Math 130 Test 2 Review Problems

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Comprehensive practice flashcards reviewing trigonometric transformations, unit circle coordinates, inverse trigonometric functions, and triangle applications from the Math 130 Test 2 Review Problems.

Last updated 3:36 AM on 10/8/26
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45 Terms

1
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Terminal Point for −t-t

For an angle tt with terminal point (56,116)(\frac{5}{6}, \frac{\sqrt{11}}{6}) on the unit circle, the angle −t-t reflects across the x-axis to give coordinates (56,−116)(\frac{5}{6}, -\frac{\sqrt{11}}{6}).

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Terminal Point for 4π+t4\pi + t

For an angle tt with terminal point (56,116)(\frac{5}{6}, \frac{\sqrt{11}}{6}), adding 4π4\pi corresponds to two complete revolutions around the unit circle, keeping the coordinates identical at (56,116)(\frac{5}{6}, \frac{\sqrt{11}}{6}).

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Terminal Point for π2−t\frac{\pi}{2} - t

For an angle tt with terminal point (56,116)(\frac{5}{6}, \frac{\sqrt{11}}{6}), the complementary angle π2−t\frac{\pi}{2} - t reflects coordinates across the line y=xy = x, resulting in (116,56)(\frac{\sqrt{11}}{6}, \frac{5}{6}).

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Terminal Point for t+5πt + 5\pi

For an angle tt with terminal point (56,116)(\frac{5}{6}, \frac{\sqrt{11}}{6}), adding an odd multiple of π\pi reflects the point through the origin to give coordinates (−56,−116)(-\frac{5}{6}, -\frac{\sqrt{11}}{6}).

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Terminal Point for π−t\pi - t

For an angle tt with terminal point (56,116)(\frac{5}{6}, \frac{\sqrt{11}}{6}), the angle π−t\pi - t reflects across the y-axis, yielding coordinates (−56,116)(-\frac{5}{6}, \frac{\sqrt{11}}{6}).

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Quadrant IV Unit Circle Point for x=54x = \frac{\sqrt{5}}{4}

Using the unit circle equation x2+y2=1x^2 + y^2 = 1 where y<0y < 0 in quadrant IV, the y-coordinate is y=−1−(54)2=−114y = -\sqrt{1 - (\frac{\sqrt{5}}{4})^2} = -\frac{\sqrt{11}}{4}.

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SSA Configuration (Ambiguous Case)

A triangle configuration where two side lengths and a non-included angle are known; it can produce zero, one, or two unique triangles (up to congruence) based on the number of positive solutions to the Law of Cosines.

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Amplitude and Midline of y=4sin⁡(3πt−π2)+7y = 4\sin(3\pi t - \frac{\pi}{2}) + 7

The amplitude is given by ∣A∣=4|A| = 4, and the midline is the horizontal center line determined by the vertical translation y=7y = 7.

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Period and Horizontal Shift of y=4sin⁡(3πt−π2)+7y = 4\sin(3\pi t - \frac{\pi}{2}) + 7

The period is 2π3π=23\frac{2\pi}{3\pi} = \frac{2}{3}, and factoring 3π(t−16)3\pi(t - \frac{1}{6}) gives a horizontal shift of 16\frac{1}{6} unit to the right.

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Midline and Amplitude of Graphed Function in Figure 0

For the curve oscillating between maximum 22 and minimum −6-6, the midline is y=2+(−6)2=−2y = \frac{2 + (-6)}{2} = -2 and the amplitude is 2−(−6)2=4\frac{2 - (-6)}{2} = 4.

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<p>Period and Formula of Graphed Function in Figure 0</p>

Period and Formula of Graphed Function in Figure 0

The horizontal distance between consecutive crests is π\pi, yielding the sinusoidal equation y=4cos⁡(2(x−π6))−2y = 4\cos(2(x - \frac{\pi}{6})) - 2 or y=4sin⁡(2x+π6)−2y = 4\sin(2x + \frac{\pi}{6}) - 2.

