Basic Trig Integrals - Calculus 1

  1. Evaluate ∫cos⁡(x)sec⁡2(sin⁡x)dx\int \cos(x) \sec^2(\sin x) dx.
    Answer: tan⁡(sin⁡x)+C\tan(\sin x) + C When you encounter an integral with a composite function structure like this, substitution is your go-to technique. The key insight is recognizing that cos⁡(x)\cos(x) is the derivative of sin⁡(x)\sin(x), which appears inside the sec⁡2\sec^2 function. Let's use substitution with u=sin⁡(x)u = \sin(x), so du=cos⁡(x)dxdu = \cos(x)dx. This transforms our integral into: ∫sec⁡2(u)du\int \sec^2(u) du Since the antiderivative of sec⁡2(u)\sec^2(u) is tan⁡(u)\tan(u), we get: tan⁡(u)+C=tan⁡(sin⁡x)+C\tan(u) + C = \tan(\sin x) + C This confirms that D) tan⁡(sin⁡x)+C\tan(\sin x) + C is correct. Now let's examine why the other options fail. Option A) sin⁡(x)tan⁡(sin⁡x)+C\sin(x)\tan(\sin x) + C would result from incorrectly applying the product rule during integration, but that's not how antiderivatives work. Option B) tan⁡(cos⁡x)+C\tan(\cos x) + C confuses the inner function—it would require −sin⁡(x)dx-\sin(x)dx in the original integral, not cos⁡(x)dx\cos(x)dx. Option C) sec⁡(sin⁡x)+C\sec(\sin x) + C mistakes the antiderivative of sec⁡2(u)\sec^2(u), which is tan⁡(u)\tan(u), not sec⁡(u)\sec(u). Study tip: When you see cos⁡(x)\cos(x) multiplied by a function of sin⁡(x)\sin(x), immediately consider u=sin⁡(x)u = \sin(x) substitution. Similarly, watch for sin⁡(x)\sin(x) with functions of cos⁡(x)\cos(x) (use u=cos⁡(x)u = \cos(x)). Memorize that ∫sec⁡2(u)du=tan⁡(u)+C\int \sec^2(u)du = \tan(u) + C—this is a fundamental antiderivative that appears frequently in calculus problems.
  2. Evaluate ∫0πxsin⁡(x2) dx\int_{0}^{\sqrt{\pi}} x \sin(x^2) \,dx
    Answer: 11 When you encounter an integral like this where the integrand contains a function and its derivative (or a multiple of it), think substitution. The key insight here is recognizing that xx is closely related to the derivative of x2x^2. Let's use the substitution u=x2u = x^2. Then du=2x dxdu = 2x \, dx, which means x dx=12dux \, dx = \frac{1}{2} du. We also need to change our limits of integration. When x=0x = 0, we have u=02=0u = 0^2 = 0. When x=πx = \sqrt{\pi}, we have u=(π)2=πu = (\sqrt{\pi})^2 = \pi. Substituting everything: ∫0πxsin⁡(x2) dx=∫0πsin⁡(u)⋅12 du=12∫0πsin⁡(u) du\int_{0}^{\sqrt{\pi}} x \sin(x^2) \,dx = \int_{0}^{\pi} \sin(u) \cdot \frac{1}{2} \,du = \frac{1}{2} \int_{0}^{\pi} \sin(u) \,du Now we can integrate: 12∫0πsin⁡(u) du=12[−cos⁡(u)]0π=12[−cos⁡(π)−(−cos⁡(0))]=12[−(−1)+1]=12[2]=1\frac{1}{2} \int_{0}^{\pi} \sin(u) \,du = \frac{1}{2}[-\cos(u)]_{0}^{\pi} = \frac{1}{2}[-\cos(\pi) - (-\cos(0))] = \frac{1}{2}[-(-1) + 1] = \frac{1}{2}[2] = 1 So the answer is B) 1. Choice A) 2 would result from forgetting the 12\frac{1}{2} factor from the substitution. Choice C) −1-1 comes from sign errors when evaluating −cos⁡(π)+cos⁡(0)-\cos(\pi) + \cos(0). Choice D) 12\frac{1}{2} would occur if you incorrectly computed −cos⁡(π)+cos⁡(0)=1-\cos(\pi) + \cos(0) = 1 instead of 2. Strategy tip: When you see xsin⁡(x2),xcos⁡(x2)x \sin(x^2),x \cos(x^2), or similar patterns, immediately consider uu-substitution with uu equal to the "inside" function.
