh x = e x + e − x 2 \sinh x = \frac{e^x - e^{-x}}{2}, \qquad \cosh x = \frac{e^x + e^{-x}}{2} sinh x = 2 e x − e − x , cosh x = 2 e x + e − x
show that:
d d x ( sinh x ) = cosh x , d d x ( cosh x ) = sinh x , d d x ( tanh x ) = sech 2 x \frac{d}{dx}(\sinh x) = \cosh x, \quad \frac{d}{dx}(\cosh x) = \sinh x, \quad \frac{d}{dx}(\tanh x) = \operatorname{sech}^2 x d x d ( sinh x ) = cosh x , d x d ( cosh x ) = sinh x , d x d ( tanh x ) = sech 2 x
Guided Exercise: Reciprocal Hyperbolic Derivatives
Show that:
d d x ( sech x ) = − tanh x sech x \frac{d}{dx}(\operatorname{sech} x) = -\tanh x \operatorname{sech} x d x d ( sech x ) = − tanh x sech x
d d x ( csch x ) = − coth x csch x \frac{d}{dx}(\operatorname{csch} x) = -\coth x \operatorname{csch} x d x d ( csch x ) = − coth x csch x
d d x ( coth x ) = − csch 2 x \frac{d}{dx}(\coth x) = -\operatorname{csch}^2 x d x d ( coth x ) = − csch 2 x
Hint: Use the quotient rule and previous results.
Guided Exercise: Derivative of arsinh
Show that d d x ( arsinh x ) = 1 x 2 + 1 \frac{d}{dx}(\operatorname{arsinh} x) = \frac{1}{\sqrt{x^2 + 1}} d x d ( arsinh x ) = x 2 + 1 1 .
Method 1 (Using definition):
Use arsinh x = ln ( x + x 2 + 1 ) \operatorname{arsinh} x = \ln(x + \sqrt{x^2 + 1}) arsinh x = ln ( x + x 2 + 1 )
Apply chain rule to differentiate
Method 2 (Implicit Differentiation):
Let y = arsinh x y = \operatorname{arsinh} x y = arsinh x , then sinh y = x \sinh y = x sinh y = x
Differentiate both sides: cosh y d y d x = 1 \cosh y \frac{dy}{dx} = 1 cosh y d x d y = 1
Use cosh 2 y − sinh 2 y = 1 \cosh^2 y - \sinh^2 y = 1 cosh 2 y − sinh 2 y = 1 to eliminate cosh y \cosh y cosh y
Guided Exercise: Derivative of arcosh
Show that d d x ( arcosh x ) = 1 x 2 − 1 \frac{d}{dx}(\operatorname{arcosh} x) = \frac{1}{\sqrt{x^2 - 1}} d x d ( arcosh x ) = x 2 − 1 1 , for x > 1 x > 1 x > 1 .
Method 1 (Using definition arcosh x = ln ( x + x 2 − 1 ) \operatorname{arcosh} x = \ln(x + \sqrt{x^2 - 1}) arcosh x = ln ( x + x 2 − 1 ) ):
Method 2 (Implicit Differentiation):
Try this yourself using y = arcosh x ⟹ cosh y = x y = \operatorname{arcosh} x \implies \cosh y = x y = arcosh x ⟹ cosh y = x .
Guided Exercise: Derivative of artanh
Show that d d x ( artanh x ) = 1 1 − x 2 \frac{d}{dx}(\operatorname{artanh} x) = \frac{1}{1 - x^2} d x d ( artanh x ) = 1 − x 2 1 , for ∣ x ∣ < 1 |x| < 1 ∣ x ∣ < 1 .
Method 1 (Using definition artanh x = 1 2 ln ( 1 + x 1 − x ) \operatorname{artanh} x = \frac{1}{2}\ln\left(\frac{1+x}{1-x}\right) artanh x = 2 1 ln ( 1 − x 1 + x ) ):
Method 2 (Implicit Differentiation):
Try this yourself using y = artanh x ⟹ tanh y = x y = \operatorname{artanh} x \implies \tanh y = x y = artanh x ⟹ tanh y = x .
Example: Q04 WFM03/01, June 2021
(a) Given that f ( x ) = x arccos x f(x) = x \arccos x f ( x ) = x arccos x where − 1 ≤ x ≤ 1 -1 \leq x \leq 1 − 1 ≤ x ≤ 1 , find the exact value of f ′ ( 0.5 ) f'(0.5) f ′ ( 0.5 ) .