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Ferris Wheel Amplitude and Midline

For a ferris wheel with diameter 32 meters32\,\text{meters} boarded 1 meter1\,\text{meter} above ground, the radius (amplitude) is 16 meters16\,\text{meters} and the midline height is 1+16=17 meters1 + 16 = 17\,\text{meters}.

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Ferris Wheel Height Equation h(t)h(t)

With a period of 6 minutes6\,\text{minutes} (B=π3B = \frac{\pi}{3}) and starting halfway heading downward at t=0t = 0, the height above ground level is h(t)=−16sin⁡(π3t)+17h(t) = -16\sin(\frac{\pi}{3}t) + 17.

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Period of y=12cot⁡(π8x+π4)y = \frac{1}{2}\cot(\frac{\pi}{8}x + \frac{\pi}{4})

For the cotangent function with coefficient B=π8B = \frac{\pi}{8}, the period is πB=ππ/8=8\frac{\pi}{B} = \frac{\pi}{\pi/8} = 8.

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Vertical Asymptotes of y=12cot⁡(π8x+π4)y = \frac{1}{2}\cot(\frac{\pi}{8}x + \frac{\pi}{4})

The vertical asymptotes occur where the inner argument equals kπk\pi, yielding π8x+π4=kπ  ⟹  x=8k−2\frac{\pi}{8}x + \frac{\pi}{4} = k\pi \implies x = 8k - 2 for any integer kk.

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Period and Asymptotes of y=2sec⁡(π2x)+3y = 2\sec(\frac{\pi}{2}x) + 3

The period is 2ππ/2=4\frac{2\pi}{\pi/2} = 4, and the vertical asymptotes occur where cos⁡(π2x)=0\cos(\frac{\pi}{2}x) = 0, giving x=2k+1x = 2k + 1 for any integer kk.

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Range of y=2sec⁡(π2x)+3y = 2\sec(\frac{\pi}{2}x) + 3

Because ∣sec⁡(θ)∣≥1|\sec(\theta)| \ge 1, the output values lie above the local minimum 3+2=53 + 2 = 5 or below the local maximum 3−2=13 - 2 = 1, giving (−∞,1]∪[5,∞)(-\infty, 1] \cup [5, \infty).

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Domain and Range of f(x)=cos⁡−1(x)f(x) = \cos^{-1}(x)

The domain of the inverse cosine function is [−1,1][-1, 1] and its principal range is [0,π][0, \pi].

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Domain and Range of g(x)=sin⁡−1(x)g(x) = \sin^{-1}(x)

The domain of the inverse sine function is [−1,1][-1, 1] and its principal range is [−π2,π2][-\frac{\pi}{2}, \frac{\pi}{2}].

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Domain and Range of h(x)=tan⁡−1(x)h(x) = \tan^{-1}(x)

The domain of the inverse tangent function is all real numbers (−∞,∞)(-\infty, \infty) and its principal range is the open interval (−π2,π2)(-\frac{\pi}{2}, \frac{\pi}{2}).

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Inverse Function of g(x)=2cos⁡(3x)+5g(x) = 2\cos(3x) + 5

For 0≤x≤π30 \le x \le \frac{\pi}{3}, solving y=2cos⁡(3x)+5y = 2\cos(3x) + 5 for xx gives g−1(x)=13cos⁡−1(x−52)g^{-1}(x) = \frac{1}{3}\cos^{-1}(\frac{x - 5}{2}).

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Domain and Range of g−1(x)g^{-1}(x) for g(x)=2cos⁡(3x)+5g(x) = 2\cos(3x) + 5

The domain of g−1(x)g^{-1}(x) is the range of g(x)g(x), which is [3,7][3, 7], and the range of g−1(x)g^{-1}(x) is the restricted domain of g(x)g(x), which is [0,π3][0, \frac{\pi}{3}].

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Exact Value of sin⁡−1(−12)\sin^{-1}(-\frac{1}{2})

The unique angle in the principal range [−π2,π2][-\frac{\pi}{2}, \frac{\pi}{2}] whose sine equals −12-\frac{1}{2}, which is −π6-\frac{\pi}{6}.