  3. A particle's velocity is given by v(t)=sec⁡(t)tan⁡(t)v(t) = \sec(t)\tan(t). If its position at t=0t=0 is s(0)=5s(0)=5, what is its position at t=π/4t=\pi/4?
    Answer: 4+24 + \sqrt{2} Position s(t)s(t) is the antiderivative of velocity v(t)v(t). So, s(t)=∫sec⁡(t)tan⁡(t)dt=sec⁡(t)+Cs(t) = \int \sec(t)\tan(t) dt = \sec(t) + C. We use the initial condition s(0)=5s(0)=5 to find the constant CC. s(0)=sec⁡(0)+C=1+Cs(0) = \sec(0) + C = 1 + C. Setting this equal to 5 gives 1+C=51+C=5, so C=4C=4. The position function is s(t)=sec⁡(t)+4s(t) = \sec(t) + 4. Evaluating at t=π/4t=\pi/4 gives s(π/4)=sec⁡(π/4)+4=2+4s(\pi/4) = \sec(\pi/4) + 4 = \sqrt{2} + 4.
  4. Find the indefinite integral ∫csc⁡2(x)1+cot⁡(x) dx\int \frac{\csc^2(x)}{1 + \cot(x)} \,dx
    Answer: −ln⁡∣1+cot⁡(x)∣+C- \ln|1 + \cot(x)| + C When you encounter an integral with trigonometric functions like csc⁡2(x)\csc^2(x) and cot⁡(x)\cot(x), look for substitution opportunities. The key insight here is recognizing that the derivative of cot⁡(x)\cot(x) is −csc⁡2(x)-\csc^2(x). Let's use substitution with u=1+cot⁡(x)u = 1 + \cot(x). Then du=−csc⁡2(x) dxdu = -\csc^2(x) \, dx, which means csc⁡2(x) dx=−du\csc^2(x) \, dx = -du. Substituting into our integral: ∫csc⁡2(x)1+cot⁡(x) dx=∫1u⋅(−du)=−∫1u du=−ln⁡∣u∣+C\int \frac{\csc^2(x)}{1 + \cot(x)} \,dx = \int \frac{1}{u} \cdot (-du) = -\int \frac{1}{u} \,du = -\ln|u| + C Substituting back: −ln⁡∣1+cot⁡(x)∣+C-\ln|1 + \cot(x)| + C This confirms answer C is correct. Let's examine why the other options fail: A suggests −11+cot⁡(x)+C\frac{-1}{1 + \cot(x)} + C. If you differentiate this, you get csc⁡2(x)(1+cot⁡(x))2\frac{\csc^2(x)}{(1 + \cot(x))^2}, which doesn't match our integrand. B gives ln⁡∣1+cot⁡(x)∣+C\ln|1 + \cot(x)| + C. This is missing the negative sign that comes from our substitution du=−csc⁡2(x) dxdu = -\csc^2(x) \, dx. D presents an unnecessarily complex expression that doesn't relate to the standard antiderivative forms we expect from this substitution. Study tip: When you see csc⁡2(x)\csc^2(x) in an integral, immediately think about cot⁡(x)\cot(x) since ddx[cot⁡(x)]=−csc⁡2(x)\frac{d}{dx}[\cot(x)] = -\csc^2(x). This derivative relationship is your gateway to effective substitution in trigonometric integrals.
