The solution to the differential can be expressed as the arc , , and the curve passes thru the origin so that , when .
The volume formed by rotating the above curve , about the -axis from to can be expressed as , where and are pairs of coprime positive integers.
Find:
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2 1 ∗ ( d x d y ) 2 − y a = 2 1 ⟹
d x d y = y 2 a + y ⟹ x = ∫ 2 a + y y d y
Let u 2 = y ⟹ 2 u d u = d y ⟹
x = 2 ∗ ∫ 2 a + u 2 u 2 d u
Let u = 2 a s i n h ( θ ) ⟹ d u = 2 a c o s h ( θ ) d θ ⟹
x = 2 a ∗ ∫ ( c o s h ( 2 θ ) − 1 ) d θ = 2 a ∗ ( 2 1 s i n h ( 2 θ ) − θ ) ) = a ∗ ( s i n h ( 2 θ ) − 2 θ ) + C .
x ( θ ) = 0 ⟹ C = 0 ⟹ X = a ∗ ( s i n h ( 2 θ ) − 2 θ ) )
x = u 2 = 2 a ∗ s i n h 2 ( θ ) = a ∗ ( c o s h ( 2 θ ) − 1 ) .
Replacing 2 θ by θ we obtain:
x = a ∗ ( s i n h ( θ ) − θ ) , y = a ∗ ( c o s h ( θ ) − 1 )
Now we rotate the curve about the x - axis from θ = 0 to θ = ln ( 2 ) .
The Volume V = π ∫ 0 ln ( 2 ) ( y ( θ ) ) 2 d θ d x d θ
a 3 π ∗ ∫ 0 ln ( 2 ) ( c o s h ( θ ) − 1 ) 3 d θ =
a 3 π ∗ ∫ 0 ln ( 2 ) ( c o s h 3 ( θ ) − 3 c o s h 2 ( θ ) + 3 c o s h ( θ ) − 1 ) d θ =
a 3 π ∗ ∫ 0 ln ( 2 ) ( ( 1 + s i n h 2 ( θ ) ) c o s h ( θ ) − 2 3 ( c o s h ( 2 θ ) + 1 ) + 3 c o s h ( θ ) − 1 ) d θ =
a 3 π ∗ ∫ 0 ln ( 2 ) ( 4 c o s h ( θ ) + s i n h 2 ( θ ) ∗ c o s h ( θ ) − 2 3 c o s h ( θ ) − 2 5 ) d θ =
a 3 π ∗ ( 4 s i n h ( θ ) + 3 s i n h 3 ( θ ) − 4 3 s i n h ( 2 θ ) − 2 5 ) ∣ 0 ln ( 2 ) =
a 3 π ∗ ( 3 + 6 4 9 − 3 2 4 5 − 2 5 ln ( 2 ) ) =
a 3 π ∗ ( 6 4 1 1 1 − 2 5 ln ( 2 ) ) = a 3 π ∗ ( n m − q p ∗ ln ( q ) )
⟹ m + n + p + q = 1 8 2 .