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Exact Value of cos⁡−1(−22)\cos^{-1}(-\frac{\sqrt{2}}{2})

The unique angle in the principal range [0,π][0, \pi] whose cosine equals −22-\frac{\sqrt{2}}{2}, which is 3π4\frac{3\pi}{4}.

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Exact Value of tan⁡−1(0)\tan^{-1}(0)

The unique angle in the principal range (−π2,π2)(-\frac{\pi}{2}, \frac{\pi}{2}) whose tangent equals 00, which is 00.

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Angle in 0∘<ϕ<360∘0^\circ < \phi < 360^\circ with the Same Cosine as 42∘42^\circ

By reflection across the horizontal axis into quadrant IV, the angle sharing the same cosine is ϕ=360∘−42∘=318∘\phi = 360^\circ - 42^\circ = 318^\circ.

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Angle in 0∘<ϕ<360∘0^\circ < \phi < 360^\circ with the Same Sine as 42∘42^\circ

By reflection across the vertical axis into quadrant II, the angle sharing the same sine is ϕ=180∘−42∘=138∘\phi = 180^\circ - 42^\circ = 138^\circ.

28
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Evaluation of cos⁡(cos⁡−1(−0.2))\cos(\cos^{-1}(-0.2))

Evaluates to −0.2-0.2 (True) because the identity cos⁡(cos⁡−1(x))=x\cos(\cos^{-1}(x)) = x holds for all values in the domain [−1,1][-1, 1].

29
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Evaluation of cos⁡(cos⁡−1(1.6))\cos(\cos^{-1}(1.6))

Undefined (False) because the input 1.61.6 lies outside the domain [−1,1][-1, 1] of cos⁡−1(x)\cos^{-1}(x).

30
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Evaluation of sin⁡−1(sin⁡(3))\sin^{-1}(\sin(3))

Evaluates to π−3\pi - 3 (False that it equals 33) because 3 radians3\,\text{radians} exceeds the principal interval [−π2,π2][-\frac{\pi}{2}, \frac{\pi}{2}], while sin⁡(π−3)=sin⁡(3)\sin(\pi - 3) = \sin(3).

31
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Evaluation of sin⁡−1(sin⁡(−π10))\sin^{-1}(\sin(-\frac{\pi}{10}))

Evaluates to −π10-\frac{\pi}{10} (True) because the angle −π10-\frac{\pi}{10} lies strictly inside the principal interval [−π2,π2][-\frac{\pi}{2}, \frac{\pi}{2}].

32
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Evaluation of tan⁡(tan⁡−1(14))\tan(\tan^{-1}(14))

Evaluates to 1414 (True) because the identity tan⁡(tan⁡−1(x))=x\tan(\tan^{-1}(x)) = x holds for all real numbers in the domain (−∞,∞)(-\infty, \infty).

33
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Value of tan⁡(cos⁡−1(−45))\tan(\cos^{-1}(-\frac{4}{5}))

For θ=cos⁡−1(−45)\theta = \cos^{-1}(-\frac{4}{5}) in quadrant II, the adjacent side is −4-4, hypotenuse is 55, and opposite side is 33, giving tan⁡(θ)=−34\tan(\theta) = -\frac{3}{4}.

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<p>Angle of Depression Formula (Figure 9)</p>

Angle of Depression Formula (Figure 9)

From a lighthouse height of 151 ft151\,\text{ft} to a ship 1197 ft1197\,\text{ft} offshore, the angle of depression is x=tan⁡−1(1511197)x = \tan^{-1}(\frac{151}{1197}).

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Solution for Triangle with A=59∘A = 59^\circ, B=57∘B = 57^\circ, c=6c = 6

The third angle is C=180∘−(59∘+57∘)=64∘C = 180^\circ - (59^\circ + 57^\circ) = 64^\circ, and by the Law of Sines, a=6sin⁡(59∘)sin⁡(64∘)a = \frac{6\sin(59^\circ)}{\sin(64^\circ)} and b=6sin⁡(57∘)sin⁡(64∘)b = \frac{6\sin(57^\circ)}{\sin(64^\circ)}.