(b) Given that g ( x ) = arctan ( e 2 x ) g(x) = \arctan(e^{2x}) g ( x ) = arctan ( e 2 x ) , show that
g ′ ′ ( x ) = k sech ( 2 x ) tanh ( 2 x ) g''(x) = k \operatorname{sech}(2x) \tanh(2x) g ′′ ( x ) = k sech ( 2 x ) tanh ( 2 x )
where k k k is a constant to be found.
Example: Q03 WFM03/01, Jan 2022
(a) Given that y = arsech ( x 2 ) y = \operatorname{arsech}\left(\frac{x}{2}\right) y = arsech ( 2 x ) , where 0 < x ≤ 2 0 < x \leq 2 0 < x ≤ 2 , show that
d y d x = p x q − x 2 \frac{dy}{dx} = \frac{p}{x\sqrt{q - x^2}} d x d y = x q − x 2 p
where p p p and q q q are constants to be determined.
(b) Given that f ( x ) = artanh ( x ) + arsech ( x 2 ) f(x) = \operatorname{artanh}(x) + \operatorname{arsech}\left(\frac{x}{2}\right) f ( x ) = artanh ( x ) + arsech ( 2 x ) where 0 < x ≤ 1 0 < x \leq 1 0 < x ≤ 1 , determine, in simplest form, the exact value of x x x for which f ′ ( x ) = 0 f'(x) = 0 f ′ ( x ) = 0 .
Example: Q04 WFM03/01, June 2022
Given that y = artanh ( cos x + a cos x − a ) y = \operatorname{artanh}\left(\frac{\cos x + a}{\cos x - a}\right) y = artanh ( c o s x − a c o s x + a ) where a a a is a non-zero constant, show that
d y d x = k tan x \frac{dy}{dx} = k \tan x d x d y = k tan x
where k k k is a constant to be determined.
Key Points
The derivative can be understood both geometrically (as slope) and algebraically (as rate of change)
Inverse trigonometric derivatives involve the form 1 1 − x 2 \frac{1}{\sqrt{1-x^2}} 1 − x 2 1
Hyperbolic function derivatives mirror trigonometric ones, but with some sign differences
Inverse hyperbolic derivatives can be derived using logarithmic definitions
Common Mistakes
Forgetting the minus sign in d d x ( arccos x ) \frac{d}{dx}(\arccos x) d x d ( arccos x )
Confusing domains of inverse functions
Not recognizing hyperbolic identities
Incorrect use of chain rule with composite functions
Past Paper Question: 6669/s10/01/5
Given that y = ( arcosh 3 x ) 2 y = (\operatorname{arcosh} 3x)^2 y = ( arcosh 3 x ) 2 , where 3 x > 1 3x > 1 3 x > 1 , show that:
(a) ( 9 x 2 − 1 ) ( d y d x ) 2 = 36 y (9x^2 - 1)\left(\frac{dy}{dx}\right)^2 = 36y ( 9 x 2 − 1 ) ( d x d y ) 2 = 36 y (5 marks)
(b) ( 9 x 2 − 1 ) d 2 y d x 2 + 9 x d y d x = 18 (9x^2 - 1)\frac{d^2y}{dx^2} + 9x\frac{dy}{dx} = 18 ( 9 x 2 − 1 ) d x 2 d 2 y + 9 x d x d y = 18 (4 marks)
Past Paper Question: 6669/s14/01/5
Given that y = artanh x 1 + x 2 y = \operatorname{artanh}\frac{x}{\sqrt{1+x^2}} y = artanh 1 + x 2 x , show that
d y d x = 1 1 + x 2 \frac{dy}{dx} = \frac{1}{\sqrt{1+x^2}} d x d y = 1 + x 2 1
(4 marks)
Key Concept 1: Unit Circle and Trigonometric Functions
For a point P ( cos θ , sin θ ) P(\cos\theta, \sin\theta) P ( cos θ , sin θ ) on the unit circle:
cos θ \cos\theta cos θ is the x x x -coordinate
sin θ \sin\theta sin θ is the y y y -coordinate
As θ \theta θ increases, P P P moves counterclockwise
Key Concept 2: Definition of Derivative
The derivative of a function f ( x ) f(x) f ( x ) at point x x x is defined as the limit of the difference quotient
f ( x + h ) − f ( x ) h \frac{f(x+h) - f(x)}{h} h f ( x + h ) − f ( x )
as h h h approaches 0 0 0 .
