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Simple Harmonic Motion
At surface of earth time period
At height
The total energy of a particle executing simple harmonic motion (SHM) is given by:
where
is the mass of the particle, is the angular frequency of the SHM, and
is the amplitude of the motion. At any point during SHM, the kinetic energy of the particle is given by:
where
is the displacement of the particle from the mean position.
The potential energy of the particle at the same point is given by:
When the kinetic energy becomes equal to the potential energy, we have:
Simplifying this equation, we get:
Therefore, the distance from the mean position when the kinetic energy becomes equal to the potential energy is
The initial momentum of the system (bullet + bob) is the momentum of the bullet because the bob is initially at rest.
The momentum of the bullet is given by its mass times its velocity :
After the collision, the bullet and the bob move together with a common velocity.
Let's denote this common velocity as .
The final momentum is the combined mass of the bullet and bob times the common velocity :
According to the principle of conservation of linear momentum,
Plugging in the values :
Solving for :
After the collision, the system has some kinetic energy which will be completely converted to potential energy at the maximum height that the bob reaches.
Using the principle of conservation of energy :
Isolating , we get :
Substituting the values for and :
Looking at the given options, the result most closely matches Option A :
Therefore, the height to which the bob rises before swinging back is approximately .
The time period of a simple pendulum is given by the formula:
where
is the time period,
is the length of the pendulum, and
is the acceleration due to gravity at the location of the pendulum.
The acceleration due to gravity changes with height above the Earth's surface.
The acceleration due to gravity at a height
above the Earth's surface can be expressed as:
where
is the acceleration due to gravity at the surface of the Earth,
is the radius of the Earth, and
is the height above the Earth’s surface.
Since the time period of the pendulum depends on the square root of the inverse of the acceleration due to gravity, any change in
due to a change in height will affect the time period. Given that the time period of the pendulum at a height
above Earth's surface is
, and we're to find the time period
at a height of
, we can use the formula for acceleration due to gravity at different heights to express the relationship between
and
. For the initial case at height
:
For the new case at height
:
The time period is proportional to the square root of the inverse of
, so:
Therefore:
Rearranging this equation:
This corresponds to Option A.
Assertion (A): A simple pendulum transported to a planet where the mass and radius are 4 times and 2 times that of the Earth, respectively, has the same time period as it does on Earth.
Reason (R): The mass of the pendulum remains unchanged whether on Earth or the other planet.
Explanation: The acceleration due to gravity on a planet is given by the formula: where is the gravitational constant, is the mass of the planet, and is the radius of the planet.
For the new planet, the gravitational acceleration is: Thus, the gravitational acceleration on this new planet is the same as on Earth, .
The time period of a simple pendulum is determined by: where is the length of the pendulum, which indicates that the time period is independent of the mass of the pendulum.
Therefore, while Assertion (A) is true and Reason (R) is true, Reason (R) does not correctly explain Assertion (A) because the time period of the pendulum is also independent of the pendulum's mass, and the key factor is the unchanged gravitational acceleration.
From (1), This means we can explain assertion with the given reason.
We can determine the time period of the oscillations by considering that when the cube is depressed by a small displacement, the additional buoyant force provided by the displaced water acts as a restoring force.
Here’s a step‐by‐step explanation: Define the given values: Side length of the cube,
. Mass of the cube,
. Density of water,
. Acceleration due to gravity,
. Cross-sectional area of the cube (face area),
When the cube is depressed by a small distance
, the additional volume of water displaced is
Thus, the additional buoyant force is:
This force acts in the upward (restoring) direction. Notice that the force is proportional to the displacement
, which is the hallmark of simple harmonic motion (SHM). The effective spring constant,
, associated with this SHM is:
The period of oscillation for SHM is given by:
which, upon substituting for
, becomes:
Substitute the given values into the expression:
Calculate the denominator:
so,
Since,
we have:
The problem states that the time period is given by:
Writing our result in the same form:
We see that
Therefore, the correct answer is: Option A: 2.