The general form of a sinusoidal wave travelling along the x-axis is:
$y(x, t) = A \cos(kx - \omega t + \phi)$
We need to find the values for Amplitude ($A$), Wavenumber ($k$), Angular Frequency ($\omega$), and Phase Constant ($\phi$) based on the given information.
The maximum displacement is given as the amplitude:
$A = 2$ cm
The wavelength is given as $\lambda = 7.5$ cm. The wavenumber $k$ is calculated using the formula:
$k = \frac{2\pi}{\lambda}$
Substituting the value of $\lambda$:
$k = \frac{2\pi}{7.5 \text{ cm}} = \frac{4\pi}{15} \text{ rad/cm} \approx 0.8377$ rad/cm
Comparing with the options, we see that Options 3 and 4 have $k \approx 0.83$. Options 1 ($k = 0.13$) and 2 ($k = 3.35$) are unlikely.
The wave travels a distance of 1.2 cm in 0.3 sec. The wave speed $v$ is:
$v = \frac{\text{Distance}}{\text{Time}} = \frac{1.2 \text{ cm}}{0.3 \text{ sec}} = 4$ cm/sec
The angular frequency $\omega$ is related to the wave speed $v$ and wavenumber $k$ by $\omega = vk$:
$\omega = v \times k = 4 \text{ cm/sec} \times \frac{4\pi}{15} \text{ rad/cm} = \frac{16\pi}{15} \text{ rad/sec} \approx 3.351$ rad/sec
Comparing with the remaining Options 3 and 4:
Option 4 aligns closely with our calculated value for $\omega$.
We are given that the wave has a crest (maximum displacement, $y=A$) at $x=0$ at $t=0$. Plugging this condition into the general cosine wave equation:
$y(0, 0) = A \cos(k(0) - \omega(0) + \phi) = A$
$A \cos(\phi) = A \implies \cos(\phi) = 1$
The simplest solution for this condition is $\phi = 0$. Therefore, the wave equation should be of the form $y = A \cos(kx - \omega t)$.
Option 3 uses a sine function. For $y = 2\sin(0.83x - 3.5t)$, at $x=0, t=0$, $y = 2\sin(0) = 0$, which is not a crest. Thus, Option 3 is incorrect.
Based on the calculations, the wave equation should be of the form $y = A \cos(kx - \omega t)$ with:
Option 4, $y = 2\cos(0.83x - 3.35t)$ cm, perfectly matches these derived parameters.
Conclusion: Option 4 correctly represents the sinusoidal wave.
Two simple harmonic motions, as shown below, are at right angles. They are combined to form lissajous figures.
$x(t) = A \sin (at + \delta)$
$y(t) = B \sin (bt)$
Identify the correct match below :
The motion of a mass on a spring, with spring constant K is as shown in figure.
The equation of motion is given by $x(t) = A\sin\omega t+B\cos\omega t$ with $\omega=\sqrt{\frac{K}{m}}$.
Suppose that at time $t = 0$, the position of mass is $x(0)$ and velocity $v(0)$, then its displacement can also be represented as $x(t) = C\cos(\omega t-\phi)$, where $C$ and $\phi$ are

A piston of mass $M$ is hung from a massless spring whose restoring force law goes as $F= -kx^3$, where $k$ is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature $T$) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $L_0$ to $L_1$, the total energy delivered by the filament is : (Assume spring to be in its natural length before heating)