/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 48 We are given a discrete-tinse, t... [FREE SOLUTION] | 91Ó°ÊÓ

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We are given a discrete-tinse, tinear, time-invariant, causal system with input denoted by \(x[n]\) and output denoted by \(y[n] .\) This system is specified by the following pair of difference equations, involving an intermextiate signal \(w[n]\) $$\begin{array}{l} y[n]+\frac{1}{4} y[n-1]+w[n]+\frac{1}{2} w[n-1]=\frac{2}{3} x[n] \\ y[n]-\frac{5}{4} y[n-1]+2 w[n]-2 w[n-1]=-\frac{5}{3} x[n] \end{array}$$ (a) Find the frequency response and wit sample response of the system. (b) Find a single difference equation relating \(x[n]\) and \(y[n]\) for the system.

Short Answer

Expert verified
To solve, apply the Z-transform to convert to frequency domain, solve for W(z), find H(z)=Y(z)/X(z), then derive H(e^{j\omega}) and h[n], finally form a single difference equation for y[n] solely.

Step by step solution

01

Apply Z-transform to the given equations

Starting with the system equations: \( y[n]+\frac{1}{4} y[n-1]+w[n]+\frac{1}{2} w[n-1]=\frac{2}{3} x[n] \) and \( y[n]-\frac{5}{4} y[n-1]+2w[n]-2w[n-1]=-\frac{5}{3} x[n] \), apply the Z-transform to both equations considering their linearity, causality, and time-invariance. Convert the differences into z-domain: \( Y(z), W(z), X(z) \) for outputs and inputs. The equations become: 1. \( Y(z) + \frac{1}{4}Y(z)z^{-1} + W(z) + \frac{1}{2}W(z)z^{-1} = \frac{2}{3} X(z) \) 2. \( Y(z) - \frac{5}{4}Y(z)z^{-1} + 2W(z) - 2W(z)z^{-1} = -\frac{5}{3} X(z) \).
02

Solve for intermediate signal W(z)

Using the transformed equations, solve for \( W(z) \) by eliminating \( Y(z) \). Rearrange the equations to isolate \( W(z) \):- From equation (1): \( W(z) + \frac{1}{2}W(z)z^{-1} = \frac{2}{3}X(z) - Y(z) - \frac{1}{4}Y(z)z^{-1} \) Solve for \( W(z) \): \( W(z) = \frac{2/3X(z) - Y(z) - 1/4Y(z)z^{-1}}{1 + 1/2z^{-1}} \).- From equation (2): Simplify similarly: \( 2W(z) - 2W(z)z^{-1} = -\frac{5}{3}X(z) - Y(z) + \frac{5}{4}Y(z)z^{-1} \).
03

Express in terms of Y(z) and X(z)

Substitute \( W(z) \) from its solved expression in Step 2 into the transformed equations to express all terms in terms of \( Y(z) \) and \( X(z) \). Simplify the resulting expressions to find a relationship for only \( Y(z) \) in terms of \( X(z) \), ideally to a single transfer function \( H(z) = \frac{Y(z)}{X(z)} \).
04

Find Frequency Response H(e^{j\omega})

From the previous step, having obtained the transfer function \( H(z) \), substitute \( z = e^{j\omega} \) to obtain the frequency response of the system, \( H(e^{j\omega}) \). This directly provides the system's response in the frequency domain, which is \( H(e^{j\omega}) = H(z)\big|_{z = e^{j\omega}} \).
05

Find Impulse Response h[n] using Inverse Z-transform

Using the transfer function \( H(z) \) derived previously, perform an inverse Z-transform to obtain the impulse response \( h[n] \). This requires decomposing \( H(z) \) into partial fractions if necessary, and then using known inverse Z-transform pairs or tables. This translates \( H(z) \) to a time-domain representation.
06

