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MA211 Assignment 1

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Question 1 a.
ο‚·
Consider πœ™ = Ρ² + Ρ°, π‘‘β„Žπ‘’π‘› π‘Ÿ = 𝑓(Ρ²)
In polar coordinates π‘₯ = π‘Ÿπ‘π‘œπ‘  Ρ² π‘Žπ‘›π‘‘ 𝑦 = π‘Ÿπ‘ π‘–π‘›Ρ²
𝑑π‘₯
𝑑π‘₯
= −π‘Ÿπ‘ π‘–π‘› Ρ² + 𝑦 = π‘Ÿπ‘π‘œπ‘ Ρ²
,
𝑑Ѳ
𝑑Ѳ
ο‚·
The geometry of the problem is evident that 2πœ‹ − Ρ‘ − Ρ² = 2πœ‹ − πœ™, thus Ρ‘ = πœ™ − Ρ², therefore
the trig formula can been used
tan Ρ° = tan(πœ™ − Ρ²) =
ο‚·
𝑑𝑦
𝑑π‘₯
= π‘Ÿπ‘π‘œπ‘ Ρ² + 𝑠𝑖𝑛Ѳ ,
𝑑Ѳ
𝑑Ѳ
π‘‘π‘Žπ‘›πœ™ − π‘‘π‘Žπ‘›Ρ²
.
1 + π‘‘π‘Žπ‘›πœ™π‘‘π‘Žπ‘›Ρ²
Since tangent line to curve 𝑓(Ρ²) makes and angle πœ™ with respect to x-axis, we have
π‘‘π‘Žπ‘›πœ™ =
𝑑𝑦/𝑑Ѳ
π‘Žπ‘›π‘‘ π‘‘β„Žπ‘’π‘  𝑒𝑠𝑖𝑛𝑔 π‘‘β„Žπ‘’ π‘“π‘œπ‘Ÿπ‘šπ‘’π‘™π‘Ž,
𝑑𝑦/𝑑 Ρ²
π‘‘π‘Žπ‘›Ρ² =
𝑦
𝑔𝑖𝑣𝑒𝑠,
π‘₯
𝑑𝑦/𝑑π‘₯ 𝑦
𝑑𝑦
𝑑π‘₯
−
π‘₯
−𝑦
𝑑π‘₯/𝑑Ѳ π‘₯
𝑑Ѳ
𝑑Ѳ
tan Ρ° =
=
𝑦 𝑑𝑦/𝑑π‘₯
𝑑𝑦
𝑑π‘₯
1+( )
π‘₯
+𝑦
π‘₯ 𝑑π‘₯/𝑑Ѳ
𝑑Ѳ
𝑑Ѳ
π‘‘π‘Ÿ
π‘‘π‘Ÿ
) − 𝑦(−π‘Ÿπ‘ π‘–π‘›Ρ² + π‘π‘œπ‘ Ρ² )
𝑑Ѳ
𝑑Ѳ
=
π‘‘π‘Ÿ
π‘‘π‘Ÿ
π‘₯ (−π‘Ÿπ‘ π‘–π‘›Ρ² + π‘π‘œπ‘ Ρ² ) + 𝑦 (π‘Ÿπ‘π‘œπ‘ Ρ² + 𝑠𝑖𝑛Ѳ )
𝑑Ѳ
𝑑Ѳ
π‘₯ (π‘Ÿπ‘π‘œπ‘ Ρ² + 𝑠𝑖𝑛Ѳ
By substituting, we have,
tan Ρ° =
π‘‘π‘Ÿ