  5. Evaluate ∫−π/3π/3(sin⁡(x)+sec⁡2(x))dx\int_{-\pi/3}^{\pi/3} (\sin(x) + \sec^2(x)) dx.
    Answer: 232\sqrt{3} We can split the integral into two parts: ∫−π/3π/3sin⁡(x)dx+∫−π/3π/3sec⁡2(x)dx\int_{-\pi/3}^{\pi/3} \sin(x) dx + \int_{-\pi/3}^{\pi/3} \sec^2(x) dx. Since sin⁡(x)\sin(x) is an odd function and it is being integrated over a symmetric interval [−a,a][-a, a], the value of the first integral is 0. The function sec⁡2(x)\sec^2(x) is an even function, so ∫−π/3π/3sec⁡2(x)dx=2∫0π/3sec⁡2(x)dx\int_{-\pi/3}^{\pi/3} \sec^2(x) dx = 2 \int_0^{\pi/3} \sec^2(x) dx. This evaluates to 2[tan⁡(x)]0π/3=2(tan⁡(π/3)−tan⁡(0))=2(3−0)=232[\tan(x)]_0^{\pi/3} = 2(\tan(\pi/3) - \tan(0)) = 2(\sqrt{3} - 0) = 2\sqrt{3}. The total value is 0+23=230 + 2\sqrt{3} = 2\sqrt{3}.
  6. What is the value of the definite integral ∫03π/2∣cos⁡(x)∣ dx\int_{0}^{3\pi/2} |\cos(x)| \,dx?
    Answer: 33 The function ∣cos⁡(x)∣|\cos(x)| is the absolute value of cos⁡(x)\cos(x). We must split the integral based on the intervals where cos⁡(x)\cos(x) is positive or negative. In the interval [0,3π/2][0, 3\pi/2], cos⁡(x)≥0\cos(x) \ge 0 for x∈[0,π/2]x \in [0, \pi/2] and cos⁡(x)≤0\cos(x) \le 0 for x∈[π/2,3π/2]x \in [\pi/2, 3\pi/2]. So, we split the integral: ∫03π/2∣cos⁡(x)∣ dx=∫0π/2cos⁡(x) dx+∫π/23π/2−cos⁡(x) dx\int_{0}^{3\pi/2} |\cos(x)| \,dx = \int_{0}^{\pi/2} \cos(x) \,dx + \int_{\pi/2}^{3\pi/2} -\cos(x) \,dx Evaluate each part: ∫0π/2cos⁡(x) dx=[sin⁡(x)]0π/2=sin⁡(π/2)−sin⁡(0)=1−0=1\int_{0}^{\pi/2} \cos(x) \,dx = [\sin(x)]_{0}^{\pi/2} = \sin(\pi/2) - \sin(0) = 1 - 0 = 1 ∫π/23π/2−cos⁡(x) dx=−[sin⁡(x)]π/23π/2=−(sin⁡(3π/2)−sin⁡(π/2))=−(−1−1)=−(−2)=2\int_{\pi/2}^{3\pi/2} -\cos(x) \,dx = -[\sin(x)]_{\pi/2}^{3\pi/2} = -(\sin(3\pi/2) - \sin(\pi/2)) = -(-1 - 1) = -(-2) = 2 The total value is the sum of the parts: 1+2=31 + 2 = 3. Distractor B is the result of integrating cos⁡(x)\cos(x) without the absolute value. Distractor C is the area of only the first positive section. Distractor D is the area from 00 to π\pi.
  7. Evaluate ∫sin⁡(2x)sin⁡(x)dx\int \frac{\sin(2x)}{\sin(x)} dx.
    Answer: 2sin⁡(x)+C2\sin(x) + C This problem requires using the double-angle identity for sine, sin⁡(2x)=2sin⁡(x)cos⁡(x)\sin(2x) = 2\sin(x)\cos(x). Substituting this into the integrand gives ∫2sin⁡(x)cos⁡(x)sin⁡(x)dx\int \frac{2\sin(x)\cos(x)}{\sin(x)} dx. For sin⁡(x)≠0\sin(x) \neq 0, this simplifies to ∫2cos⁡(x)dx\int 2\cos(x) dx. The antiderivative is 2sin⁡(x)+C2\sin(x) + C.
