Fundamental Theory of Channel Impulse Response
The fundamental theory behind the channel impulse response in wireless communication often involves complex exponential components such as:
\( h(t) = \sum_{i=1}^{L} a_i \cdot \delta(t - \tau_i) \cdot e^{j\theta_i} \)
Where:
- \( a_i \) is the amplitude of the \( i^{th} \) path
- \( \tau_i \) is the delay of the \( i^{th} \) path
- \( \theta_i \) is the phase shift (often due to Doppler effect, reflection, etc.)
- \( e^{j\theta_i} \) introduces a phase rotation (complex exponential)
- The convolution \( x(t) * h(t) \) gives the received signal
So, instead of representing the channel with only real-valued amplitudes, each path can be more accurately modeled using a complex gain:
\( h[n] = a_i \cdot e^{j\theta_i} \)
Channel Impulse Response Simulator
Input Signal (Unit Impulse x[n])
Channel Impulse Response (CIR)
Output Signal (Impulse Convolved with h[n]) — Real Part
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