π‘‘π‘Ÿ
π‘Ÿπ‘π‘œπ‘ Ρ² (π‘Ÿπ‘π‘œπ‘ Ρ² + 𝑠𝑖𝑛Ѳ ( )) − π‘Ÿπ‘ π‘–π‘›Ρ² (−π‘Ÿπ‘ π‘–π‘›Ρ² + π‘π‘œπ‘ Ρ² ( ))
𝑑Ѳ
𝑑Ѳ
π‘‘π‘Ÿ
π‘‘π‘Ÿ
π‘Ÿπ‘ π‘–π‘›Ρ² (−π‘Ÿπ‘ π‘–π‘›Ρ² + π‘π‘œπ‘ Ρ² ( )) + π‘Ÿπ‘π‘œπ‘ Ρ² (π‘Ÿπ‘π‘œπ‘ Ρ² + 𝑠𝑖𝑛Ѳ ( ))
𝑑Ѳ
𝑑Ѳ
π‘Ÿ 2 π‘π‘œπ‘  2 Ρ² + π‘Ÿ 2 𝑠𝑖𝑛2 Ρ²
π‘Ÿ
=
π‘‘π‘Ÿ
π‘‘π‘Ÿ⁄
π‘Ÿπ‘π‘œπ‘  2
π‘Ÿ + π‘Ÿ 2 𝑠𝑖𝑛2 Ρ²
𝑑Ѳ
𝑑Ѳ
π‘‘π‘Žπ‘›Ρ° =
π‘Ÿ
π‘‘π‘Ÿ/𝑑 Ρ²
Ρ° = π‘‘π‘Žπ‘›−1 (
π‘Ÿ
)
π‘‘π‘Ÿ
Ρ²
𝑑
Question 1 c
ο‚·
the equation of the larger circle in the cartesian coordinate equals, π‘₯ 2 + 𝑦 2 = 1
ο‚·
the points are, (1,
ο‚·
the center of the circle would be (
ο‚·
the equation of the smaller circle would be (π‘₯ −
ο‚·
π‘₯ 2 + 𝑦 2 − √2π‘₯ = 0
ο‚·
𝑙𝑒𝑑 π‘₯ = π‘…π‘π‘œπ‘ Ρ², π‘Žπ‘›π‘‘ 𝑦 = 𝑅𝑠𝑖𝑛Ѳ
πœ‹
)
√2
1 1
,
√2 √2
π‘Žπ‘›π‘‘ π‘’π‘žπ‘’π‘Žπ‘™π‘  (
)
1
, 0 ) π‘Žπ‘›π‘‘
√2
𝑖𝑑𝑠 π‘Ÿπ‘Žπ‘‘π‘–π‘’π‘  π‘€π‘œπ‘’π‘™π‘‘ 𝑏𝑒
1 2
)
√2
π‘₯ 2 = √2π‘₯ π‘…π‘π‘œπ‘ Ρ²
𝑅 = √2π‘₯ π‘π‘œπ‘ Ρ² , That is the equation of the small circle
+ 𝑦2 =
1
√2
1
√2
𝑖𝑛 π‘π‘Žπ‘Ÿπ‘‘π‘’π‘ π‘–π‘Žπ‘› π‘π‘œπ‘œπ‘Ÿπ‘‘π‘–π‘›π‘Žπ‘‘π‘’
Question 3
a)
I.
𝑦
𝑑𝐴
π‘₯ 2 +𝑦 2
βˆ¬π‘…
.R→ π‘‘π‘Ÿπ‘Žπ‘π‘’π‘§π‘–π‘œπ‘‘ π‘π‘œπ‘’π‘›π‘‘π‘’π‘‘ 𝑏𝑦 𝑦 = π‘₯; 𝑦 = 2π‘₯ ; π‘₯ = 1 ; π‘₯ = 2.
