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Calculate the derivative of the following functions. $$y=\theta^{2} \sec 5 \theta$$

Short Answer

Expert verified
Answer: The derivative is \(\frac{dy}{d\theta} = 5\theta^2\sec(5\theta)\tan(5\theta) + 2\theta\sec(5\theta)\).

Step by step solution

01

Identify the components of the function

We can rewrite the given function as a product of two functions of \(\theta\): $$(u(\theta) \cdot v(\theta))=\theta^2 \cdot \sec(5\theta)$$ where \(u(\theta) = \theta^2\) and \(v(\theta) = \sec(5\theta)\).
02

Find the derivatives of \(u(\theta)\) and \(v(\theta)\)

First we find the derivative of \(u(\theta)\) with respect to \(\theta\): $$u'(\theta) = \frac{d(\theta^2)}{d\theta}= 2\theta$$ Next we find the derivative of \(v(\theta)\) with respect to \(\theta\). Using the chain rule, we have: $$v'(\theta) = \frac{d(\sec(5\theta))}{d\theta} = \sec(5\theta)\tan(5\theta)\cdot\frac{d(5\theta)}{d\theta} = 5\sec(5\theta)\tan(5\theta)$$
03

Apply the product rule

Now, we'll use the product rule to find the derivative of the given function \(y = \theta^2\sec(5\theta)\). The product rule states that: $$\frac{d(u(\theta) \cdot v(\theta))}{d\theta} = u(\theta)v'(\theta)+u'(\theta)v(\theta)$$ Applying the product rule with our function components: $$\frac{dy}{d\theta} = \theta^2 \cdot 5\sec(5\theta)\tan(5\theta) + 2\theta \cdot \sec(5\theta)$$
04

Simplify the expression

Finally, let's simplify the expression for the derivative: $$\frac{dy}{d\theta} = 5\theta^2\sec(5\theta)\tan(5\theta) + 2\theta\sec(5\theta)$$ This is our final answer for the derivative of the function \(y = \theta^2 \sec(5\theta)\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Product Rule
The product rule is a fundamental technique in calculus used when taking the derivative of a product of two functions. Imagine you have two differentiable functions, let's call them u(\theta) and v(\theta). The product rule states that the derivative of their product is given by u'(\theta)v(\theta) + u(\theta)v'(\theta).

Let's put it into a simple analogy. If you have two machines, each producing items at variable rates, the product rule helps you calculate the total rate of production at any given time by considering the output rates of both machines simultaneously. In the context of our exercise, we treated \(\theta^2\) and \(\text{sec}(5\theta)\) as separate 'machines'. We first found the derivatives of each 'machine's output' separately, and then we used the product rule to find the overall 'production rate,' which in calculus terms is the derivative of the original function.
Chain Rule
Imagine you have a set of gears, where turning one causes another to turn. That's what the chain rule is like—it's used to differentiate compositions of functions, or functions within functions.

In our example, we used the chain rule to differentiate \(\text{sec}(5\theta)\), which is a composite function since \(5\theta\) resides inside the secant function. The chain rule asserts that to find the derivative of this composite function, v'(\theta), you multiply the derivative of the outer function by the derivative of the inner function. Specifically, we derived the outer function \(\text{sec}(5\theta)\) and then multiplied it by the derivative of the inner function, \(5\theta\), giving us the final derivative of the composite function.
Trigonometric Derivatives
Derivatives of trigonometric functions are the rates at which the functions' values change. For students, this is akin to learning a new language in mathematics. The basic trigonometric functions—sine, cosine, tangent, and their reciprocals—each have specific rules for differentiation.

The derivatives for sine and cosine are particularly memorable: the derivative of sine is cosine, and the derivative of cosine is minus sine. For tangent, which is \(\text{sin}(\theta) / \text{cos}(\theta)\), the derivative turns out to be \(\text{sec}^2(\theta)\). For their reciprocals—cosecant, secant, and cotangent—the derivatives are somewhat more complex, but they follow a pattern that can be learned with practice. Understanding these rules is essential for solving any problem involving trigonometric derivatives, such as in our exercise.
Derivative of Secant Function
Now let's zero in on the secant function, which often confuses learners because it's less commonly used than sine or cosine. The secant function, \(\text{sec}(\theta)\), is the reciprocal of the cosine function. So where cosine represents the adjacent side over the hypotenuse in a right triangle, secant gives the ratio of the hypotenuse over the adjacent side.