Derive a Single Difference Equation

Add together or eliminate intermediate terms in the original difference equations to find a unified difference equation that describes the relationship between \( x[n] \) and \( y[n] \) directly. Simplify using algebraic manipulations until you isolate terms involving only \( y[n], y[n-1], x[n], \) and potentially higher or mixed order terms to express in standard difference equation form. This shows \( y[n] \) explicitly as a function of past \( y's \) and current/past \( x's \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Frequency Response
To understand the frequency response of a system, think about how that system reacts to various input frequencies. It's like analyzing how a musical instrument plays different notes. Each note or frequency will have a different impact on the system output. In the context of the given system, the frequency response can be determined once you know the transfer function, denoted as \( H(z) \).
To find the frequency response, we substitute \( z = e^{j\omega} \) into the transfer function \( H(z) \). This transformation tells us how the system behaves in the frequency domain, showing us the magnitude and phase of the output for each frequency \( \omega \).
  • Magnitude Response: Shows how the amplitude of each frequency is altered.
  • Phase Response: Shows how the phase of each frequency is shifted.
Understanding the frequency response is essential because it helps to predict system behavior for a given input, which is crucial in designing and analyzing filters and other signal processing applications.
Z-transform
The Z-transform is a powerful mathematical tool that converts time-domain signals into the z-domain. This is analogous to how the Laplace transform works for continuous-time systems. The Z-transform provides a clearer viewpoint for understanding and working with difference equations of discrete systems.
Using the Z-transform, you can analyze and manipulate the system equations more easily than working directly in the time domain. When applied to the given set of equations, the time shifts (delays in \( y[n] \) and \( w[n] \)) transform into multiplications of powers of \( z^{-1} \). This makes it straightforward to handle convolutions and other operations.
  • Direct Mapping: Convert time-domain shifts into simple algebraic manipulations.
  • Simplification: Help in expressing systems with multiple difference equations into a single transfer function.
Once transformed, solving for the output \( Y(z) \) in terms of the input \( X(z) \) yields the system transfer function \( H(z) \). This function forms the core of system analysis, allowing exploration of both time-response and frequency-response characteristics.
Causal Systems
A causal system is one in which the output depends only on the current and past input values, not future ones. This concept is particularly important in real-time signal processing where future inputs are not available.
In the context of our system, causality is inherent in how the equations are structured. Both difference equations directly relate outputs and intermediate signals to past values, showcasing a classic feature of causality.
  • Real-world Relevance: Models systems that operate in real-time, such as audio processing or control systems.
  • Stability Considerations: In the design and analysis process, ensuring causality is crucial to maintaining system stability and predictability.
While analyzing or designing systems, understanding causality ensures that the models are physically realizable and implementable in a real-world scenario.
Impulse Response
The impulse response of a system is its output when the input is an impulse signal, often represented as \( \delta[n] \). It is crucial because it fully characterizes the behavior of linear time-invariant (LTI) systems, allowing you to predict the output for any arbitrary input through convolution.
For the system described by the difference equations, finding its impulse response starts with obtaining its transfer function \( H(z) \). Once you have \( H(z) \), performing the inverse Z-transform translates \( H(z) \) back to the time domain, providing the impulse response \( h[n] \).
  • System Characterization: Comprehensively describes how a system will behave for any input signal.
  • Predictive Ability: Allows calculation of the system's output in response to any input via the convolution operation.
By understanding and applying the concept of impulse response, especially in combination with the Z-transform, you can effectively model, analyze, and design discrete-time systems efficiently and accurately.

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Most popular questions from this chapter

Compute the Fourier transform of each of the following signals: $$\text { (a) } x[n]=u[n-2]-u[n-6]$$ $$\text { (b) } x[n]=\left(\frac{1}{2}\right)^{-n} u[-n-1]$$ $$\text { (c) } x[n]=\left\\{\frac{1}{3}\right)^{|n|} u[-n-2]$$ $$\text { (d) } x[n]=2^{n} \sin \left(\frac{\pi}{4} n\right) u[-n]$$ $$\text { (e) } x[n]=\left(\frac{1}{2}\right)^{|n|} \cos \left(\frac{\pi}{8}(n-1)\right)$$ $$\text { (P) } x[n]=\left\\{\begin{array}{ll} n, & -3 \leq n \leq 3 \\ 0, & \text { otherwise } \end{array}\right.$$ $$\text { (g) } x[n]=\sin \left(\frac{\pi}{2} n\right)+\cos (n)$$ $$\text { (h) } x[n]=\sin \left(\frac{5 \pi}{3} n\right)+\cos \left(\frac{7 \pi}{3} n\right)$$ (i) \(x[n]=x[n-6],\) and \(x[n]=u[n]-u[n-5]\) for \(0 \leq n \leq 5\) $$\text { (j) } x[n]=(n-1)\left(\frac{1}{3}\right)^{|n|}$$ $$\text { (k) } x[n]=\left(\frac{(\ln (\pi r / 5)}{\pi n}\right) \cos \left(\frac{7 \pi}{2} n\right)$$

