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Solving g'(x) = 2 for tan(x) on an interval

Let g(x)=tan⁡(x)g(x) = \tan(x).

Find all points xx in the interval [0,2π)[0, 2\pi) where g′(x)=2g'(x) = 2. Express your answer(s) in terms of arctan⁡\arctan, and also identify which solutions are related by the periodicity of tan⁡(x)\tan(x).

Hint

First differentiate g(x)=tan⁡(x)g(x) = \tan(x) using the trigonometric derivative rule. Then set the derivative equal to 2 and solve for xx. Since tan⁡(x)\tan(x) has period π\pi, solutions will be spaced π\pi apart. Remember that sec⁡2(x)=2\sec^2(x) = 2 depends only on cos⁡2(x)\cos^2(x), which yields multiple solutions in the given interval.

Step-by-step solution

The derivative of tan⁡(x)\tan(x) is g′(x)=sec⁡2(x)g'(x) = \sec^2(x), one of the six memorized trigonometric derivative rules. Setting this equal to 2 gives the equation sec⁡2(x)=2\sec^2(x) = 2 that must be solved for xx in [0,2π)[0, 2\pi).

Since sec⁡2(x)=2\sec^2(x) = 2, we have cos⁡2(x)=1/2\cos^2(x) = 1/2. Using the identity sec⁡2(x)=1+tan⁡2(x)\sec^2(x) = 1 + \tan^2(x), we get tan⁡2(x)=1\tan^2(x) = 1, so tan⁡(x)=±1\tan(x) = \pm 1. Since sec⁡2(x)\sec^2(x) depends only on cos⁡2(x)\cos^2(x), the equation sec⁡2(x)=2\sec^2(x) = 2 is satisfied whenever cos⁡(x)=±1/2\cos(x) = \pm 1/\sqrt{2}, giving four candidate angles: x=π/4,3π/4,5π/4,7π/4x = \pi/4, 3\pi/4, 5\pi/4, 7\pi/4.

We can verify these are related by periodicity: when tan⁡(x)=1\tan(x) = 1, the principal solution in [0,2π)[0, 2\pi) is x=arctan⁡(1)=π/4x = \arctan(1) = \pi/4, and the next solution (shifted by the period π\pi) is x=π/4+π=5π/4x = \pi/4 + \pi = 5\pi/4. When tan⁡(x)=−1\tan(x) = -1, the principal solution is x=π+arctan⁡(−1)=3π/4x = \pi + \arctan(-1) = 3\pi/4, and the next solution is x=3π/4+π=7π/4x = 3\pi/4 + \pi = 7\pi/4.

Thus, on [0,2π)[0, 2\pi), the four solutions where g′(x)=2g'(x) = 2 are x=π/4,3π/4,5π/4,7π/4x = \pi/4, 3\pi/4, 5\pi/4, 7\pi/4. In terms of arctan⁡\arctan, these can be expressed as x=arctan⁡(1)x = \arctan(1) and x=arctan⁡(1)+πx = \arctan(1) + \pi (the two solutions where tan⁡(x)=1\tan(x) = 1), and x=π+arctan⁡(−1)x = \pi + \arctan(-1) and x=π+arctan⁡(−1)+πx = \pi + \arctan(-1) + \pi (the two solutions where tan⁡(x)=−1\tan(x) = -1).

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