  8. Evaluate ∫0π/4dxcos⁡2(x)\int_0^{\pi/4} \frac{dx}{\cos^2(x)}.
    Answer: 1 The integrand 1cos⁡2(x)\frac{1}{\cos^2(x)} is equivalent to sec⁡2(x)\sec^2(x). The problem is to evaluate ∫0π/4sec⁡2(x)dx\int_0^{\pi/4} \sec^2(x) dx. The antiderivative of sec⁡2(x)\sec^2(x) is tan⁡(x)\tan(x). Evaluating the definite integral gives [tan⁡(x)]0π/4=tan⁡(π/4)−tan⁡(0)=1−0=1[\tan(x)]_0^{\pi/4} = \tan(\pi/4) - \tan(0) = 1 - 0 = 1.
  9. Evaluate ∫π/4π/2csc⁡(x)cot⁡(x)dx\int_{\pi/4}^{\pi/2} \csc(x)\cot(x) dx.
    Answer: 2−1\sqrt{2}-1 The antiderivative of csc⁡(x)cot⁡(x)\csc(x)\cot(x) is −csc⁡(x)-\csc(x). Evaluating the definite integral gives [−csc⁡(x)]π/4π/2=−csc⁡(π/2)−(−csc⁡(π/4))[-\csc(x)]_{\pi/4}^{\pi/2} = -\csc(\pi/2) - (-\csc(\pi/4)). Since csc⁡(π/2)=1\csc(\pi/2) = 1 and csc⁡(π/4)=2\csc(\pi/4) = \sqrt{2}, the result is −1−(−2))=2−1-1 - (-\sqrt{2})) = \sqrt{2}-1.
  10. What is the average value of the function f(x)=sec⁡2(x)f(x) = \sec^2(x) on the interval [0,π/4][0, \pi/4]?
    Answer: 4π\frac{4}{\pi} The average value of a function f(x)f(x) on an interval [a,b][a, b] is given by 1b−a∫abf(x)dx\frac{1}{b-a} \int_a^b f(x) dx. Here, a=0a=0 and b=π/4b=\pi/4. The average value is 1π/4−0∫0π/4sec⁡2(x)dx=4π∫0π/4sec⁡2(x)dx\frac{1}{\pi/4 - 0} \int_0^{\pi/4} \sec^2(x) dx = \frac{4}{\pi} \int_0^{\pi/4} \sec^2(x) dx. The antiderivative of sec⁡2(x)\sec^2(x) is tan⁡(x)\tan(x). So, we have 4π[tan⁡(x)]0π/4=4π(tan⁡(π/4)−tan⁡(0))=4π(1−0)=4π\frac{4}{\pi} [\tan(x)]_0^{\pi/4} = \frac{4}{\pi}(\tan(\pi/4) - \tan(0)) = \frac{4}{\pi}(1-0) = \frac{4}{\pi}.
