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Q14.19(e):
Explain why (or how): the shape of a pulse gets distorted during propagation in a dispersive medium.

Solution :

Theoretical Foundation: Wave Superposition and Dispersion

A wave pulse is not a pure monochromatic wave of a single frequency $\omega$. According to the Fourier Theorem, any complex pulse $f(x, t)$ can be mathematically represented as a linear superposition of an infinite number of harmonic (sinusoidal) waves, each characterized by a distinct angular frequency $\omega$ and a corresponding wave number $k$.

The total pulse at time $t$ and position $x$ is given by the integral:

$f(x, t) = \int_{-\infty}^{\infty} A(k) e^{i(kx - \omega(k)t)} dk$

[Per the principle of superposition and Fourier analysis].

Step 1: The Role of the Dispersion Relation

In a non-dispersive medium, the phase velocity $v_p = \frac{\omega}{k}$ is constant for all frequencies. Consequently, every constituent component of the pulse travels at the same velocity $v$. The pulse shape remains invariant as it moves through space. [Ref: Wave Equation derivation for non-dispersive media].

In a dispersive medium, the dispersion relation is non-linear, meaning $\omega$ is a non-linear function of $k$ (i.e., $\frac{d^2\omega}{dk^2} \neq 0$). Thus, the phase velocity depends on the frequency: $v_p(k) = \frac{\omega(k)}{k}$.

Step 2: Differential Propagation Velocities

Since the pulse is a packet of waves with a range of wave numbers $[k, k + dk]$, each constituent frequency component travels at its own phase velocity $v_p(\omega)$. Because these components move at different speeds, they do not maintain their relative spatial positions within the envelope of the pulse.

Initial Pulse Shape Distorted/Spread Pulse Propagation Direction (x)

Step 3: Analytical Mechanism of Distortion

As the wave packet propagates, the individual spectral components undergo a relative phase shift $\Delta \phi = (k_1 - k_2)x - (\omega_1 - \omega_2)t$.

  • Phase Mismatch: Because $\frac{\omega_1}{k_1} \neq \frac{\omega_2}{k_2}$, the constructive interference that originally formed the "peak" of the pulse at $t=0$ is gradually lost.
  • Group Velocity Dispersion (GVD): The pulse envelope travels at the group velocity $v_g = \frac{d\omega}{dk}$. In dispersive media, $v_g$ is also a function of $k$. Different parts of the pulse envelope move at different speeds, leading to pulse broadening or "chirping."

Summary of Physical Process

The distortion is the direct result of Differential Phase Velocity. When different Fourier components of a pulse propagate with unequal phase velocities, the temporal alignment of these components is disrupted. This violates the condition for a rigid translation of the wave packet, manifesting macroscopically as a spreading and reshaping of the pulse profile. [Per the theory of Wave Packet Dynamics].

Final Solution: The shape of a pulse is distorted because a dispersive medium causes different frequency components of the pulse to propagate at different phase velocities, resulting in the loss of coherence in the superposition that maintains the original pulse envelope.


More Questions from Class 11 Physics Waves EXERCISES


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