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Law of Cosines for Triangle with a=2a = 2, c=5c = 5, B=70∘B = 70^\circ

The side opposite angle BB is determined by b=a2+c2−2accos⁡(B)=22+52−2(2)(5)cos⁡(70∘)=29−20cos⁡(70∘)b = \sqrt{a^2 + c^2 - 2ac\cos(B)} = \sqrt{2^2 + 5^2 - 2(2)(5)\cos(70^\circ)} = \sqrt{29 - 20\cos(70^\circ)}.

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Law of Cosines Formulation for SSS Triangle (a=20a = 20, b=28b = 28, c=41c = 41)

The largest angle CC is obtained using cos⁡(C)=a2+b2−c22ab=202+282−4122(20)(28)\cos(C) = \frac{a^2 + b^2 - c^2}{2ab} = \frac{20^2 + 28^2 - 41^2}{2(20)(28)}.

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Ambiguous Case Analysis for c=50c = 50, a=57a = 57, C=38∘C = 38^\circ

Because the altitude h=asin⁡(C)=57sin⁡(38∘)≈35.1h = a\sin(C) = 57\sin(38^\circ) \approx 35.1 satisfies h<c<ah < c < a with acute angle CC, exactly two distinct triangles can be formed.

39
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<p>Distance Between Two Kites (Figure 10)</p>

Distance Between Two Kites (Figure 10)

Using the Law of Cosines on string lengths 102 ft102\,\text{ft} and 110 ft110\,\text{ft} with an included angle of 40∘40^\circ, the distance is d=1022+1102−2(102)(110)cos⁡(40∘) ftd = \sqrt{102^2 + 110^2 - 2(102)(110)\cos(40^\circ)}\,\text{ft}.

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<p>Angle of Lean of the Tree (Figure 11)</p>

Angle of Lean of the Tree (Figure 11)

In the triangle with ground base 54 ft54\,\text{ft}, tree length 74 ft74\,\text{ft}, and elevation angle 67∘67^\circ, the angle at the tree top satisfies sin⁡(α)=54sin⁡(67∘)74\sin(\alpha) = \frac{54\sin(67^\circ)}{74}, making the lean angle θ=180∘−(67∘+α)\theta = 180^\circ - (67^\circ + \alpha).

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<p>Airplane Triangle Angles in Figure 12</p>

Airplane Triangle Angles in Figure 12

From depression angles 46∘46^\circ to ship A and 70∘70^\circ to ship B on opposite sides, the angle of elevation at ship A is 46∘46^\circ, at ship B is 70∘70^\circ, and the included vertex angle at the plane is 180∘−(46∘+70∘)=64∘180^\circ - (46^\circ + 70^\circ) = 64^\circ.

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Distance Between Ships A and B in Figure 12

Using the Law of Sines with plane distance 5 miles5\,\text{miles} to ship A, vertex angle 64∘64^\circ, and ship B elevation angle 70∘70^\circ, the distance between ships is d=5sin⁡(64∘)sin⁡(70∘) milesd = \frac{5\sin(64^\circ)}{\sin(70^\circ)}\,\text{miles}.

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Included Angle Between Bearings N50∘W\text{N}50^\circ\text{W} and N30∘E\text{N}30^\circ\text{E}

The total angle formed between a course 50∘50^\circ west of north and a course 30∘30^\circ east of north is 50∘+30∘=80∘50^\circ + 30^\circ = 80^\circ.

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Ship Distances After 40 Minutes40\,\text{Minutes}

In 40 minutes40\,\text{minutes} (23 hr\frac{2}{3}\,\text{hr}), a ship sailing at 15 mph15\,\text{mph} travels 15×23=10 miles15 \times \frac{2}{3} = 10\,\text{miles}, and a ship sailing at 30 mph30\,\text{mph} travels 30×23=20 miles30 \times \frac{2}{3} = 20\,\text{miles}.

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Separation Distance on Bearing Paths

Using the Law of Cosines for paths of 10 miles10\,\text{miles} and 20 miles20\,\text{miles} with an included angle of 80∘80^\circ, the distance apart is d=102+202−2(10)(20)cos⁡(80∘) milesd = \sqrt{10^2 + 20^2 - 2(10)(20)\cos(80^\circ)}\,\text{miles}.