Key Concept 3: Arclength Definition of Arcsin
On the unit circle, arcsin x \arcsin x arcsin x represents the arclength of the arc from the point ( 1 , 0 ) (1, 0) ( 1 , 0 ) to the point ( 1 − x 2 , x ) (\sqrt{1-x^2}, x) ( 1 − x 2 , x ) .
Key Properties:
The angle θ = arcsin ( x ) \theta = \arcsin(x) θ = arcsin ( x ) is measured in radians
For any point ( 1 − x 2 , x ) (\sqrt{1-x^2}, x) ( 1 − x 2 , x ) on the unit circle, x = sin ( θ ) x = \sin(\theta) x = sin ( θ )
The arclength equals the radian measure θ \theta θ (since radius = 1)
Domain restriction ∣ x ∣ ≤ 1 |x| \leq 1 ∣ x ∣ ≤ 1 comes from the unit circle geometry
Task 1: Physical Method
Consider a particle moving on the plane with parametric equations:
x ( t ) = cos t , y ( t ) = sin t x(t) = \cos t, \quad y(t) = \sin t x ( t ) = cos t , y ( t ) = sin t
What does this mean physically?
The velocity vector v ⃗ ( t ) \vec{v}(t) v ( t ) is given by v ⃗ ( t ) = ( x ′ ( t ) , y ′ ( t ) ) \vec{v}(t) = (x'(t), y'(t)) v ( t ) = ( x ′ ( t ) , y ′ ( t )) .
What is the direction of the velocity vector?
Why must it be perpendicular to the position vector?
What is its magnitude?
How does this physical interpretation help us understand why d d t sin t = cos t \frac{d}{dt}\sin t = \cos t d t d sin t = cos t ?
Task 2: Understanding the Derivative Through Limits
Let’s break down the derivative of sine function step by step:
At any point a a a , we want to find ( sin x ) ′ (\sin x)' ( sin x ) ′ at x = a x = a x = a . This means we need to evaluate:
sin ( a + h ) − sin a h as h gets closer and closer to 0 \frac{\sin(a+h) - \sin a}{h} \quad \text{as $h$ gets closer and closer to 0} h s i n ( a + h ) − s i n a as h gets closer and closer to 0
We can use the trigonometric addition formula:
sin ( a + h ) = sin a cos h + cos a sin h \sin(a+h) = \sin a \cos h + \cos a \sin h sin ( a + h ) = sin a cos h + cos a sin h
Q: Substitute this into our difference quotient and show that:
sin ( a + h ) − sin a h = sin a ⋅ ( cos h − 1 ) h + cos a ⋅ sin h h \frac{\sin(a+h) - \sin a}{h} = \sin a \cdot \frac{(\cos h - 1)}{h} + \cos a \cdot \frac{\sin h}{h} h s i n ( a + h ) − s i n a = sin a ⋅ h ( c o s h − 1 ) + cos a ⋅ h s i n h
To show this approaches cos a \cos a cos a , we need to understand what happens to:
sin h h \frac{\sin h}{h} h s i n h as h h h approaches 0 0 0
cos h − 1 h \frac{\cos h - 1}{h} h c o s h − 1 as h h h approaches 0 0 0
Q: Using the identity cos h − 1 = − 2 sin 2 ( h / 2 ) \cos h - 1 = -2\sin^2(h/2) cos h − 1 = − 2 sin 2 ( h /2 ) , show that:
cos h − 1 h = − sin ( h / 2 ) ⋅ sin ( h / 2 ) h / 2 \frac{\cos h - 1}{h} = -\sin(h/2) \cdot \frac{\sin(h/2)}{h/2} h c o s h − 1 = − sin ( h /2 ) ⋅ h /2 s i n ( h /2 )
Hence explain why cos h − 1 h \frac{\cos h - 1}{h} h c o s h − 1 approaches 0 0 0 as long as sin h h \frac{\sin h}{h} h s i n h approaches 1 1 1 as h h h approaches 0 0 0 .
Therefore, if we can show sin h h \frac{\sin h}{h} h s i n h approaches 1 1 1 as h h h approaches 0 0 0 (which we’ll do in Task 3), we’ll have proved that the derivative of sin x \sin x sin x at any point a a a is cos a \cos a cos a .
