Which one of the following four particles, whose displacement x and acceleration a xare related as following, is executing simple harmonic motion?
a x= -3x 2
Simple Harmonic Motion (SHM) is a special type of periodic motion where the restoring force is directly proportional to the displacement from the equilibrium position and acts towards the equilibrium position. A key characteristic of SHM is the relationship between the acceleration and the displacement of the particle.
Mathematically, the condition for a particle to be executing SHM is that its acceleration \(a_x\) along the direction of motion is directly proportional to its displacement \(x\) from the equilibrium position (usually taken as \(x=0\)) and is always directed towards the equilibrium position. This is represented by the equation:
\[ a_x = -\omega^2 x \]
Here, \(a_x\) is the acceleration, \(x\) is the displacement, and \(\omega\) (omega) is a positive constant called the angular frequency. The negative sign is crucial; it indicates that the acceleration is always in the opposite direction to the displacement, pulling the particle back towards the equilibrium point.
Let's examine each of the given relationships between displacement \(x\) and acceleration \(a_x\) to see which one fits the condition \(a_x = -\omega^2 x\).
Option 1: \(a_x = +3x\)
Option 2: \(a_x = +3x^2\)
Option 3: \(a_x = -3x^2\)
Option 4: \(a_x = -3x\)
Based on the analysis, the relationship that describes Simple Harmonic Motion among the given options is the one where acceleration is directly proportional to displacement and negatively signed, indicating it's directed towards the equilibrium. This is found in Option 4: \(a_x = -3x\).
| Property | Condition for SHM | Example from Options |
|---|---|---|
| Acceleration \(a_x\) and Displacement \(x\) Relationship | \(a_x \propto -x\) | \(a_x = -3x\) |
| Mathematical Form | \(a_x = -\omega^2 x\) (where \(\omega^2\) is a positive constant) | \(a_x = -3x\) (Here \(\omega^2 = 3\)) |
| Direction of Acceleration | Always directed towards the equilibrium position (\(x=0\)), opposite to the displacement. | If \(x > 0\), \(a_x < 0\); If \(x < 0\), \(a_x > 0\). |
The relationship \(a_x = -\omega^2 x\) is directly related to the restoring force in SHM. According to Newton's second law, \(F_x = m a_x\). Substituting the SHM acceleration condition, we get:
\[ F_x = m (-\omega^2 x) = -m\omega^2 x \]
Since \(m\) (mass) and \(\omega^2\) are positive constants, let \(k = m\omega^2\). Then the force becomes:
\[ F_x = -kx \]
This is Hooke's Law, which describes the restoring force exerted by an ideal spring. The constant \(k\) is the spring constant, and the negative sign shows the force is always directed towards the equilibrium position (\(x=0\)), opposite to the displacement. Systems that obey this force law, such as a mass on a spring (neglecting friction), execute Simple Harmonic Motion.
Therefore, a particle executes SHM if and only if the net force acting on it is a linear restoring force proportional to its displacement from equilibrium.
A pendulum clock is lifted to a height where the gravitational acceleration has a certain value g. Another pendulum clock of same length but of double the mass of the bob is lifted to another height where the gravitational acceleration is g/2. The time period of the second pendulum would be:
(in terms of period T of the first pendulum)In simple harmonic motion, the particle velocity lags behind the displacement by a phase angle of __________.