In this problem we introduce the concept of windowing, which is of great importance both in the design of LTI systerns and in the spectral analysis of signals. Windowing is the operation of taking a signal \(x[n]\) and multiplying it by a finite-duration window. \(\operatorname{signal} w[n] .\) That is $$p[n]=x[n] w[n]$$ Note that \(p[n]\) is also of finite duration. The importance of windowing in spectral analysis stems from the fact that in numerous applications one wishes to compute the Fousier transform of a signal that has been measured Since in practice we can measure a signal \(x[n]\) only over a finte time interval (the time window), the actual signal available for spectral analysis is $$p[n]=\left\\{\begin{array}{ll} x[n], & -M \leq n \leq M \\ 0, & \text { otherwise } \end{array}\right.$$ where \(-M \leq n \leq M\) is the time window. Thus, \\[ p[n]=x[n] w[n] \\] where \(w[n]\) is the rectangular window; that is, \\[ w[n]=\left\\{\begin{array}{ll} 1, & -M \leq n \leq M \\ 0, & \text { otherwise } \end{array}\right. \\] Windowing also plays a role in LTI system design. Specifically, for a variety of reasons (such as the potential utility of the FFT algorithm; see Problem P5.54), it is often advantageous to design a system that has an impulse response of finite duration to achieve some desired signal-processing objective. That is, we often begin with a desired frequency response \(H\left(e^{j \omega}\right)\) whose inverse transform \(h[n]\) is an impulse response of infinite (or at least excessively long) duration. What is required then is the construction of an impulse response \(g[n]\) of finite duration whose transform \(G\left(e^{j \omega}\right)\) adequately approximates \(H\left(e^{j 00}\right),\) One general approach to choosing \(g[n]\) is to find a window function \(w[n]\) such that the transform of \(h[n] w[n]\) meets the desired specifications for \(G\left(e^{j \omega}\right)\) Clearly, the windowing of a signal has an effect on the resulting spectrum. In this problem, we illustrate that effect. (a) To gain some understanding of the effect of windowing, consider windowing the signal $$x[n]=\sum_{k=-\infty}^{\infty} \delta[n-k]$$ using the rectangular window signal given in eq. (PS.55-1). (i) What is \(X\left(e^{j \omega}\right) ?\) (ii) Sketch the tansform of \(p[n]=x\\{n] w[n]\) when \(M=1\) (iii) Do the same for \(M=10\) (b) Next, consider a signal \(x[n]\) whose Fourier transform is specified by $$X\left(e^{j \omega}\right)=\left\\{\begin{array}{ll} 1, & |\omega|<\pi / 4 \\ 0, & \pi / 4<|\omega| \leq \pi \end{array}\right.$$ Let \(p[n]=x[n] w[n],\) where \(w[n]\) is the rectangular window of eq. \((P 5.55-1) .\) Roughly sketch \(P\left(e^{j \omega}\right)\) for \(M=4,8,\) and 16 (c) One of the problems with the use of a rectangular window is that it intrioduces ripples in the transforn \(P\left(e^{\prime \omega}\right)\). (This is in fact directly related to the Gibbs phenomenon.) For that reason, a variety of other window signals have been developed. These signals are tapered; that is, they go from 0 to 1 more gradually than the abrupt transition of the rectangular window, The result is a reduction in the amplitude of the ripples in \(P\left(e^{j \omega}\right)\) at the expense of adding a bit of distortion in terms of further smoothing of \(X\left(e^{\prime \omega}\right)\) To illustrate the points just made, consider the signal \(x[n]\) described in part (b), and let \(p[n]=x[n] w[n],\) where \(w[n]\) is the triangular or Bartlet window: that is, $$w[n]=\left\\{\begin{array}{ll} 1-\frac{|n|}{n+1}, & -M \leq n \leq M \\ 0, & \text { otherwise } \end{array}\right.$$ Roughly sketch the Fourier transform of \(p[n]=x[n] w[n]\) for \(M=4,8,\) and 16\. [Hint: Note that the triangular signal can be obtained as a convolution of a rectangular signal with itself. This fact Jeads to a convenient expression for \(W\left(e^{J \omega}\right)\) (d) Let \(p[n]=x[n] w[n],\) where \(w[n]\) is a raised cosine signal known as the \(H a n\) ning wradow: i.e., $$w[n]=\left\\{\begin{array}{ll} \frac{1}{2}[1+\cos (\pi n / M)], & -M \leq n \leq M \\ 0, & \text { otherwise } \end{array}\right.$$ Roughly skecch \(P\left(e^{j \omega}\right)\) for \(M=4,8,\) and 16