Task 3: Analytical Method
In this task, we will explore an alternative definition of the sine function through integration and use such definition to prove that sin x x \frac{\sin x}{x} x s i n x approaches 1 1 1 as x x x approaches 0 0 0 .
Part 1: Understanding Arclength and Arcsine
Recall from Task 1 that when a point moves along the unit circle with position vector ( cos t , sin t ) (\cos t, \sin t) ( cos t , sin t ) :
Its velocity vector is ( − sin t , cos t ) (-\sin t, \cos t) ( − sin t , cos t )
The speed (magnitude of velocity) is constant = 1
Therefore, the parameter t t t equals the arclength traveled
Consider the arclength definition of arcsin x \arcsin x arcsin x (see Key Concept 3):
On the unit circle, arcsin x \arcsin x arcsin x is the arclength from ( 1 , 0 ) (1, 0) ( 1 , 0 ) to ( 1 − x 2 , x ) (\sqrt{1-x^2}, x) ( 1 − x 2 , x )
For a curve given by ( f ( t ) , g ( t ) ) (f(t), g(t)) ( f ( t ) , g ( t )) , its arclength is ∫ ( f ′ ( t ) ) 2 + ( g ′ ( t ) ) 2 d t \int \sqrt{(f'(t))^2 + (g'(t))^2}\,dt ∫ ( f ′ ( t ) ) 2 + ( g ′ ( t ) ) 2 d t
Remark: this is how “arc”sin is related to “arc”length and we will discuss the computation of arclength in detail in the next chapter.
Q: Using the arclength formula above:
(a) Express the arc representing arcsin x \arcsin x arcsin x as ( x ( t ) , y ( t ) ) = ( 1 − t 2 , t ) (x(t), y(t)) = (\sqrt{1-t^2}, t) ( x ( t ) , y ( t )) = ( 1 − t 2 , t ) for 0 ≤ t ≤ x 0 \leq t \leq x 0 ≤ t ≤ x .
(b) Show that arcsin x = ∫ 0 x 1 1 − t 2 d t \arcsin x = \int_0^x \frac{1}{\sqrt{1-t^2}}\,dt arcsin x = ∫ 0 x 1 − t 2 1 d t .
Part 2: Properties of the Integral
For the function f ( x ) = ∫ 0 x 1 1 − t 2 d t f(x) = \int_0^x \frac{1}{\sqrt{1-t^2}}\,dt f ( x ) = ∫ 0 x 1 − t 2 1 d t , explain why:
The value of f ( 0 ) f(0) f ( 0 ) must be 0 0 0
As x x x increases, f ( x ) f(x) f ( x ) must increase (think about the area under a positive curve)
The function is symmetric about the origin (what happens if you replace x x x with − x -x − x ?)
For any x x x between 0 0 0 and 1 1 1 :
Find the smallest value of 1 1 − t 2 \frac{1}{\sqrt{1-t^2}} 1 − t 2 1 on [ 0 , x ] [0, x] [ 0 , x ]
Find the largest value of 1 1 − t 2 \frac{1}{\sqrt{1-t^2}} 1 − t 2 1 on [ 0 , x ] [0, x] [ 0 , x ]
Use these facts to explain why:
x ≤ f ( x ) ≤ x 1 − x 2 x \leq f(x) \leq \frac{x}{\sqrt{1-x^2}} x ≤ f ( x ) ≤ 1 − x 2 x
Part 3: The Fundamental Property
The Squeeze Theorem states: if a ( x ) ≤ b ( x ) ≤ c ( x ) a(x) \leq b(x) \leq c(x) a ( x ) ≤ b ( x ) ≤ c ( x ) for all x x x near some value p p p , and if a ( x ) a(x) a ( x ) and c ( x ) c(x) c ( x ) both approach the same value L L L as x x x approaches p p p , then b ( x ) b(x) b ( x ) must also approach L L L .
Use the squeeze theorem to explain why f ( x ) x \frac{f(x)}{x} x f ( x ) approaches 1 1 1 as x x x approaches 0 0 0 .
Let y = f ( x ) y = f(x) y = f ( x ) , then show that sin y y \frac{\sin y}{y} y s i n y also approaches 1 1 1 as y y y approaches 0 0 0 .