  11. Let F(x)=∫xπ/4sec⁡2(t) dtF(x) = \int_{x}^{\pi/4} \sec^2(t) \,dt. What is the value of F′(π/4)F'(\pi/4)?
    Answer: −2-2 When you see a derivative of an integral where the variable appears in the limits of integration, you need the Fundamental Theorem of Calculus Part I combined with the chain rule. For F(x)=∫xπ/4sec⁡2(t) dtF(x) = \int_{x}^{\pi/4} \sec^2(t) \,dt, notice that the variable xx appears in the lower limit. The general rule states that if G(x)=∫a(x)b(x)f(t) dtG(x) = \int_{a(x)}^{b(x)} f(t) \,dt, then G′(x)=f(b(x))⋅b′(x)−f(a(x))⋅a′(x)G'(x) = f(b(x)) \cdot b'(x) - f(a(x)) \cdot a'(x). In our case, a(x)=xa(x) = x, b(x)=π/4b(x) = \pi/4, and f(t)=sec⁡2(t)f(t) = \sec^2(t). Since a′(x)=1a'(x) = 1 and b′(x)=0b'(x) = 0 (constant), we get: F′(x)=sec⁡2(π/4)⋅0−sec⁡2(x)⋅1=−sec⁡2(x)F'(x) = \sec^2(\pi/4) \cdot 0 - \sec^2(x) \cdot 1 = -\sec^2(x) Therefore, F′(π/4)=−sec⁡2(π/4)=−(2)2=−2F'(\pi/4) = -\sec^2(\pi/4) = -(\sqrt{2})^2 = -2, confirming answer D. Let's examine why the other options are wrong: A) −1-1 likely comes from forgetting that sec⁡(π/4)=2\sec(\pi/4) = \sqrt{2}, not 1. B) 22 results from dropping the negative sign that comes from having xx in the lower limit. C) 00 might stem from incorrectly thinking the derivative is zero because one limit is constant. Key strategy: When the variable is in the lower limit of integration, there's always a negative sign in front. Remember that sec⁡(π/4)=2\sec(\pi/4) = \sqrt{2}, so sec⁡2(π/4)=2\sec^2(\pi/4) = 2. Practice recognizing when to apply the Fundamental Theorem versus basic antiderivative rules.
  12. The acceleration of a particle is a(t)=−sin⁡(t)a(t) = -\sin(t). If the particle's initial velocity is v(0)=1v(0)=1 and initial position is s(0)=3s(0)=3, what is its position at t=πt=\pi?
    Answer: 3 First, find the velocity function v(t)v(t) by integrating the acceleration function a(t)a(t): v(t)=∫−sin⁡(t)dt=cos⁡(t)+C1v(t) = \int -\sin(t) dt = \cos(t) + C_1. Use the initial velocity v(0)=1v(0)=1 to find C1C_1: 1=cos⁡(0)+C1  ⟹  1=1+C1  ⟹  C1=01 = \cos(0) + C_1 \implies 1 = 1 + C_1 \implies C_1 = 0. So, v(t)=cos⁡(t)v(t) = \cos(t). Next, find the position function s(t)s(t) by integrating the velocity function v(t)v(t): s(t)=∫cos⁡(t)dt=sin⁡(t)+C2s(t) = \int \cos(t) dt = \sin(t) + C_2. Use the initial position s(0)=3s(0)=3 to find C2C_2: 3=sin⁡(0)+C2  ⟹  3=0+C2  ⟹  C2=33 = \sin(0) + C_2 \implies 3 = 0 + C_2 \implies C_2 = 3. So, s(t)=sin⁡(t)+3s(t) = \sin(t) + 3. Finally, evaluate the position at t=πt=\pi: s(π)=sin⁡(π)+3=0+3=3s(\pi) = \sin(\pi) + 3 = 0 + 3 = 3.