Determine the Fourier transform for \(-\pi \leq \omega<\pi\) in the case of each of the following periodic signals: (a) \(\sin \left(\frac{\pi}{3} n+\frac{\pi}{4}\right)\) (b) \(2+\cos \left(\frac{\pi}{6} n+\frac{\pi}{8}\right)\)

Let \(x[m, n]\) be a signal that is a function of the two independent, discrete variables \(m\) and \(n .\) In analogy with one dimension and with the continuous- time case treated in Problem \(4.53,\) we can define the two-dimensional Fourier transforn of \(x[m, n]\) as $$X\left(e^{j \omega_{1}}, e^{j \omega_{2}}\right)=\sum_{n=-x}^{\pi} \sum_{m=-\infty}^{\infty} x[m, n] e^{-j(\omega) n+\omega_{1} n}$$ (a) Show that eq. (P5.56-1) can be calculated as two successive one-dimensional Fourier transforms, first in \(m,\) with \(n\) regarded as fixed, and then in \(n .\) Use this result to detemine an expression for \(x[m, n]\) in terms of \(X\left(e^{j \omega_{1}}, e^{j \omega_{2}}\right)\) (b) Suppose that $$x[m, n]=a[m] b[n]$$ where \(a[m]\) and \(b[n]\) are each functions of only one independent variable. Let \(A\left(e^{j \omega}\right)\) and \(B\left(e^{j \omega}\right)\) denote the Fourier transforms of \(a[m]\) and \(b[n],\) respectively. (c) Determine the two-dimensional Fourier transforms of the following signais: (f) \(\quad x[m, n]=\delta[m-1] \delta[n+4]\) (ii) \(x[m, n]=\left(\frac{1}{2}\right)^{n} m u[n-2] u[-m]\) (ifi) \(x[m, n]=\left(\frac{1}{2}\right)^{\prime \prime} \cos (2 \pi m / 3) u\\{n 1\) (iv) \(x[m, n]=\left\\{\begin{array}{ll}1, & -2

Deternine whether each of the following statements is true or false. Justify your answers. In each statement, the Fourier transform of \(x[n]\) is denoted by \(X\left(e^{j \omega}\right)\) (a) If \(X\left(e^{j \omega}\right)=X\left(e^{j(\omega-1)}\right),\) then \(x[n]=0\) for \(|n|>0\) (b) If \(X\left(e^{j \omega}\right)=X\left(e^{j\left(\omega-\Psi^{\prime}\right)}\right),\) then \(x[n]=0\) for \(|n|>0\) (c) If \(X\left(e^{j \omega}\right)=X\left(e^{j \omega / 2}\right),\) then \(x[n]=B\) for \(|n|>0\) (d) If \(X\left(e^{j \omega}\right)=X\left(e^{j 2 \omega}\right),\) then \(x[n]=0\) for \(|n|>0\)

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