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A body having mass \(5 \mathrm{~g}\) is executing S.H.M. with an amplitude of \(0.3 \mathrm{~m}\). If the periodic time of the system is \((\pi / 10) \mathrm{s}\), then the maximum force acting on body is \(\ldots \ldots \ldots \ldots\) (A) \(0.6 \mathrm{~N}\) (B) \(0.3 \mathrm{~N}\) (C) \(6 \mathrm{~N}\) (D) \(3 \mathrm{~N}\)

Short Answer

Expert verified
The maximum force acting on the body is 0.6 N (Option A).

Step by step solution

01

Identify the given values and the formula to find maximum acceleration

We are given the mass (m) of the body, the amplitude (A) of the oscillation, and the periodic time (T). We will use the maximum acceleration (a_max) formula in SHM, which is: a_max = ω²A, where ω is the angular frequency, and it is related to the periodic time by the formula: ω = 2π/T.
02

Calculate the angular frequency (ω)

Using the formula ω = 2π/T, we can find ω. We are given T = π/10 s, so we have: ω = 2π/(π/10) ω = 2 × 10 ω = 20 rad/s
03

Calculate the maximum acceleration (a_max)

Now, we can use the maximum acceleration formula: a_max = ω²A. We have found ω and the given amplitude A = 0.3 m, so we can calculate a_max: a_max = (20 rad/s)² × 0.3 m a_max = 400 × 0.3 m a_max = 120 m/s²
04

Calculate the maximum force (F_max)

Finally, we will use Newton's second law of motion (F = ma) to find the maximum force acting on the body. We have the mass (m = 5 g) and maximum acceleration (a_max = 120 m/s²). First, we need to convert the mass from grams to kilograms: m = 5 g × (1 kg/1000 g) m = 0.005 kg Now, we can calculate the maximum force (F_max): F_max = m × a_max F_max = 0.005 kg × 120 m/s² F_max = 0.6 N So, the maximum force acting on the body is 0.6 N, and the correct option is (A).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Maximum Force Calculation
When a body undergoes simple harmonic motion (SHM), it experiences force due to acceleration. The maximum force on the body is determined using Newton's second law: \( F = ma \), where \( F \) is force, \( m \) is mass, and \( a \) is acceleration.
In this specific context, we use the maximum acceleration of the body in SHM to find the maximum force.
  • First, convert the mass of the object from grams to kilograms, as the standard unit of mass in physics calculations is kg.
  • The formula for maximum acceleration in SHM is related to angular frequency \( \omega \) and amplitude \( A \): \( a_{max} = \omega^2 A \).
Calculate \( a_{max} \) with given \( \omega \) and amplitude, and then apply it in \( F = ma \) to find the maximum force.
This understanding makes it clear how force dynamics work in harmonic motion systems like springs and pendulums.
Angular Frequency
Angular frequency is a key concept in understanding SHM. It represents the rate of change of the phase of a sinusoidal waveform and is crucial for calculating many elements like velocity and acceleration.
  • Angular frequency \( \omega \) is related to the periodic time \( T \), which is the time required for one complete cycle of motion.
  • The formula is \( \omega = \frac{2\pi}{T} \), expressing how many radians a system executes per second.
Understanding \( \omega \) helps make sense of how a body oscillates within a system and allows for calculation of parameters like maximum acceleration and velocity.
Finding \( \omega \) is the first step in a host of subsequent calculations necessary for SHM analysis.
Newton's Second Law
Newton's second law is foundational in physics, stating that the force acting on an object is equal to the mass of the object multiplied by its acceleration: \( F = ma \).
In SHM, this relationship helps us determine how external forces affect motion. When maximum acceleration is calculated, as shown with max acceleration \( a_{max} \), we plug it into \( F = ma \) to discover the maximum force.
  • This law emphasizes that force and acceleration are directly proportional. Doubling the acceleration with a consistent mass doubles the force.
  • By analyzing how mass and acceleration affect force, you can predict motion behavior accurately, a critical element in engineering and physics.
This helps break down complex motion into measurable and predictable models, making problems more approachable and easier to solve.

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Most popular questions from this chapter

A person standing in a stationary lift measures the periodic time of a simple pendulum inside the lift to be equal to \(\mathrm{T}\). Now, if the lift moves along the vertically upward direction with an acceleration of \((\mathrm{g} / 3)\), then the periodic time of the lift will now be \((\mathrm{A}) \sqrt{3} \mathrm{~T}\) (B) \(\sqrt{(3 / 2) \mathrm{T}}\) (C) \((\mathrm{T} / 3)\) (D) \((\mathrm{T} / \sqrt{3})\)

If the equation for a transverse wave is \(\mathrm{y}=\mathrm{A} \operatorname{Sin} 2 \pi\) \(\\{(1 / \mathrm{T})-(\mathrm{x} / \lambda)\\}\). then for what wavelength will the maximum velocity of the particle be double the wave velocity ? (A) \((\pi \mathrm{A} / 4)\) (B) \((\pi \mathrm{A} / 2)\) (C) \(\pi \mathrm{A}\) (D) \(2 \pi \mathrm{A}\)

Twenty four tuning forks are arranged in such a way that each fork produces 6 beats/s with the preceding fork. If the frequency of the last tuning fork is double than the first fork, then the frequency of the second tuning fork is \(\ldots \ldots\) (A) 132 (B) 138 (C) 276 (D) 144

The periodic time of two oscillators are \(\mathrm{T}\) and \((5 \mathrm{~T} / 4)\) respectively. Both oscillators starts their oscillation simultaneously from the midpoint of their path of motion. When the oscillator having periodic time \(\mathrm{T}\) completes one oscillation, the phase difference between the two oscillators will be \(\ldots \ldots \ldots\) (A) \(90^{\circ}\) (B) \(112^{\circ}\) (C) \(72^{\circ}\) (D) \(45^{\circ}\)

A simple pendulum having length \(\ell\) is suspended at the roof of a train moving with constant acceleration 'a' along horizontal direction. The periodic time of this pendulum is.... (A) \(\mathrm{T}=2 \pi \sqrt{(\ell / \mathrm{g})}\) (B) \(\mathrm{T}=2 \pi \sqrt{\\{\ell /(\mathrm{g}+\mathrm{a})\\}}\) (C) \(\mathrm{T}=2 \pi \sqrt{\\{\ell /(\mathrm{g}-\mathrm{a})\\}}\) (D) \(\left.\mathrm{T}=2 \pi \sqrt{\\{\ell} /\left(\mathrm{g}^{2}+\mathrm{a}^{2}\right)\right\\}\)

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