  13. What is the average value of the function f(x)=sin⁡(x)f(x) = \sin(x) on the closed interval [0,π][0, \pi]?
    Answer: 2/π2/\pi When you encounter a question about the average value of a function, you're working with the Mean Value Theorem for Integrals. The average value of a continuous function f(x)f(x) over an interval [a,b][a,b] is given by the formula: Average value=1b−a∫abf(x) dx\text{Average value} = \frac{1}{b-a}\int_a^b f(x)\,dx For f(x)=sin⁡(x)f(x) = \sin(x) on [0,π][0,\pi], we need to calculate: 1π−0∫0πsin⁡(x) dx=1π∫0πsin⁡(x) dx\frac{1}{\pi-0}\int_0^\pi \sin(x)\,dx = \frac{1}{\pi}\int_0^\pi \sin(x)\,dx The antiderivative of sin⁡(x)\sin(x) is −cos⁡(x)-\cos(x), so: 1π[−cos⁡(x)]0π=1π[−cos⁡(π)−(−cos⁡(0))]=1π[−(−1)+1]=2π\frac{1}{\pi}[-\cos(x)]_0^\pi = \frac{1}{\pi}[-\cos(\pi) - (-\cos(0))] = \frac{1}{\pi}[-(-1) + 1] = \frac{2}{\pi} This confirms answer choice D is correct. Looking at the wrong answers: A) −2/π-2/\pi results from a sign error when evaluating the antiderivative—forgetting that −cos⁡(π)=−(−1)=1-\cos(\pi) = -(-1) = 1, not −1-1. B) 22 comes from correctly finding the numerator (2) but forgetting to divide by π\pi. C) 00 might seem tempting because sin⁡(x)\sin(x) has both positive and negative values over many intervals, but on [0,π][0,\pi], sine is entirely non-negative. Remember: the average value formula always requires both the definite integral AND division by the interval length. Also, visualize the function—sin⁡(x)\sin(x) forms a complete "hump" above the x-axis from 0 to π\pi, so the average should be positive and reasonable in magnitude.
  14. A function is defined by f(x)=∫xπ/4sec⁡(t)tan⁡(t)dtf(x) = \int_x^{\pi/4} \sec(t)\tan(t) dt. What is the value of f(0)f(0)?
    Answer: 2−1\sqrt{2}-1 When you encounter a definite integral that defines a function, you need to use the Fundamental Theorem of Calculus to evaluate it. Here, f(x)=∫xπ/4sec⁡(t)tan⁡(t)dtf(x) = \int_x^{\pi/4} \sec(t)\tan(t) dt, so you're looking for f(0)=∫0π/4sec⁡(t)tan⁡(t)dtf(0) = \int_0^{\pi/4} \sec(t)\tan(t) dt. To evaluate this integral, recognize that sec⁡(t)tan⁡(t)\sec(t)\tan(t) is the derivative of sec⁡(t)\sec(t). You can verify this: ddt[sec⁡(t)]=sec⁡(t)tan⁡(t)\frac{d}{dt}[\sec(t)] = \sec(t)\tan(t). Therefore: ∫0π/4sec⁡(t)tan⁡(t)dt=sec⁡(t)∣0π/4=sec⁡(π/4)−sec⁡(0)\int_0^{\pi/4} \sec(t)\tan(t) dt = \sec(t)\Big|_0^{\pi/4} = \sec(\pi/4) - \sec(0) Since sec⁡(π/4)=1cos⁡(π/4)=12/2=2\sec(\pi/4) = \frac{1}{\cos(\pi/4)} = \frac{1}{\sqrt{2}/2} = \sqrt{2} and sec⁡(0)=1cos⁡(0)=1\sec(0) = \frac{1}{\cos(0)} = 1: f(0)=2−1f(0) = \sqrt{2} - 1 Looking at the wrong answers: Choice A gives -1, which would result from incorrectly computing sec⁡(0)−sec⁡(π/4)\sec(0) - \sec(\pi/4) (reversing the order). Choice B gives 1−21 - \sqrt{2}, which happens if you mistakenly use sec⁡(0)−sec⁡(π/4)\sec(0) - \sec(\pi/4) instead of the correct order. Choice C gives 1, which occurs if you forget to subtract sec⁡(0)\sec(0) entirely and only use sec⁡(π/4)−1\sec(\pi/4) - 1 incorrectly. Study tip: When evaluating definite integrals, always remember that the Fundamental Theorem gives you F(b)−F(a)F(b) - F(a) for ∫abf(t)dt\int_a^b f(t) dt, where the upper limit comes first. Also, memorize that ddt[sec⁡(t)]=sec⁡(t)tan⁡(t)\frac{d}{dt}[\sec(t)] = \sec(t)\tan(t) — it's a frequently tested derivative-antiderivative pair.
