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Derivative of a Function

The derivative of a function is a fundamental concept in calculus and mathematical analysis. It represents the rate at which a function changes as its input (or variable) changes. In other words, the derivative provides information about the slope of the function at a particular point, or how steep the function is at that point.
Let's consider a function \(f(x)\). The derivative of \(f(x)\) with respect to \(x\) is denoted as \(f' (x)\), or sometimes as \( \frac{df}{dx} \) . To find the derivative, we look at the limit of the average rate of change of the function as the interval between two points on the function approaches zero. Mathematically, this is expressed as:
\( f'(x) = \underset{h \to 0}{\lim} \frac{f(x + h) - f(x)}{h} \)
Here, \(h\) is a very small change in the input \(x\), and the limit ensures that \(h\) approaches zero.

There are several rules and techniques for finding derivatives of different types of functions. Some of the most common rules are:

For example, let's find the derivative of
\( f(x)=3x^2 +4x+5 \)

Using the sum rule, we can break this down into three separate derivatives:
\( f' (x) = \frac{d}{dx} (3x^2 )+ \frac{d}{dx} (4x)+ \frac{d}{dx} (5) \)

Now, applying the power rule to the first two terms and the constant rule to the last term, we get:
\( f' (x) = (6x)+(4)+(0) \)

So, the derivative of the function is:
\( f' (x)=6x+4 \)


In summary, the derivative of a function provides information about the rate of change or slope of the function at any point. There are various rules and techniques for finding derivatives, which can be applied depending on the type and structure of the function.

In addition to the basic rules and techniques mentioned earlier, there are also some special techniques and properties related to derivatives that can be useful when working with more complex functions or specific types of functions.

Implicit Differentiation: When dealing with equations where both \(x\) and \(y\) are implicitly defined (e.g., \(x^2+y^2=1\) ), we can use implicit differentiation to find the derivative. This involves taking the derivative of both sides with respect to \(x\) and then solving for\(\frac{dy}{dx} \)

Higher-order derivatives: The derivative of a function can be taken multiple times, resulting in higher-order derivatives. For example, the second derivative \(f'' (x)\) is the derivative of the first derivative, \(f' (x)\). Similarly, the third derivative, \(f''' (x)\), is the derivative of the second derivative, and so on. Higher-order derivatives are useful in studying the curvature, concavity, and inflection points of a function.

Inverse Function Rule: \(y=f(x) \) and \(x=g(y) \) are inverse functions, then:
\( \frac{dx}{dy}= 1 \div \frac{dy}{dx} \)

Parametric Functions: When a function is defined parametrically, such as \(x(t)\) and \(y(t)\), the derivative of \(y\) with respect to \(x\) can be found by taking the derivative of \(y\) with respect to \(t\) and dividing it by the derivative of \(x\) with respect to \(t\):
\( \frac{dy}{dx} = \frac{dy}{dt} \div \frac{dx}{dt} \)

Differentiating Trigonometric Functions: Derivatives of basic trigonometric functions can be useful when working with functions involving sine, cosine, tangent, and their inverse functions. Some of the key derivatives are:


Differentiating Exponential and Logarithmic Functions:

Differentiating Hyperbolic Functions: Hyperbolic functions are defined in terms of exponentials and have derivatives similar to trigonometric functions. Some important derivatives are:

Taylor Series: The Taylor series is a representation of a function as an infinite sum of terms, calculated using the function's derivatives at a single point. If a function \(f(x)\) has continuous derivatives of all orders in an interval containing \(x=a\), then the Taylor series of \(f(x)\) about the point \(x=a\) is:

\( \small f(x) = f(a) + f'(a)(x - a) + \) \( \small \frac{f''(a)(x - a)^2}{2!} + \frac{f'''(a)(x - a)^3}{3!} + \ldots \)

Partial Derivatives: When dealing with functions of multiple variables, such as \(f(x,y)\) or \(f(x,y,z)\), partial derivatives are used to find the rate of change of the function with respect to one variable, while keeping the other variables constant. The partial derivative of \(f(x,y)\) with respect to \(x\) is denoted as \( \frac{\partial f}{ \partial x} \) , and similarly, with respect to \(y\) as \( \frac{\partial f}{ \partial y} \). The process of finding partial derivatives is similar to finding the derivative of a single-variable function, treating other variables as constants while differentiating with respect to the chosen variable.

Gradient: The gradient is a vector containing all the first-order partial derivatives of a multivariable function.
For a function \(f(x,y)\), the gradient is denoted as \( \vec{\nabla}f \) or grad \(f\), and is defined as:
\( \vec{\nabla}f = \left( \frac{\partial f}{\partial x}, \frac{\partial f}{\partial y} \right) \)

For a function \(f(x,y,z)\), the gradient is:
\( \vec{\nabla}f = \left( \frac{\partial f}{\partial x}, \frac{\partial f}{\partial y}, \frac{\partial f}{\partial z} \right) \)

The gradient is crucial in understanding the direction of the steepest increase or decrease of a function, and it plays a significant role in optimization and other applications in physics, engineering, and economics.

Directional Derivative: The directional derivative of a function of multiple variables represents the rate of change of the function in a specific direction.
Given a function \(f(x,y)\), the directional derivative in the direction of the unit vector \( u=(u_1,u_2 )\) is denoted as \(D_{u} f \) and is defined as:
\( D_{u} f = \vec{\nabla}f \cdot \vec{u} = \frac{\partial f}{\partial x} u_1 + \frac{\partial f}{\partial y} u_2 \)

For a function \( f(x,y,z) \), the directional derivative in the direction of the unit vector \( u=(u_1,u_2,u_3 ) \) is:
\( D_{u} f = \vec{\nabla}f \cdot \vec{u} = \frac{\partial f}{\partial x} u_1 + \frac{\partial f}{\partial y} u_2 + \frac{\partial f}{\partial z} u_3 \)

Laplacian: The Laplacian is a scalar quantity derived from the gradient and is associated with the second-order partial derivatives of a function.
For a function \(f(x,y)\), the Laplacian is denoted as \( \vec{\nabla}^2 f \) and is defined as:
\( \vec{\nabla}^2 f = \frac{\partial^2 f}{\partial x^2} + \frac{\partial^2 f}{\partial y^2} \)

For a function \(f(x,y,z)\), the Laplacian is:
\( \vec{\nabla}^2 f = \frac{\partial^2 f}{\partial x^2} + \frac{\partial^2 f}{\partial y^2} + \frac{\partial^2 f}{\partial z^2} \)