The second order derivative is the derivative of the derivative. If we differentiate once, we get dydx. Differentiating again gives d2ydx2, which is known as the second derivative. It can also be written as f″(x). The second derivative gives the rate of change of the derivative, or the gradient of the curve, with respect to x. Important: The second derivative is less than zero at a local maximum. The second derivative is greater than zero at a local minimum. The second derivative is zero at a point of inflection.
Imagine a car is travelling along a straight road. At any given time, its distance from its starting point can be assigned to the value x. Therefore, the rate with which this distance changes with respect to time is dxdt - the velocity. The rate at which their velocity changes with respect to time - the acceleration - can then be expressed as the second order derivative, d2xdt2. This is demonstrated in the diagram below.
In this example, the Displacement (Distance from starting position) vs Time graph is a quadratic function. Differentiating this function should give us a linear function. This is because when we differentiate a function containing an x2 term, this will be come an x term. This means what was previously a quadratic equation now becomes an equation of a line. The second graph shows dxdt, the velocity, as a function of time. The slope of the velocity vs time graph is d2xdt2, the acceleration. As you may already know, the slope of a straight line is constant. This is because when we differentiate the x term, we get a constant. Therefore, in this case, d2xdt2 is a constant. As a result, the graph of d2xdt2 as a function of time is simply a constant.
Part 1: Without detailed calculation, draw a rough sketch of the graph of the slope of the function f(x)=2x3−3x2−36x+4
Simply differentiate again to find the second derivative. f″(x)=(6)(2x2−1−x1−1)=6(2x−1)
Question:A cyclist starts cycling at t=0 from x=0. For the first ten seconds, her journey can be described by the equation x=4√5t+6t2
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