The derivative of the secant function is \(\text{sec}(\theta)\text{tan}(\theta)\). This may seem daunting at first, but by remembering that it relates directly to the derivative of the tangent function, it becomes easier to grasp. In the exercise, when we found the derivative of \(\text{sec}(5\theta)\), we first applied the chain rule since it involved the function \(5\theta\). The result was \(5\text{sec}(5\theta)\text{tan}(5\theta)\), demonstrating the combination of the secant's derivative with the chain rule.

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Most popular questions from this chapter

Vibrations of a spring Suppose an object of mass \(m\) is attached to the end of a spring hanging from the ceiling. The mass is at its equilibrium position \(y=0\) when the mass hangs at rest. Suppose you push the mass to a position \(y_{0}\) units above its equilibrium position and release it. As the mass oscillates up and down (neglecting any friction in the system , the position y of the mass after t seconds is $$y=y_{0} \cos (t \sqrt{\frac{k}{m}})(4)$$ where \(k>0\) is a constant measuring the stiffness of the spring (the larger the value of \(k\), the stiffer the spring) and \(y\) is positive in the upward direction. Use equation (4) to answer the following questions. a. The period \(T\) is the time required by the mass to complete one oscillation. Show that \(T=2 \pi \sqrt{\frac{m}{k}}\) b. Assume \(k\) is constant and calculate \(\frac{d T}{d m}\) c. Give a physical explanation of why \(\frac{d T}{d m}\) is positive.

Earth's atmospheric pressure decreases with altitude from a sea level pressure of 1000 millibars (a unit of pressure used by meteorologists). Letting \(z\) be the height above Earth's surface (sea level) in kilometers, the atmospheric pressure is modeled by \(p(z)=1000 e^{-z / 10}\) a. Compute the pressure at the summit of Mt. Everest, which has an elevation of roughly \(10 \mathrm{km} .\) Compare the pressure on Mt. Everest to the pressure at sea level. b. Compute the average change in pressure in the first \(5 \mathrm{km}\) above Earth's surface. c. Compute the rate of change of the pressure at an elevation of \(5 \mathrm{km}\) d. Does \(p^{\prime}(z)\) increase or decrease with \(z ?\) Explain. e. What is the meaning of \(\lim _{z \rightarrow \infty} p(z)=0 ?\)

Vibrations of a spring Suppose an object of mass \(m\) is attached to the end of a spring hanging from the ceiling. The mass is at its equilibrium position \(y=0\) when the mass hangs at rest. Suppose you push the mass to a position \(y_{0}\) units above its equilibrium position and release it. As the mass oscillates up and down (neglecting any friction in the system , the position y of the mass after t seconds is $$y=y_{0} \cos (t \sqrt{\frac{k}{m}})(4)$$ where \(k>0\) is a constant measuring the stiffness of the spring (the larger the value of \(k\), the stiffer the spring) and \(y\) is positive in the upward direction. A mechanical oscillator (such as a mass on a spring or a pendulum) subject to frictional forces satisfies the equation (called a differential equation) $$y^{\prime \prime}(t)+2 y^{\prime}(t)+5 y(t)=0$$ where \(y\) is the displacement of the oscillator from its equilibrium position. Verify by substitution that the function \(y(t)=e^{-t}(\sin 2 t-2 \cos 2 t)\) satisfies this equation.

The following equations implicitly define one or more functions. a. Find \(\frac{d y}{d x}\) using implicit differentiation. b. Solve the given equation for \(y\) to identify the implicitly defined functions \(y=f_{1}(x), y=f_{2}(x), \ldots.\) c. Use the functions found in part (b) to graph the given equation. \(y^{3}=a x^{2}\) (Neile's semicubical parabola)

The hands of the clock in the tower of the Houses of Parliament in London are approximately \(3 \mathrm{m}\) and \(2.5 \mathrm{m}\) in length. How fast is the distance between the tips of the hands changing at \(9.00 ?\) (Hint: Use the Law of Cosines.)

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