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ESCUELA SUPERIOR POLITÉCNICA DE CHIMBORAZO PRIMER SEMESTRE PARALELO ¨B¨ ANÁLISIS MATEMÁTICO I BORIS JOSUE ASQUI VACA 2020-2021 𝑟 = 1 − cos 𝜃 ; 𝜗 = 𝜋 3 • 𝐶𝑜𝑟𝑑𝑖𝑜𝑖𝑑𝑒 0 < 1 1 < 1 • 𝑉𝑒𝑟𝑖𝑓𝑖𝑐𝑎𝑟 𝑠𝑖 𝑟 = 𝑓(𝜃) 𝑝𝑎𝑠𝑎 𝑝𝑜𝑟 𝑒𝑙 𝑝𝑜𝑙𝑜 𝑟 = 0 1 − cos 𝜃 = 0 𝜃 = cos−1(1) 𝜃 = 0 • 𝐼𝑛𝑡𝑒𝑟𝑠𝑒𝑐𝑐𝑖ó𝑛 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 (0, 𝜋); 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 90𝑜 ( 𝜋 2 , 3𝜋 2 ) 𝜃 𝑟 (𝑟, 𝜃) 0 0 (0,0) 𝜋 2 1 (1, 𝜋 2 ) 𝜋 2 (2, 𝜋) 3𝜋 2 1 (1, 3𝜋 2 ) 4)𝐷𝑎𝑡𝑜𝑠 𝜋 6 𝜋 3 2𝜋 3 5𝜋 6 7𝜋 6 4𝜋 3 5𝜋 3 11𝜋 6 0.1339 0.5 1.5 1.8660 1.8660 1.5 0.5 0.1339 • 𝐻𝑎𝑙𝑙𝑎𝑟( 𝜇; 𝜑) → 𝜃 = 𝜋 3 = 60𝑜 tan 𝜇 = 1 − cos 𝜃 sin 𝜃 = 1 − cos(60𝑜) sin 60𝑜 = √3 3 𝜇 = arctan √3 3 → 30𝑜 = 𝜇 = 𝜋 6 𝜑 = 𝜃 + 𝜇 𝜑 = 60 + 30 𝜑 = 90 tan 𝜑 = 𝑟′ sin 𝜃 + 𝑟 cos 𝜃 𝑟′ cos 𝜃 − 𝑟 sin 𝜃 𝑟 = 1 − cos 𝜃 𝑟′ = sin 𝜃 tan 𝜑 = (sin 𝜃) sin 𝜃 + (1 − cos 𝜃) cos 𝜃 (sin 𝜃) cos 𝜃 − (1 − cos 𝜃) sin 𝜃 tan 𝜑 = sin2 𝜃 + cos 𝜃 − cos2 𝜃 2(sin 𝜃) cos 𝜃 − sin 𝜃 • 𝑇𝑎𝑛𝑔𝑒𝑛𝑡𝑒𝑠 𝐻𝑜𝑟𝑖𝑧𝑜𝑛𝑡𝑎𝑙𝑒𝑠 sin2 𝜃 + cos 𝜃 − cos2 𝜃 = 0 1 − cos2 𝜃 + cos 𝜃 − cos2 𝜃 = 0 −2 cos2 𝜃 + cos 𝜃 + 1 = 0 𝑉𝑒𝑟𝑡𝑖𝑐𝑎𝑙𝑒𝑠 2(sin 𝜃) cos 𝜃 − sin 𝜃 = 0 sin 𝜃 (2 cos 𝜃 − 1) = 0 cos 𝜃 = 1 𝜃 = 0 𝜃 = 0 + 2𝜋𝑘 𝑘 = 0 𝜃 = 0 + 2𝜋(0) 𝜃 = 0 𝑘 = 1 𝜃 = 0 + 2𝜋(1) 𝜃 = 2𝜋 𝑘 = −1 𝜃 = 0 + 2𝜋(−1) 𝜃 = 0 − 2𝜋 𝜃 = −2𝜋 cos 𝜃 = − 