𝑦
𝑦
2
2π‘₯
5π‘₯ 2
𝑦
∫ ∫ − π‘₯2 +𝑦2 𝑑𝐴 = ∫1 ∫π‘₯
𝑦
𝑑𝑦𝑑π‘₯
π‘₯ 2 +𝑦2
𝐿𝑒𝑑 𝑒 = π‘₯ 2 + 𝑦 2
2π‘₯
= ∫π‘₯
=
1
2
𝑦
π‘₯ 2 +𝑦 2
𝑑𝑦 = ∫2π‘₯ 2 2 2𝑒 𝑑𝑒
5π‘₯ 2
2
5π‘₯
∫2π‘₯ 2 2 ∗ 𝑒 𝑑𝑒 = 2 [ln(𝑒)] 2
2π‘₯
1
1
1
= 2 ln[5π‘₯ 2 ] − ln[2π‘₯ 2 ]
1
= 2 ln[5] − ln[2]
21
= ∫1 2 ln(5) − ln(2) 𝑑π‘₯
21
= ∫1 2 ln(5) − ln(2) 𝑑π‘₯
1
2
= 2 [ln(5) − ln(2) x]
1
1
5
= 2 (ln(2)(2 − 1)
𝟏
πŸ“
Thus; R = 𝟐 π₯𝐧(𝟐)
II.
∫ ∫𝑅 π‘₯𝑑𝐴. Where R is a sector of the circle bounded by 𝑦 = √25 − π‘₯ 2 , 3π‘₯ − 4𝑦 = 0, 𝑦 = 0
3π‘₯ − 4𝑦 = 0
3π‘₯
4
𝑦=
π‘Žπ‘›π‘‘ π‘₯ =
4𝑦
3
2
𝑦 = √25 − π‘₯ 2 ; 𝑦 = 25 − π‘₯ 2
π‘₯ = √25 − 𝑦 2
π‘₯ = √25 − 𝑦 2 π‘Žπ‘›π‘‘ π‘₯ =
=
4𝑦
3
π‘₯=
< π‘₯ < √25 − 𝑦 2
4𝑦
3
=
16𝑦 2
9
+ 𝑦 2 = 25
25𝑦 2
9
= 25;
25𝑦 2
25
𝑦2 =
225
;𝑦
25
= √9
𝑦=3
= 225
4𝑦
3
√25−𝑦 2
3
π‘π‘œπ‘€; ∫0 ∫4𝑦
π‘₯𝑑π‘₯𝑑𝑦
3
√25−𝑦2
= ∫4𝑦
3
1
√25 − 𝑦 2
]
𝑑𝑦
4𝑦
2
3 π‘₯2
π‘₯𝑑π‘₯ = ∫0
3
3
= 2 ∫0 25 − 𝑦 2 −
1
= 2 ∫ 25 (1 −
16𝑦 2
𝑑𝑦
9
𝑦2
) 𝑑𝑦
9
𝑦3 3
− 27]
0
=
25
[𝑦
2
=
(3)3
25
(3 − 27 )
2
=
25
(3 −
2
=
25
(2)
2
1)
= πŸπŸ“
III.
Inside the cardioid π‘Ÿ = 1 + π‘π‘œπ‘ πœƒ and outside the circle π‘Ÿ = 3π‘π‘œπ‘ πœƒ
πœƒ
π‘Ÿ = 1 + π‘π‘œπ‘ πœƒ
0
45
90
135
180
225
270
315
360
2
1.71
1
0.29
0
0.29
1
1.71
2
π‘Ÿ1 = π‘Ÿ2
1 + π‘π‘œπ‘ πœƒ = 3π‘π‘œπ‘ πœƒ
1 + π‘π‘œπ‘ πœƒ − 3π‘π‘œπ‘ πœƒ = 0
1
π‘π‘œπ‘ πœƒ = 2 =
πœ‹
3
There are two area on the graph
π΄π‘Ÿπ‘’π‘Ž = 𝐴1 + 𝐴2
πœ‹
1+π‘π‘œπ‘ πœƒ
𝐴 = 2(∫03 π‘‘πœƒ ∫0
πœ‹
3π‘π‘œπ‘ πœƒ
π‘Ÿπ‘‘π‘Ÿ + ∫πœ‹2 π‘‘πœƒ + ∫0
3
3π‘π‘œπ‘ πœƒ
3
2.12
0
-2.12
-3
-2.12
0
2.12
3
π‘Ÿπ‘‘π‘Ÿ)
πœ‹
1+π‘π‘œπ‘ πœƒ
𝐴1 = ∫04 ∫0
π‘Ÿπ‘‘π‘Ÿπ‘‘πœƒ
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