Given:
Step 1: Governing Equation of Damped Oscillations
The motion of a damped harmonic oscillator is given by:
\[ m \frac{d^2x}{dt^2} + b \frac{dx}{dt} + kx = 0 \]
Step 2: Expressions for Different Quantities
Step 3: Identifying the Incorrect Expression
The given option:
\[ x = A e^{-\frac{b}{m}} \cos(\omega' t + \phi) \]
is incorrect because the exponent should be \( -\frac{b}{2m} t \), not \( -\frac{b}{m} \).
Answer: The incorrect option is D.
In the case of damped oscillations, the general form of the displacement \(x(t)\) of the block is given by: \[ x(t) = Ae^{-\frac{b}{2m} t} \cos(\omega' t + \phi) \] where:
\(A\) is the initial amplitude,
\(b\) is the damping constant,
\(m\) is the mass of the block,
\(\omega'\) is the angular frequency of the damped oscillations,
\(\phi\) is the phase constant.
Now let's analyze each option: -
Option (A) is correct: The angular frequency \(\omega'\) of damped oscillations is given by \(\omega' = \sqrt{\frac{k}{m} - \left(\frac{b}{2m}\right)^2}\), which is the correct expression.
Option (B) is correct: The energy \(E\) in damped oscillations decreases exponentially over time, as shown by \(E = \frac{1}{2} kA^2 e^{-\frac{b}{m} t}\).
Option (C) is correct: This is the equation of motion for the damped harmonic oscillator.
Option (D) is incorrect: The expression \(x = Ae^{-\frac{b}{m}} \cos(\omega' t + \phi)\) is incorrect because the exponential decay factor should be in terms of time \(t\) rather than just a constant factor. The correct form is \(x(t) = Ae^{-\frac{b}{2m} t} \cos(\omega' t + \phi)\).
Thus, the correct answer is: \[{\text{(D) } x = Ae^{-\frac{b}{m}} \cos(\omega' t + \phi)} \]
A particle is subjected to simple harmonic motions as: $ x_1 = \sqrt{7} \sin 5t \, \text{cm} $ $ x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \, \text{cm} $ where $ x $ is displacement and $ t $ is time in seconds. The maximum acceleration of the particle is $ x \times 10^{-2} \, \text{m/s}^2 $. The value of $ x $ is:
A block of certain mass is placed on a rough floor. The coefficients of static and kinetic friction between the block and the floor are 0.4 and 0.25 respectively. A constant horizontal force \( F = 20 \, \text{N} \) acts on it so that the velocity of the block varies with time according to the following graph. The mass of the block is nearly (Take \( g = 10 \, \text{m/s}^2 \)):
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is