1 2 𝜃 = 2𝜋 3 𝜃 = (−1)𝑘 2𝜋 3 + 𝜋𝑘 𝑘 = 0 𝜃 = (−1)0 2𝜋 3 + 𝜋𝑘 𝜃 = 2𝜋 3 𝑘 = 1 𝜃 = (−1)1 𝜋 3 + 𝜋(1) 𝜃 = 2 3 𝜋 𝑘 = −1 𝜃 = (−1)−1 𝜋 3 + 𝜋(−1) 𝜃 = − 4 3 𝜋 sin 𝜃 = 0 𝜃 = 0 𝜃 = 0 + 𝜋𝑘 𝑘 = 0 𝜃 = 0 + 𝜋(0) 𝜃 = 0 𝑘 = 1 𝜃 = 0 + 𝜋(1) 𝜃 = 𝜋 𝑘 = −1 𝜃 = 0 + 𝜋(−1) 𝜃 = −𝜋 cos 𝜃 = 1 2 𝜃 = 𝜋/3 𝜃 = 𝜋 3 + 2𝜋𝑘 𝑘 = 0 𝜃 = 𝜋 3 + 2𝜋(0) 𝜃 = 𝜋 3 𝑘 = 1 𝜃 = 𝜋 3 + 2𝜋(1) 𝜃 = 7 3 𝜋 𝑘 = −1 𝜃 = 𝜋 3 + 2𝜋(−1) 𝜃 = 𝜋 3 𝑟 = 2 − 3sin 𝜃 ; 𝜗 = 𝜋 4 • 𝐿𝑖𝑚𝑎𝑧𝑜𝑛 0 < 2 3 < 1 • 𝑉𝑒𝑟𝑖𝑓𝑖𝑐𝑎𝑟 𝑠𝑖 𝑟 = 𝑓(𝜃) 𝑝𝑎𝑠𝑎 𝑝𝑜𝑟 𝑒𝑙 𝑝𝑜𝑙𝑜 𝑟 = 0 2 − 3sin 𝜃 = 0 𝜃 = sin−1 ( 2 3 ) 𝜃 = 41.81 • 𝐼𝑛𝑡𝑒𝑟𝑠𝑒𝑐𝑐𝑖ó𝑛 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 (0, 𝜋); 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 90𝑜 ( 𝜋 2 , 3𝜋 2 ) 𝜃 𝑟 (𝑟, 𝜃) 0 2 (2,0) 𝜋 2 −1 (−1, 𝜋 2 ) 𝜋 2 (2, 𝜋) 3𝜋 2 5 (5, 3𝜋 2 ) 4)𝐷𝑎𝑡𝑜𝑠 𝜋 6 𝜋 3 2𝜋 3 5𝜋 6 7𝜋 6 4𝜋 3 5𝜋 3 11𝜋 6 0.5 0.5 -0.60 0.5 3.5 4.60 4.60 3.5 • 𝐻𝑎𝑙𝑙𝑎𝑟 (𝜇; 𝜑) → 𝜃 = 𝜋 4 = 45𝑜 tan 𝜇 = 2 − 3sin 𝜃 −3 cos 𝜃 = 2 − 3sin(45) −3 cos(45) = 0.057 𝜇 = arctan 0.057 → 𝜇 = 3.27𝑜 𝜑 = 𝜃 + 𝜇 𝜑 = 45 + 3.27 𝜑 = 48.27 tan 𝜑 = 𝑟′ sin 𝜃 + 𝑟 cos 𝜃 𝑟′ cos 𝜃 − 𝑟 sin 𝜃 𝑟 = 2 − 3sin 𝜃 𝑟′ = −3 cos 𝜃 tan 𝜑 = (−3 cos 𝜃) sin 𝜃 + (2 − 3sin 𝜃) cos 𝜃 (−3 cos 𝜃) cos 𝜃 − (2 − 3sin 𝜃) sin 𝜃 tan 𝜑 = −6 cos 𝜃 𝑠𝑖𝑛𝜃 + 2 cos 𝜃 −3 cos2 𝜃 − 2 sin 𝜃 + 3 sin2 𝜃 • 𝑇𝑎𝑛𝑔𝑒𝑛𝑡𝑒𝑠 𝐻𝑜𝑟𝑖𝑧𝑜𝑛𝑡𝑎𝑙𝑒𝑠 −6 cos 𝜃 𝑠𝑖𝑛𝜃 + 2 cos 𝜃 = 0 2 cos 𝜃 (−3 sin 𝜃 + 1) = 0 𝑉𝑒𝑟𝑡𝑖𝑐𝑎𝑙𝑒𝑠 −3(1 − sin2 𝜃) − 2 sin 𝜃 + 3 sin2 𝜃 6 sin2 𝜃 − 2 sin 𝜃 − 3 = 0 2 cos 𝜃 = 0 𝜃 = 𝜋 2 𝜃 = 𝜋 2 + 𝜋𝑘 𝑘 = 0 𝜃 = 𝜋 2 + 𝜋(0) 𝜃 = 𝜋 2 𝑘 = 1 𝜃 = 𝜋 2 + 𝜋(1) 𝜃 = 3𝜋 2 𝑘 = −1 𝜃 = 𝜋 2 + 𝜋(−1) 𝜃 = − 𝜋 2 sin 𝜃 = 1 3 𝜃 = 0.1081𝜋 𝜃 = (−1)𝑘0.1081𝜋 + 𝜋𝑘 𝑘 = 0 𝜃 = (−1)00.1081𝜋 + 𝜋(0) 𝜃 = 0.1081𝜋 𝑘 = 1 𝜃 = (−1)10.1081𝜋 + 𝜋(1) 𝜃 = 0.8919𝜋 𝑘 = −1 𝜃 = (−1)−10.1081𝜋 + 𝜋(−1) 𝜃 = −1.1081𝜋 sin 𝜃 = 0.8931 𝜃 = 0.3515𝜋 𝜃 = 0.3515𝜋 + 𝜋𝑘 𝑘 = 0 𝜃 = 0.3515𝜋 + 𝜋(0) 𝜃 = 0.3515𝜋 𝑘 = 1 𝜃 = 0.3515𝜋 + 𝜋(1) 𝜃 = 1.3515𝜋 𝑘 = −1 𝜃 = 0.3515𝜋 + 𝜋(−1) 𝜃 = −0.6485𝜋 cos 𝜃 = −0.5598 𝜃 = 65 36 𝜋 𝜃 = 65 36 𝜋 + 2𝜋𝑘 𝑘 = 0 𝜃 = 65 36 𝜋 + 2𝜋(0) 𝜃 = 65 36 𝜋 𝑘 = 1 𝜃 = 65 36 𝜋 + 2𝜋(1) 𝜃 = 137 36 𝜋 𝑘 = −1 𝜃 = 65 36 𝜋 + 2𝜋(−1) 𝜃 = − 7 36 𝜋 𝑟 = 3 + 2 sin 𝜃 ; 𝜗 = 𝜋 6 • 0 < 3 2 < 1 • 𝑉𝑒𝑟𝑖𝑓𝑖𝑐𝑎𝑟 𝑠𝑖 𝑟 = 𝑓(𝜃) 𝑝𝑎𝑠𝑎 𝑝𝑜𝑟 𝑒𝑙 𝑝𝑜𝑙𝑜 𝑟 = 0 3 + 2 sin 𝜃 = 0 𝜃 = sin−1 (− 3 2 ) 𝜃 = 𝑆𝑖𝑛 𝑠𝑜𝑙𝑢𝑐𝑖ó𝑛 • 𝐼𝑛𝑡𝑒𝑟𝑠𝑒𝑐𝑐𝑖ó𝑛 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 (0, 𝜋); 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 90𝑜 ( 𝜋 2 , 3𝜋 2 ) 𝜃 𝑟 (𝑟, 𝜃) 0 3 (3,0) 𝜋 2 5 (5, 𝜋 2 ) 𝜋 3 (3, 𝜋) 3𝜋 2 1 (1, 3𝜋 2 ) 4)𝐷𝑎𝑡𝑜𝑠 𝜋 6 𝜋 3 2𝜋 3 5𝜋 6 7𝜋 6 4𝜋 3 5𝜋 3 11𝜋 6 4 4.73 4.73 4 2 1.26 1.26 2 • 𝐻𝑎𝑙𝑙𝑎𝑟 (𝜇; 𝜑) → 𝜃 = 𝜋 6 = 30𝑜 tan 𝜇 = 3 + 2 sin 𝜃 2 cos 𝜃 = 3 + 2 sin(30𝑜) 2 cos(30𝑜) = 2.3094 𝜇 = arctan 2.3094 → 𝜇 = 65.58𝑜 𝜑 = 𝜃 + 𝜇 𝜑 = 30 + 65.58 𝜑 = 96.58 tan 𝜑 = 𝑟′ sin 𝜃 + 𝑟 cos 𝜃 𝑟′ cos 𝜃 − 𝑟 sin 𝜃 𝑟 = 3 + 2 sin 𝜃 𝑟′ = 2 cos 𝜃 tan 𝜑 = (2 cos 𝜃) sin 𝜃 + (3 + 2 sin 𝜃) cos 𝜃 (2 cos 𝜃) cos 𝜃 − (3 + 2 sin 𝜃) sin 𝜃 tan 𝜑 = 4 sin 𝜃 cos 𝜃 + 3 cos 𝜃 2 cos2 𝜃 − 3 sin 𝜃 − 2 sin2 𝜃 • 𝑇𝑎𝑛𝑔𝑒𝑛𝑡𝑒𝑠 𝐻𝑜𝑟𝑖𝑧𝑜𝑛𝑡𝑎𝑙𝑒𝑠 4 sin 𝜃 cos 𝜃 + 3 cos 𝜃 = 0 cos 𝜃 (4 sin 𝜃 + 3) = 0 𝑉𝑒𝑟𝑡𝑖𝑐𝑎𝑙𝑒𝑠 2(1 − sin2 𝜃) − 3 sin 𝜃 − 2 sin2 𝜃 −4 sin2 𝜃 − 3 sin 𝜃 + 2 = 0 cos 𝜃 = 0 𝜃 = 𝜋 2 𝜃 = 𝜋 2 + 𝜋𝑘 𝑘 = 0 𝜃 = 𝜋 2 + 𝜋(0) 𝜃 = 𝜋 2 𝑘 = 1 𝜃 = 𝜋 2 + 𝜋(1) 𝜃 = 3𝜋 2 𝑘 = −1 𝜃 = 𝜋 2 + 𝜋(−1) 𝜃 = − 𝜋 2 sin 𝜃 = −3 4 𝜃 = 1.73𝜋 𝜃 = (−1)𝑘1.73𝜋 + 𝜋𝑘 𝑘 = 0 𝜃 = (−1)01.73𝜋 + 𝜋(0) 𝜃 = 1.73𝜋 𝑘 = 1 𝜃 = (−1)11.73𝜋 + 𝜋(1) 𝜃 = −0.73𝜋 𝑘 = −1 𝜃 = (−1)−11.73𝜋 + 𝜋(−1) 𝜃 = −2.73𝜋 sin 𝜃 = 1.1753 sin 𝜃 = 0.4253 𝜃 = 5 36 𝜋 𝜃 = 5 36 𝜋 + 2𝜋𝑘 𝑘 = 0 𝜃 = 5 36 𝜋 + 2𝜋(0) 𝜃 = 5 36 𝜋 𝑘 = 1 𝜃 = 5 36 𝜋 + 2𝜋(1) 𝜃 = 77 36 𝜋 𝑘 = −1 𝜃 = 5 36 𝜋 + 2𝜋(−1) 𝜃 = − 67 36 𝜋 𝑟 = 3 + 2 cos 𝜃 ; 𝜗 = 𝜋 9 0 < 3 2 < 1 • 𝑉𝑒𝑟𝑖𝑓𝑖𝑐𝑎𝑟 𝑠𝑖 𝑟 = 𝑓(𝜃) 𝑝𝑎𝑠𝑎 𝑝𝑜𝑟 𝑒𝑙 𝑝𝑜𝑙𝑜 𝑟 = 0 3 + 2 cos 𝜃 = 0 𝜃 = cos−1 (− 3 2 ) 𝜃 = 𝑁𝑜 ℎ𝑎𝑦 𝑠𝑜𝑙𝑢𝑐𝑖ó𝑛 • 𝐼𝑛𝑡𝑒𝑟𝑠𝑒𝑐𝑐𝑖ó𝑛 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 (0, 𝜋); 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 90𝑜 ( 𝜋 2 , 3𝜋 2 ) 𝜃 𝑟 (𝑟, 𝜃) 0 5 (5,0) 𝜋 2 3 (3, 𝜋 2 ) 𝜋 1 (1, 𝜋) 3𝜋 2 3 (3, 3𝜋 2 ) 4)𝐷𝑎𝑡𝑜𝑠 𝜋 6 𝜋 3 2𝜋 3 5𝜋 6 7𝜋 6 4𝜋 3 5𝜋 3 11𝜋 6 4.7320 