3.
Let R = R= R = the radius of the sphere.
Let A D = r , B D = h , ∠ A B C = θ . AD=r, BD=h, \angle ABC=\theta. A D = r , B D = h , ∠ A BC = θ .
△ A B C \triangle ABC △ A BC
A C = 2 r , A O = O C = R , ∠ A O C = 2 ∠ A B C = 2 θ AC=2r, AO=OC=R, \angle AOC=2\angle ABC=2\theta A C = 2 r , A O = OC = R , ∠ A OC = 2∠ A BC = 2 θ
The Law of Cosines
( 2 r ) 2 = R 2 + R 2 − 2 R 2 cos ( 2 θ ) (2r)^2=R^2+R^2-2R^2\cos(2\theta) ( 2 r ) 2 = R 2 + R 2 − 2 R 2 cos ( 2 θ )
4 r 2 = 2 R 2 ( 2 sin 2 θ ) 4r^2=2R^2(2\sin^2\theta) 4 r 2 = 2 R 2 ( 2 sin 2 θ )
r = R sin θ r=R\sin \theta r = R sin θ
h = r tan ( θ / 2 ) = R sin θ tan ( θ / 2 ) h=r\tan(\theta/2)=R\sin \theta\tan(\theta/2) h = r tan ( θ /2 ) = R sin θ tan ( θ /2 )
V c o n e = 1 3 π r 2 h V_{cone}=\dfrac{1}{3}\pi r^2 h V co n e = 3 1 π r 2 h
V c o n e = V c o n e ( θ ) = 1 3 π R 3 sin 3 θ tan ( θ / 2 ) V_{cone}=V_{cone}(\theta)=\dfrac{1}{3}\pi R^3\sin^3 \theta\tan(\theta/2) V co n e = V co n e ( θ ) = 3 1 π R 3 sin 3 θ tan ( θ /2 )
( V c o n e ) θ ′ = 1 3 π R 3 ( 3 sin 2 θ cos ( θ ) tan ( θ / 2 ) (V_{cone})'_{\theta}=\dfrac{1}{3}\pi R^3\bigg(3\sin^2 \theta\cos(\theta)\tan(\theta/2) ( V co n e ) θ ′ = 3 1 π R 3 ( 3 sin 2 θ cos ( θ ) tan ( θ /2 )
+ 1 2 sin 3 θ ( 1 cos 2 ( θ / 2 ) ) ) +\dfrac{1}{2}\sin^3\theta(\dfrac{1}{\cos ^2(\theta/2)})\bigg) + 2 1 sin 3 θ ( cos 2 ( θ /2 ) 1 ) ) Find the critical numbr(s)
( V c o n e ) θ ′ = 0 (V_{cone})'_{\theta}=0 ( V co n e ) θ ′ = 0
1 3 π R 3 ( 3 sin 2 θ cos θ tan ( θ / 2 ) \dfrac{1}{3}\pi R^3\bigg(3\sin^2 \theta\cos\theta\tan(\theta/2) 3 1 π R 3 ( 3 sin 2 θ cos θ tan ( θ /2 )
+ sin 3 θ 2 cos 2 ( θ / 2 ) ) = 0 +\dfrac{\sin^3\theta}{2\cos ^2(\theta/2)}\bigg)=0 + 2 cos 2 ( θ /2 ) sin 3 θ ) = 0
sin 3 θ ( 3 cos θ + 1 ) 2 cos 2 ( θ / 2 ) = 0 \dfrac{\sin^3 \theta(3\cos\theta+1)}{2\cos ^2(\theta/2)}=0 2 cos 2 ( θ /2 ) sin 3 θ ( 3 cos θ + 1 ) = 0
cos θ = − 1 3 \cos \theta=-\dfrac{1}{3} cos θ = − 3 1 If 0 < θ < π − cos − 1 ( 1 / 3 ) , ( V c o n e ) θ ′ > 0 , V c o n e 0< \theta<\pi-\cos^{-1}(1/3), (V_{cone})'_{\theta}>0, V_{cone} 0 < θ < π − cos − 1 ( 1/3 ) , ( V co n e ) θ ′ > 0 , V co n e increases.
If π − cos − 1 ( 1 / 3 ) < θ < π , ( V c o n e ) θ ′ < 0 , V c o n e \pi-\cos^{-1}(1/3)<\theta<\pi, (V_{cone})'_{\theta}<0, V_{cone} π − cos − 1 ( 1/3 ) < θ < π , ( V co n e ) θ ′ < 0 , V co n e decreases.
The volune of inscribed cone has the absolute maximum at
θ = π − cos − 1 ( 1 / 3 ) \theta=\pi-\cos^{-1}(1/3) θ = π − cos − 1 ( 1/3 )
4.
