IB Mathematics AA SL Derivatives of xn , sinx , cosx , tanx Study Notes - New Syllabus
IB Mathematics AA SL Derivatives of xn , sinx , cosx , tanx Study Notes
LEARNING OBJECTIVE
- Derivative of xn (n ∈ ℚ), sinx, cosx, ex and lnx
Key Concepts:
- Basic Derivatives
- Sum Rule & Constant Multiple Rule
- Chain Rule
- Product Rule & Quotient Rule
- Application
- IBDP Maths AA SL- IB Style Practice Questions with Answer-Topic Wise-Paper 1
- IBDP Maths AA SL- IB Style Practice Questions with Answer-Topic Wise-Paper 2
- IB DP Maths AA HL- IB Style Practice Questions with Answer-Topic Wise-Paper 1
- IB DP Maths AA HL- IB Style Practice Questions with Answer-Topic Wise-Paper 2
- IB DP Maths AA HL- IB Style Practice Questions with Answer-Topic Wise-Paper 3
Basic Derivatives
Basic Derivatives
The derivative of standard functions such as power functions, trigonometric, exponential, and logarithmic functions follows known formulas:
Function | Derivative |
---|---|
\( f(x) = x^n \) (where \( n \in \mathbb{Q} \)) | \( f'(x) = nx^{n-1} \) |
\( f(x) = \sin x \) | \( f'(x) = \cos x \) |
\( f(x) = \cos x \) | \( f'(x) = -\sin x \) |
\( f(x) = e^x \) | \( f'(x) = e^x \) |
\( f(x) = \ln x \) | \( f'(x) = \dfrac{1}{x} \) |
Example Differentiate the following functions: ▶️ Answer/ExplanationSolution: a) \( f'(x) = 4x^{3} \) b) \( f'(x) = \cos x \) c) \( f'(x) = e^x \) d) \( f'(x) = \dfrac{1}{x} \) |
Sum Rule & Constant Multiple Rule
Sum Rule & Constant Multiple Rule
Sum Rule:
\( \dfrac{d}{dx}[f(x) + g(x)] = f'(x) + g'(x) \)
Constant Multiple Rule:
\( \dfrac{d}{dx}[a \cdot f(x)] = a \cdot f'(x) \), where \( a \) is a constant
Explanation:
You can differentiate term-by-term. Constants in front stay as multipliers
Example Differentiate the following: ▶️ Answer/ExplanationSolution: a) \( f'(x) = 3 \cdot 4x^3 + 5 = 12x^3 + 5 \) |
Chain Rule (Composite Functions)
Chain Rule (Composite Functions)
If \( f(x) = h(g(x)) \), then
$f^{\prime}(x) = h{\prime}(g(x)) \cdot g{\prime}(x)$
In words:
Differentiate the outer function, keeping the inner function unchanged, then multiply by the derivative of the inner function.
Example Differentiate the following: ▶️ Answer/ExplanationSolutions: a) Let outer = \( \sin(u) \), inner = \( u = 3x \) b) Outer = \( \ln(u) \), inner = \( u = 2x^2 + 1 \) c) Outer = \( e^u \), inner = \( u = x^2 + 2 \) |
Product Rule & Quotient Rule
Product Rule & Quotient Rule
Product Rule:
$\frac{d}{dx}[f(x) \cdot g(x)] = f^{\prime}(x)g(x) + f(x)g^{\prime}(x)$
Quotient Rule:
$\frac{d}{dx}\left[\frac{f(x)}{g(x)}\right] = \frac{f'(x)g(x) – f(x)g'(x)}{(g(x))^2}$
Example: Differentiate the following: ▶️ Answer/ExplanationSolutions: a) Use product rule: \( f'(x) = 2x \sin x + x^2 \cos x \) b) Use quotient rule: |
Applications of Differentiation in Physics
Applications of Differentiation in Physics
Differentiation plays a critical role in describing motion and electromagnetic phenomena in physics. Two key examples are:
- Uniform Circular Motion: Differentiation of position functions gives velocity and acceleration vectors.
- Induced emf: Faraday’s law involves the rate of change of magnetic flux, modeled using derivatives.
Example: Uniform Circular Motion
A particle moves in a circle of radius \( r = 5 \) m with angular velocity \( \omega = 2 \) rad/s. Its position is given by:
▶️ Answer/ExplanationStep 1: Differentiate \( \vec{r}(t) \) to find velocity: $ \vec{v}(t) = \frac{d\vec{r}}{dt} = -10 \sin(2t)\, \hat{i} + 10 \cos(2t)\, \hat{j} $ Step 2: Differentiate again to find acceleration: $ \vec{a}(t) = \frac{d\vec{v}}{dt} = -20 \cos(2t)\, \hat{i} – 20 \sin(2t)\, \hat{j} $ Step 3: The acceleration points towards the center and has magnitude: $ |\vec{a}(t)| = \sqrt{(-20 \cos(2t))^2 + (-20 \sin(2t))^2} = 20 $ This confirms the object is undergoing uniform circular motion with constant centripetal acceleration. |
Example: Induced emf using Faraday’s Law
A magnetic field through a coil changes over time according to: $ \Phi(t) = 3t^2 – 2t \text{ (in Wb)} $ Use Faraday’s law to find the induced emf at time \( t = 2 \) s. ▶️ Answer/ExplanationStep 1: Use Faraday’s Law: $ \mathcal{E} = -\frac{d\Phi}{dt} $ $ \frac{d\Phi}{dt} = \frac{d}{dt}(3t^2 – 2t) = 6t – 2 $ Step 2: Substitute \( t = 2 \): $ \mathcal{E} = -(6(2) – 2) = -10 \text{ V} $ Conclusion: The induced emf at \( t = 2 \) s is −10 V. |