  15. Which of the following definite integrals has a value of 0?
    Answer: ∫0πcos⁡(x)dx\int_0^{\pi} \cos(x) dx We evaluate each integral: A) ∫0πsin⁡(x)dx=[−cos⁡(x)]0π=−(−1)−(−1)=2\int_0^{\pi} \sin(x) dx = [-\cos(x)]_0^{\pi} = -(-1) - (-1) = 2. B) ∫0πcos⁡(x)dx=[sin⁡(x)]0π=sin⁡(π)−sin⁡(0)=0−0=0\int_0^{\pi} \cos(x) dx = [\sin(x)]_0^{\pi} = \sin(\pi) - \sin(0) = 0 - 0 = 0. C) ∫−π/4π/4sec⁡2(x)dx=[tan⁡(x)]−π/4π/4=1−(−1)=2\int_{-\pi/4}^{\pi/4} \sec^2(x) dx = [\tan(x)]_{-\pi/4}^{\pi/4} = 1 - (-1) = 2. D) ∫0π/2sin⁡(x)dx=[−cos⁡(x)]0π/2=0−(−1)=1\int_0^{\pi/2} \sin(x) dx = [-\cos(x)]_0^{\pi/2} = 0 - (-1) = 1. The only integral that evaluates to 0 is B.
  16. If F(x)=∫π/4x2sec⁡2(t)dtF(x) = \int_{\pi/4}^{x^2} \sec^2(t) dt, what is F′(π/3)F'(\sqrt{\pi/3})?
    Answer: 8π38\sqrt{\frac{\pi}{3}} By the Fundamental Theorem of Calculus Part 1, combined with the Chain Rule, if F(x)=∫ag(x)f(t)dtF(x) = \int_a^{g(x)} f(t) dt, then F′(x)=f(g(x))⋅g′(x)F'(x) = f(g(x)) \cdot g'(x). Here, f(t)=sec⁡2(t)f(t) = \sec^2(t) and g(x)=x2g(x) = x^2, so g′(x)=2xg'(x) = 2x. Therefore, F′(x)=sec⁡2(x2)⋅2xF'(x) = \sec^2(x^2) \cdot 2x. We need to evaluate this at x=π/3x = \sqrt{\pi/3}. F′(π/3)=sec⁡2((π/3)2)⋅2π/3=sec⁡2(π/3)⋅2π/3F'(\sqrt{\pi/3}) = \sec^2((\sqrt{\pi/3})^2) \cdot 2\sqrt{\pi/3} = \sec^2(\pi/3) \cdot 2\sqrt{\pi/3}. Since cos⁡(π/3)=1/2\cos(\pi/3) = 1/2, sec⁡(π/3)=2\sec(\pi/3) = 2, and sec⁡2(π/3)=4\sec^2(\pi/3) = 4. The result is 4⋅2π/3=8π34 \cdot 2\sqrt{\pi/3} = 8\sqrt{\frac{\pi}{3}}.
  17. If ∫π/2ccos⁡(x)dx=−1\int_{\pi/2}^c \cos(x) dx = -1 and c>π/2c > \pi/2, which of the following could be a value for cc?
    Answer: π\pi First, evaluate the integral in terms of cc: ∫π/2ccos⁡(x)dx=[sin⁡(x)]π/2c=sin⁡(c)−sin⁡(π/2)=sin⁡(c)−1\int_{\pi/2}^c \cos(x) dx = [\sin(x)]_{\pi/2}^c = \sin(c) - \sin(\pi/2) = \sin(c) - 1. We are given that this equals -1, so sin⁡(c)−1=−1\sin(c) - 1 = -1, which implies sin⁡(c)=0\sin(c) = 0. Among the answer choices with c>π/2c > \pi/2, we need sin⁡(c)=0\sin(c) = 0. Checking: sin⁡(π)=0\sin(\pi) = 0. Verification: ∫π/2πcos⁡(x)dx=[sin⁡(x)]π/2π=sin⁡(π)−sin⁡(π/2)=0−1=−1\int_{\pi/2}^\pi \cos(x)dx = [\sin(x)]_{\pi/2}^\pi = \sin(\pi) - \sin(\pi/2) = 0 - 1 = -1. ✓
