Oscillations
- A simple pendulum is suspended from the roof of a trolley which moves in a horizontal direction with an acceleration a, then the time period is given by T = 2π √l / g where g is equal to
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The effective value of acceleration due to gravity is √(a² + g²)
Correct Option: D
The effective value of acceleration due to gravity is √(a² + g²)
- A body is executing S.H.M. When the displacements from the mean position are 4cm and 5 cm, the corresponding velocities of the body are 10 cm per sec and 8 cm per sec. Then the time period of the body is
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For S.H.M., Velocity,
v = ω √a² - x² at displacement x.
⇒ 10 = ω √a² - 16 ..........(1)
and 8 = ω √a² - 25 ..........(2)Dividing , 52 = a2 - 16 = 25 42 a2 - 25 16
or , 16a2 - 256 = 25a2 - 625 ⇒ 9a2 = 369∴ a2 = 369 9
Putting this value in equation (2) mentioned above,10 = ω √{ (369 / 9) - 16 } ⇒ 10 = ω 225 9 or , ω = 10 × 3 = 2 radian / sec 15 Time period = 2π = 2π = π sec ω 2
Correct Option: C
For S.H.M., Velocity,
v = ω √a² - x² at displacement x.
⇒ 10 = ω √a² - 16 ..........(1)
and 8 = ω √a² - 25 ..........(2)Dividing , 52 = a2 - 16 = 25 42 a2 - 25 16
or , 16a2 - 256 = 25a2 - 625 ⇒ 9a2 = 369∴ a2 = 369 9
Putting this value in equation (2) mentioned above,10 = ω √{ (369 / 9) - 16 } ⇒ 10 = ω 225 9 or , ω = 10 × 3 = 2 radian / sec 15 Time period = 2π = 2π = π sec ω 2
- A simple harmonic oscillator has an amplitude A and time period T. The time required by it to travel from x = A to x = A/2 is
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For S.H.M., x = A sin 2π . t T When x = A , A = A sin 2π . t T ∴ sin 2π . t = 1 T ⇒ sin 2π . t = sin π ⇒ t = (T / 4) T 2 When x = A , A = A sin 2π .t 2 2 T or , sin π = sin 2π .t or t = (T / 12) 6 T
Now, time taken to travel from x = A tox = A/2 is (T/4 – T/12) = T/6Correct Option: A
For S.H.M., x = A sin 2π . t T When x = A , A = A sin 2π . t T ∴ sin 2π . t = 1 T ⇒ sin 2π . t = sin π ⇒ t = (T / 4) T 2 When x = A , A = A sin 2π .t 2 2 T or , sin π = sin 2π .t or t = (T / 12) 6 T
Now, time taken to travel from x = A tox = A/2 is (T/4 – T/12) = T/6
- If a simple harmonic oscillator has got a displacement of 0.02 m and acceleration equal to 2.0 m/s2 at any time, the angular frequency of the oscillator is equal to
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ω2 = acceleration = 2.0 displacement 0.02
ω2 = 100 or ω = 10 rad / sCorrect Option: A
ω2 = acceleration = 2.0 displacement 0.02
ω2 = 100 or ω = 10 rad / s
- A hollow sphere is filled with water. It is hung by a long thread. As the water flows out of a hole at the bottom, the period of oscillation will
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Time period of simple pendulum , T = 2π l ∝ √l g
where l is effective length.
[i.e distance between centre of suspension and centre of gravity of bob]
Initially, centre of gravity is at the centre of sphere. When water leaks the centre of gravity goes down until it is half filled; then it begins to go up and finally it again goes at the centre. That is effective length first increases and then decreases. As T ∝ √l , so time period first increases and then decreases.
Correct Option: A
Time period of simple pendulum , T = 2π l ∝ √l g
where l is effective length.
[i.e distance between centre of suspension and centre of gravity of bob]
Initially, centre of gravity is at the centre of sphere. When water leaks the centre of gravity goes down until it is half filled; then it begins to go up and finally it again goes at the centre. That is effective length first increases and then decreases. As T ∝ √l , so time period first increases and then decreases.