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Chapter – 13
Applications of Derivatives
When we talk about derivatives in this context, we often refer to the derivative of a function with respect to time or another variable, which gives us the rate at which that function is changing. For example, if $latex y = f(x)$ represents the distance traveled by an object over time $latex x$, then the derivative $latex \frac{dy}{dx}$, or $latex f'(x)$,
represents the distance traveled by an object over time $latex x$, then the derivative $latex \frac{dy}{dx}$, or $latex f'(x)$, represents the object’s velocity – how quickly the distance is changing with time. Similarly, in physics, the derivative of velocity with respect to time gives acceleration, a measure of how the velocity is changing over time.
Applications of Derivatives Class 12 Maths Solutions PDF
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Derivatives as the Rate Measure
Let $latex y = f(x)$ be the continuous function. By the definition of a function, $latex y$ changes while $latex x$ will change. If $latex \Delta x$ and $latex \Delta y$ be the small changes in $latex x$ and $latex y$ respectively, then $latex \frac{\Delta y}{\Delta x} = \frac{f(x + \Delta x) – f(x)}{\Delta x}$
is the change in $latex y$ per unit change in $latex x$ and hence is the average rate of change of $latex y$ with respect to $latex x$ on the interval $latex [x, x + \Delta x]$. The average rate of change becomes the instantaneous rate of change when $latex \Delta x \rightarrow 0$ provided that the limit exists. Thus,
$latex \lim_{{\Delta x \to 0}} \frac{\Delta y}{\Delta x} = \lim_{{\Delta x \to 0}} \frac{f(x_0 + \Delta x) – f(x_0)}{\Delta x}$. i.e,
$latex \left(\frac{dy}{dx}\right){x = x_0} = \lim{{\Delta x \to 0}} \frac{f(x_0 + \Delta x) – f(x_0)}{\Delta x}$ is the instantaneous rate of change of $latex y$ with respect to $latex x$ at $latex x = x_0$.
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