  18. What is the value of ∫02π∣sin⁡(x)∣dx\int_0^{2\pi} |\sin(x)| dx in terms of A?
    Answer: 4A First, let's find the value of A: A=∫0π/2sin⁡(x)dx=[−cos⁡(x)]0π/2=−cos⁡(π/2)−(−cos⁡(0))=0−(−1)=1A = \int_0^{\pi/2} \sin(x) dx = [-\cos(x)]_0^{\pi/2} = -\cos(\pi/2) - (-\cos(0)) = 0 - (-1) = 1. The integral ∫02π∣sin⁡(x)∣dx\int_0^{2\pi} |\sin(x)| dx represents the area under two full arches of the sine curve. The area of one arch is ∫0πsin⁡(x)dx=[−cos⁡(x)]0π=−(−1)−(−1)=2\int_0^\pi \sin(x) dx = [-\cos(x)]_0^\pi = -(-1) - (-1) = 2. Since there are two identical arches between 0 and 2π2\pi, the total area is 2×2=42 \times 2 = 4. Since A=1A=1, the value of the integral is 4A4A.
  19. What is the value of ∫π/4π/3(1+cot⁡2(x))dx\int_{\pi/4}^{\pi/3} (1+\cot^2(x)) dx?
    Answer: 1−331 - \frac{\sqrt{3}}{3} First, use the Pythagorean identity 1+cot⁡2(x)=csc⁡2(x)1+\cot^2(x) = \csc^2(x). The integral simplifies to ∫π/4π/3csc⁡2(x)dx\int_{\pi/4}^{\pi/3} \csc^2(x) dx. The antiderivative of csc⁡2(x)\csc^2(x) is −cot⁡(x)-\cot(x). Now, evaluate the definite integral: [−cot⁡(x)]π/4π/3=−cot⁡(π/3)−(−cot⁡(π/4))=−13−(−1)=1−13=1−33[-\cot(x)]_{\pi/4}^{\pi/3} = -\cot(\pi/3) - (-\cot(\pi/4)) = -\frac{1}{\sqrt{3}} - (-1) = 1 - \frac{1}{\sqrt{3}} = 1 - \frac{\sqrt{3}}{3}.
  20. Which of the following is an antiderivative of f(θ)=2tan⁡2(θ)f(\theta) = 2\tan^2(\theta)?
    Answer: 2tan⁡(θ)−2θ+C2\tan(\theta) - 2\theta + C To find the integral of 2tan⁡2(θ)2\tan^2(\theta), we first use the Pythagorean identity tan⁡2(θ)=sec⁡2(θ)−1\tan^2(\theta) = \sec^2(\theta) - 1. So, the integral becomes: ∫2tan⁡2(θ) dθ=∫2(sec⁡2(θ)−1) dθ=∫(2sec⁡2(θ)−2) dθ\int 2\tan^2(\theta) \,d\theta = \int 2(\sec^2(\theta) - 1) \,d\theta = \int (2\sec^2(\theta) - 2) \,d\theta We can integrate term by term. The integral of 2sec⁡2(θ)2\sec^2(\theta) is 2tan⁡(θ)2\tan(\theta), and the integral of 22 is 2θ2\theta. Therefore, the antiderivative is 2tan⁡(θ)−2θ+C2\tan(\theta) - 2\theta + C. Distractor B arises from incorrectly applying the power rule to a trigonometric function. Distractor C results from forgetting to integrate the −1-1 term from the identity. Distractor D is the derivative of the original function's rewritten form, not its antiderivative.

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