Physics Oscillations

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2 months ago

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A
alok kumar singh

Contributor-Level 10

y = A sin ? 2 π t T

t 2 - t 1 = T 2 π sin - 1 ? x 1 A - sin - 1 ? x 2 A

New answer posted

2 months ago

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V
Vishal Baghel

Contributor-Level 10

T = 2 π l g

In summer, length will increase due to expansion, hence for same time period we have to decrease l  in summer.

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2 months ago

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New answer posted

2 months ago

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V
Vishal Baghel

Contributor-Level 10

at t = t? , x? = 0 ⇒ 0 = asin (ωt? + π/6)
⇒ ωt? + π/6 = π
at t = t? , x? = 0 ⇒ 0 = asin (ωt? + π/4)
⇒ ωt? + π/4 = π
From (i) and (ii)
ω (t? - t? ) = π/4 - π/6 ⇒ t? - t? = π/ (12ω)

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A
alok kumar singh

Contributor-Level 10

  π 2 a 2 F 4 L = π 2 * 1 π 2 1 0 4 * 1 = 2 . 5 J

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A
alok kumar singh

Contributor-Level 10

  τ A = I α

K x R = 3 2 M R 2 α            

K R θ R = 3 2 M R 2 α            

α = 2 K 3 M            

T = 2 π 3 M 2 K            

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2 months ago

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R
Raj Pandey

Contributor-Level 9

v m a x = A ω = A k m

Momentum conservation   m v max   + 0 = m v A + 2 m v B

v A + 2 v B = v m a x

v 2 - v 1 = u 1 - u 2 v B - v A = v m a x

By (1) & (2) v A = - A ω 3

v A = A new   ω

A ω 3 = A new   ω A new   = A 3 ; f = 1 3

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2 months ago

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V
Vishal Baghel

Contributor-Level 10

f? = 300 Hz
3rd overtone = 7f? = 2100 Hz

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R
Raj Pandey

Contributor-Level 9

H = λ 4

2 0 = λ 4

λ = 8 0 c m

Now first overtone for open organ pipe

L 2 = 4 λ 4 = λ = 8 0 c m

 

New answer posted

2 months ago

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A
alok kumar singh

Contributor-Level 10

Velocity of block in equilibrium, in first case,

v = A ω = A . k M            

Velocity of block in equilibrium, is second case,

v ' = A ' ω ' = A ' k M + m                  

From conservation of momentum,

Mv = (M + m) v'

M A k M = ( M + m ) A ' k M + m A ' = A M M + m          

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