tan α = 13 − 5 x = 8 x \tan \alpha=\dfrac{13-5}{x}=\dfrac{8}{x} tan α = x 13 − 5 = x 8
tan ( α + θ ) = 13 − 5 + 10 x = 18 x \tan (\alpha+\theta)=\dfrac{13-5+10}{x}=\dfrac{18}{x} tan ( α + θ ) = x 13 − 5 + 10 = x 18
tan ( α + θ ) = tan α + tan θ 1 − tan α tan θ \tan (\alpha+\theta)=\dfrac{\tan \alpha+\tan \theta}{1-\tan \alpha\tan \theta} tan ( α + θ ) = 1 − tan α tan θ tan α + tan θ
8 x + tan θ 1 − 8 x ( tan θ ) = 18 x \dfrac{\dfrac{8}{x}+\tan \theta}{1-\dfrac{8}{x}(\tan \theta)}=\dfrac{18}{x} 1 − x 8 ( tan θ ) x 8 + tan θ = x 18
8 + x tan θ = 18 − 144 x ( tan θ ) 8+x\tan \theta=18-\dfrac{144}{x}(\tan \theta) 8 + x tan θ = 18 − x 144 ( tan θ )
tan θ = 10 x x 2 + 144 \tan \theta=\dfrac{10x}{x^2+144} tan θ = x 2 + 144 10 x
( tan θ ) x ′ = 10 ( x 2 + 144 − 2 x 2 ) ( x 2 + 144 ) 2 (\tan\theta)'_x=\dfrac{10(x^2+144-2x^2)}{(x^2+144)^2} ( tan θ ) x ′ = ( x 2 + 144 ) 2 10 ( x 2 + 144 − 2 x 2 )
= 10 ( 144 − x 2 ) ( x 2 + 144 ) 2 =\dfrac{10(144-x^2)}{(x^2+144)^2} = ( x 2 + 144 ) 2 10 ( 144 − x 2 ) Find the critical number(s)
( tan θ ) x ′ = 0 = > 10 ( 144 − x 2 ) ( x 2 + 144 ) 2 = 0 (\tan\theta)'_x=0=>\dfrac{10(144-x^2)}{(x^2+144)^2}=0 ( tan θ ) x ′ = 0 => ( x 2 + 144 ) 2 10 ( 144 − x 2 ) = 0
x 1 = − 12 , x 2 = 12 x_1=-12, x_2=12 x 1 = − 12 , x 2 = 12 We consider x ≥ 0 x\geq 0 x ≥ 0
If 0 ≤ x < 12 , ( tan θ ) x ′ = 0 > 0 , tan θ 0\leq x<12, (\tan\theta)'_x=0>0, \tan \theta 0 ≤ x < 12 , ( tan θ ) x ′ = 0 > 0 , tan θ increases.
If x > 12 , ( tan θ ) x ′ = 0 < 0 , tan θ x>12, (\tan\theta)'_x=0<0, \tan \theta x > 12 , ( tan θ ) x ′ = 0 < 0 , tan θ decreases.
The angle θ \theta θ has the local maximum at x = 12 x=12 x = 12 ft.
Since the function tan θ \tan \theta tan θ has the only extremum for x ≥ 0 , x\geq 0, x ≥ 0 , then the angle θ \theta θ has the absolute maximum for x ≥ 0 x\geq 0 x ≥ 0 at x = 12 x=12 x = 12 ft.
5.
a = 8 cos θ , b = w sin θ a=\dfrac{8}{\cos \theta}, b=\dfrac{w}{\sin \theta} a = cos θ 8 , b = sin θ w
a + b = 27 a+b=27 a + b = 27
8 cos θ + w sin θ = 24 \dfrac{8}{\cos \theta}+\dfrac{w}{\sin \theta}=24 cos θ 8 + sin θ w = 24
w = 27 sin θ − 8 tan θ w=27\sin \theta-8\tan \theta w = 27 sin θ − 8 tan θ Find the first derivative
w θ ′ = 27 cos θ − 8 cos 2 θ w'_{\theta}=27\cos \theta-\dfrac{8}{\cos^2\theta} w θ ′ = 27 cos θ − cos 2 θ 8 Find the critical number(s)
w θ ′ = 0 = > 27 cos θ − 8 cos 2 θ = 0 w'_{\theta}=0=>27\cos \theta-\dfrac{8}{\cos^2\theta}=0 w θ ′ = 0 => 27 cos θ − cos 2 θ 8 = 0
27 cos 3 θ = 8 27\cos^3\theta=8 27 cos 3 θ = 8
cos θ = 2 / 3 \cos \theta=2/3 cos θ = 2/3
θ = cos − 1 ( 2 / 3 ) \theta=\cos^{-1}(2/3) θ = cos − 1 ( 2/3 ) If 0 < θ < cos − 1 ( 2 / 3 ) , w θ ′ > 0 , w 0<\theta<\cos^{-1}(2/3), w'_{\theta}>0, w 0 < θ < cos − 1 ( 2/3 ) , w θ ′ > 0 , w increases.
If cos − 1 ( 2 / 3 ) < θ < π / 2 , w θ ′ < 0 , w \cos^{-1}(2/3)<\theta<\pi/2, w'_{\theta}<0, w cos − 1 ( 2/3 ) < θ < π /2 , w θ ′ < 0 , w decreases.
sin 2 θ = 1 − ( 2 / 3 ) 2 = 5 / 9 \sin^2\theta=1-(2/3)^2=5/9 sin 2 θ = 1 − ( 2/3 ) 2 = 5/9
sin θ = 5 / 3 \sin \theta=\sqrt{5}/3 sin θ = 5 /3
w = 27 ( 5 / 3 ) − 8 ( 5 / 2 ) w=27(\sqrt{5}/3)-8(\sqrt{5}/2) w = 27 ( 5 /3 ) − 8 ( 5 /2 )
w = 5 5 f t w=5\sqrt{5}\ ft w = 5 5 f t
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