4 2 1.2679 1.2679 2 4 4.7320 • 𝐻𝑎𝑙𝑙𝑎𝑟( 𝜇; 𝜑) → 𝜃 = 𝜋 9 = 20𝑜 tan 𝜇 = 3 + 2 cos 𝜃 −2 sin 𝜃 = 3 + 2 cos(20) −2 sin(20) = −7.1331 𝜇 = arctan −7.1331 → 278𝑜 = 𝜇 = 139 90 𝜋 𝜑 = 𝜃 + 𝜇 𝜑 = 20 + 278 𝜑 = 298𝑜 tan 𝜑 = 𝑟′ sin 𝜃 + 𝑟 cos 𝜃 𝑟′ cos 𝜃 − 𝑟 sin 𝜃 𝑟 = 3 + 2 cos 𝜃 𝑟′ = −2 sin 𝜃 tan 𝜑 = (−2 sin 𝜃) sin 𝜃 + (3 + 2 cos 𝜃) cos 𝜃 (−2 sin 𝜃) cos 𝜃 − (3 + 2 cos 𝜃) sin 𝜃 tan 𝜑 = −2 sin2 𝜃 + 3 cos 𝜃 + 2 cos2 𝜃 −2 sin 𝜃 cos 𝜃 − 3 sin 𝜃 − 2 cos 𝜃 sin 𝜃 • 𝑇𝑎𝑛𝑔𝑒𝑛𝑡𝑒𝑠 𝐻𝑜𝑟𝑖𝑧𝑜𝑛𝑡𝑎𝑙𝑒𝑠 −2 sin2 𝜃 + 3 cos 𝜃 + 2 cos2 𝜃 = 0 −2 (1 − cos2 𝜃) + 3 cos 𝜃 + 2 cos2 𝜃 = 0 4 cos2 𝜃 + 3 cos 𝜃 − 2 = 0 𝑉𝑒𝑟𝑡𝑖𝑐𝑎𝑙𝑒𝑠 −2 sin 𝜃 cos 𝜃 − 3 sin 𝜃 − 2 cos 𝜃 sin 𝜃 sin 𝜃 (−4 cos 𝜃 − 3) = 0 cos 𝜃 = 0.4253 𝜃 = 13 36 𝜋 𝜃 = 13 36 𝜋 + 2𝜋𝑘 𝑘 = 0 𝜃 = 13 36 𝜋 + 2𝜋(0) 𝜃 = 13 36 𝜋 𝑘 = 1 𝜃 = 13 36 𝜋 + 2𝜋(1) 𝜃 = 85 36 𝜋 𝑘 = −1 𝜃 = 13 36 𝜋 + 2𝜋(−1) 𝜃 = 59 36 𝜋 cos 𝜃 = −1.1753 sin 𝜃 = 0 𝜃 = 0 𝜃 = 0 + 𝜋𝑘 𝑘 = 0 𝜃 = 0 + 𝜋(0) 𝜃 = 0 𝑘 = 1 𝜃 = 0 + 𝜋(1) 𝜃 = 𝜋 𝑘 = −1 𝜃 = 0 + 𝜋(−1) 𝜃 = −𝜋 cos 𝜃 = − 3 4 𝜃 = 23 30 𝜋 𝜃 = 23 30 𝜋 + 2𝜋𝑘 𝑘 = 0 𝜃 = 23 30 𝜋 + 2𝜋(0) 𝜃 = 23 30 𝜋 𝑘 = 1 𝜃 = 23 30 𝜋 + 2𝜋(1) 𝜃 = 83 30 𝜋 𝑘 = −1 𝜃 = 23 30 𝜋 + 2𝜋(−1) 𝜃 = − 37 30 𝜋 𝑟 = 1 − sin2 𝜃; 𝜗 = 𝜋 6 • 𝐿𝑒𝑚𝑛𝑖𝑠𝑐𝑎𝑡𝑎𝑠 • 𝑉𝑒𝑟𝑖𝑓𝑖𝑐𝑎𝑟 𝑠𝑖 𝑟 = 𝑓(𝜃) 𝑝𝑎𝑠𝑎 𝑝𝑜𝑟 𝑒𝑙 𝑝𝑜𝑙𝑜 𝑟 = 0 cos2 𝜃 = 0 𝜃 = (cos−1(1))2 𝜃 = 1 • 𝐼𝑛𝑡𝑒𝑟𝑠𝑒𝑐𝑐𝑖ó𝑛 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 (0, 𝜋); 𝑒𝑗𝑒 𝑝𝑜𝑙𝑎𝑟 90𝑜 ( 𝜋 2 , 3𝜋 2 ) 𝜃 𝑟 (𝑟, 𝜃) 0 1 (1,0) 𝜋 2 0 (0, 𝜋 2 ) 𝜋 1 (1, 𝜋) 3𝜋 2 0 (0, 3𝜋 2 ) 4)𝐷𝑎𝑡𝑜𝑠 𝜋 6 𝜋 3 2𝜋 3 5𝜋 6 7𝜋 6 4𝜋 3 5𝜋 3 11𝜋 6 3/4 1/4 1.4 3/4 3/4 1.4 1/4 3/4 • 𝐻𝑎𝑙𝑙𝑎𝑟( 𝜇; 𝜑) → 𝜃 = 𝜋 6 = 30𝑜 tan 𝜇 = 1 − sin2 𝜃 −sin 2𝜃 = 1 − sin2(30) −sin(60) = −√3 2 𝜇 = arctan −√3 2 → 320𝑜 = 𝜇 = 16𝜋 9 𝜑 = 𝜃 + 𝜇 𝜑 = 320𝑜 + 30𝑜 𝜑 = 350𝑜 tan 𝜑 = 𝑟′ sin 𝜃 + 𝑟 cos 𝜃 𝑟′ cos 𝜃 − 𝑟 sin 𝜃 𝑟 = 1 − sin2 𝜃 𝑟′ = −sin 2𝜃 tan 𝜑 = (−2 cos 𝜃 sin 𝜃) sin 𝜃 + (cos2 𝜃) cos 𝜃 (−2 cos 𝜃 sin 𝜃) cos 𝜃 − (cos2 𝜃) sin 𝜃 tan 𝜑 = −2 cos 𝜃 (1 − cos2 𝜃) + cos3 𝜃 −3(1 − sin2 𝜃) sin 𝜃 • 𝑇𝑎𝑛𝑔𝑒𝑛𝑡𝑒𝑠 𝐻𝑜𝑟𝑖𝑧𝑜𝑛𝑡𝑎𝑙𝑒𝑠 −2 cos 𝜃 (1 − cos2 𝜃) + cos3 𝜃 = 0 3 cos3 𝜃 − 2 cos 𝜃 = 0 cos 𝜃 (3 cos2 𝜃 − 2) = 0 𝑉𝑒𝑟𝑡𝑖𝑐𝑎𝑙𝑒𝑠 −3(1 − sin2 𝜃) sin 𝜃 = 0 −3sin 𝜃 (1 − sin2 𝜃) = 0 cos 𝜃 = 0 𝜃 = 𝜋 2 𝜃 = 𝜋 2 + 2𝜋𝑘 𝑘 = 0 𝜃 = 𝜋 2 + 2𝜋(0) 𝜃 = 𝜋 2 𝑘 = 1 𝜃 = 𝜋 2 + 2𝜋(1) 𝜃 = 5 2 𝜋 𝑘 = −1 𝜃 = 𝜋 2 + 2𝜋(−1) 𝜃 = 𝜋 2 cos2 𝜃 = 2 3 𝜃 = 7𝜋 36 𝜃 = (−1)𝑘 7𝜋 36 + 𝜋𝑘 𝑘 = 0 𝜃 = (−1)0 7𝜋 36 + 𝜋𝑘 𝜃 = 7𝜋 36 𝑘 = 1 𝜃 = (−1)1 7𝜋 36 + 𝜋(1) 𝜃 = 29 36 𝜋 𝑘 = −1 𝜃 = (−1)−1 7𝜋 36 + 𝜋(−1) 𝜃 = 29 36 𝜋 −3 sin 𝜃 = 0 𝜃 = 0 𝜃 = 0 + 𝜋𝑘 𝑘 = 0 𝜃 = 0 + 𝜋(0) 𝜃 = 0 𝑘 = 1 𝜃 = 0 + 𝜋(1) 𝜃 = 𝜋 𝑘 = −1 𝜃 = 0 + 𝜋(−1) 𝜃 = −𝜋 cos2 𝜃 = 0 𝜃 = 𝜋 2 𝜃 = 𝜋 2 + 2𝜋𝑘 𝑘 = 0 𝜃 = 𝜋 2 + 2𝜋(0) 𝜃 = 𝜋 2 𝑘 = 1 𝜃 = 𝜋 2 + 2𝜋(1) 𝜃 = 5 2 𝜋 𝑘 = −1 𝜃 = 𝜋 2 + 2𝜋(−1) 𝜃 = 𝜋 2