Lets talk about a kind of force, acting on a particle of mass m , where the mean position is the origin ,is
F = ⎩ ⎪ ⎪ ⎨ ⎪ ⎪ ⎧ − k x 3 , for x>0 − 4 k 1 x 5 , for x<0 0 for x=0 .
Say that the particle is displaced by A in + v e x direction, and released.
Find the time period.
If your time period comes out to be
T = a k b m ∫ 0 A A c − x c d x + k 1 e m ∫ − 6 g f A 2 / 3 0 n j A 4 − x q d x
Find the value of a + b + c + e + f + g + j + n + q
Here all of the a , b , c , e , f , g , j , n , q are postive integers and g cd ( j , n ) = g cd ( f , g ) = 1 and e is square free integer. a is also square free integer.
Details and Assumptions
− ( 6 g f × A 3 2 ) is the lower limit of the second integral
Original
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Wow! What a latex you wrote! Let me copy!
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Haha. Sure :P
Good problem @Md Zuhair
By the way , @Md Zuhair Do you know to delete a set on BRILLIANT?
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First, consider the positive half of the harmonic oscillation.
We have,
F = − k x 3 ⟹ m a = − k x 3 ⟹ m v d x d v = − k x 3 ⟹ m ∫ 0 v v d v = − k ∫ A x x 3 d x ⟹ 2 v 2 = 4 m k A 4 − x 4 ( ∗ ) ⟹ v = 2 m k ( A 4 − x 4 ) ⟹ d t d x = 2 m k ( A 4 − x 4 ) ⟹ ∫ 0 t d t = k 2 m ∫ 0 A A 4 − x 4 d x ⟹ t = k 2 m ∫ 0 A A 4 − x 4 d x
The value of t is equal to half time-period of the oscillation on the positive side of the x-axis. The time period for positive half oscillation is thus
T 1 = 2 k 2 m ∫ 0 A A 4 − x 4 d x
Using ( ∗ ) , at x = 0 , we get 2 v 2 = 4 m k A 4 .
Now, consider the negative half of the harmonic oscillation.
We have,
F = − 4 k x 5 ⟹ m a = − 4 k x 5 ⟹ m v d x d v = − 4 k x 5 ⟹ m ∫ v 0 v d v = − 4 k ∫ x p x 5 d x ⟹ 2 v 2 = 3 m 2 k ( p 6 − x 6 ) ( ∗ ∗ ) ⟹ v = 3 m 4 k ( p 6 − x 6 ) ⟹ d t d x = 3 m 4 k ( p 6 − x 6 ) ⟹ ∫ 0 t d t = 4 k 3 m ∫ − p 0 p 6 − x 6 d x ⟹ t = 4 k 3 m ∫ − p 0 p 6 − x 6 d x
The value of t is equal to half time-period of the oscillation on the negative side of the x-axis. The time period for negative half oscillation is thus
T 2 = 2 4 k 3 m ∫ − p 0 p 6 − x 6 d x = k 3 m ∫ − p 0 p 6 − x 6 d x
Here p denotes the amplitude of oscillation on the negative side of the x-axis. Using ( ∗ ) and ( ∗ ∗ ) , at x = 0 , we get
2 v 2 = 4 m k A 4 = 3 m 2 k p 6 ⟹ p = 6 8 3 A 2 / 3
Hence
T 2 = k 3 m ∫ − 6 8 3 A 2 / 3 0 8 3 A 4 − x 6 d x
The total time period of oscillations is thus
T = T 1 + T 2 = 2 k 2 m ∫ 0 A A 4 − x 4 d x + k 3 m ∫ − 6 8 3 A 2 / 3 0 8 3 A 4 − x 6 d x
Comparing required values, we get
a + b + c + e + f + g + j + n + q = 2 + 2 + 4 + 3 + 3 + 8 + 3 + 8 + 6 = 3 9 .