Give step-by-step explanation and final answer A relaxed
(
zero initial conditions
)
DSP system is described by the difference equation y
(
n
)
+
0
.
1
y
(
n
-
9
)
-
0
.
2
y
(
n
-
8
)
-
0
.
3
y
(
n
-
1
)
-
0
.
4
y
(
n
-
0
)
-
0
.
5
y
(
n
-
1
)
=
x
(
n
)
+
x
(
n
+
1
)
a
.
Determine the impulse response y
(
n
)
due to the impulse sequence chi
(
n
)
=
delta
(
n
)
b
.
Determine system response y
(
n
)
due to the unit step function excitation, where u
(
n
)
=
1
for n
>
=
0
c
.
Find the transfer function H
(
z
)
d
.
Plot the poles and zeros on the z
-
plane with the unit circle e
.
Determine the stability of the system from the pole
-
zero plot f
.
Calculate the amplitude
(
magnitude
)
response of H
(
z
)
g
.
Calculate the phase response of H
(
z
)
Question:
Give step-by-step explanation and final answer A relaxed
(
zero initial conditions
)
DSP system is described by the difference equation y
(
n
)
+
0
.
1
y
(
n
-
9
)
-
0
.
2
y
(
n
-
8
)
-
0
.
3
y
(
n
-
1
)
-
0
.
4
y
(
n
-
0
)
-
0
.
5
y
(
n
-
1
)
=
x
(
n
)
+
x
(
n
+
1
)
a
.
Determine the impulse response y
(
n
)
due to the impulse sequence chi
(
n
)
=
delta
(
n
)
b
.
Determine system response y
(
n
)
due to the unit step function excitation, where u
(
n
)
=
1
for n
>
=
0
c
.
Find the transfer function H
(
z
)
d
.
Plot the poles and zeros on the z
-
plane with the unit circle e
.
Determine the stability of the system from the pole
-
zero plot f
.
Calculate the amplitude
(
magnitude
)
response of H
(
z
)
g
.
Calculate the phase response of H
(
z
)
This is AI generated Response.
Asked by: Test User 100192
Created at: 2025-05-17 13:39:47
Final Answer:
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Let's solve the **DSP system** described by the difference equation:
\[
y(n) + 0.1y(n-9) - 0.2y(n-8) - 0.3y(n-1) - 0.4y(n-0) - 0.5y(n-1) = x(n) + x(n+1)
\]
Let's first **rewrite and clarify** the equation.
Notice that \(y(n-0) = y(n)\):
\[
y(n) + 0.1y(n-9) - 0.2y(n-8) - 0.3y(n-1) - 0.4y(n) - 0.5y(n-1) = x(n) + x(n+1)
\]
Combine like terms:
\[
[y(n) - 0.4y(n)] + 0.1y(n-9) - 0.2y(n-8) + [-0.3y(n-1) - 0.5y(n-1)] = x(n) + x(n+1)
\]
\[
0.6y(n) + 0.1y(n-9) - 0.2y(n-8) - 0.8y(n-1) = x(n) + x(n+1)
\]
---
## a) **Impulse Response \( h(n) \) (i.e., response to \( x(n) = \delta(n) \))**
Let \( x(n) = \delta(n) \):
\[
0.6y(n) + 0.1y(n-9) - 0.2y(n-8) - 0.8y(n-1) = \delta(n) + \delta(n+1)
\]
But \( \delta(n+1) \) is 1 at \( n = -1 \), so for \( n \geq 0 \):
\[
0.6y(n) + 0.1y(n-9) - 0.2y(n-8) - 0.8y(n-1) = \delta(n)
\]
Initial conditions (system is relaxed): \( y(n) = 0 \) for \( n < 0 \).
### Let's compute \( y(0) \):
For \( n = 0 \):
\[
0.6y(0) + 0.1y(-9) - 0.2y(-8) - 0.8y(-1) = \delta(0) = 1
\]
All terms with negative indices are zero:
\[
0.6y(0) = 1 \implies y(0) = \frac{1}{0.6} = \boxed{1.6667}
\]
---
### For \( n = 1 \):
\[
0.6y(1) + 0.1y(-8) - 0.2y(-7) - 0.8y(0) = \delta(1) = 0
\]
\[
0.6y(1) - 0.8y(0) = 0
\]
\[
0.6y(1) = 0.8y(0)
\]
\[
y(1) = \frac{0.8}{0.6}y(0) = \frac{0.8}{0.6} \cdot 1.6667 = 1.3333 \cdot 1.6667 = \boxed{2.2222}
\]
---
### For \( n = 2 \):
\[
0.6y(2) + 0.1y(-7) - 0.2y(-6) - 0.8y(1) = 0
\]
\[
0.6y(2) - 0.8y(1) = 0
\]
\[
0.6y(2) = 0.8y(1)
\]
\[
y(2) = \frac{0.8}{0.6}y(1) = 1.3333 \cdot 2.2222 = \boxed{2.9629}
\]
---
### For \( n = 3 \):
\[
0.6y(3) - 0.8y(2) = 0
\]
\[
y(3) = 1.3333 \cdot 2.9629 = \boxed{3.9506}
\]
---
### Pattern:
So for \( n < 8 \), the impulse response is
\[
h(n) = 1.3333 \cdot h(n-1)
\]
with \( h(0) = 1.6667 \).
So \( h(n) = 1.6667 \cdot (1.3333)^n \) for \( n < 8 \).
---
**For \( n = 8 \):**
\[
0.6y(8) + 0.1y(-1) - 0.2y(0) - 0.8y(7) = 0
\]
\[
0.6y(8) - 0.2y(0) - 0.8y(7) = 0
\]
\[
0.6y(8) = 0.2y(0) + 0.8y(7)
\]
\[
y(8) = \frac{0.2y(0) + 0.8y(7)}{0.6}
\]
**For \( n = 9 \):**
\[
0.6y(9) + 0.1y(0) - 0.2y(1) - 0.8y(8) = 0
\]
Continue recursively by plugging values.
**Conclusion:**
- For \( n < 8 \), \( h(n) = 1.6667 \cdot (1.3333)^n \).
- For \( n \geq 8 \), use full recursion.
---
## b) **System Response to Unit Step Input \( x(n) = u(n) \)**
Right side: \( x(n) + x(n+1) = u(n) + u(n+1) \)
But \( u(n+1) = 1 \) for \( n \geq -1 \), so for \( n \geq 0 \), both are 1:
For \( n \geq 0 \):
\[
x(n) + x(n+1) = 1 + 1 = 2
\]
So the equation becomes:
\[
0.6y(n) + 0.1y(n-9) - 0.2y(n-8) - 0.8y(n-1) = 2
\]
Repeat similar steps as above, but with "2" on the right, compute \( y(0) \), \( y(1) \), etc.
---
## c) **Transfer Function \( H(z) \)**
Take the Z-transform (zero initial conditions):
\[
0.6Y(z) + 0.1z^{-9}Y(z) - 0.2z^{-8}Y(z) - 0.8z^{-1}Y(z) = X(z) + zX(z)
\]
\[
\left[0.6 + 0.1z^{-9} - 0.2z^{-8} - 0.8z^{-1}\right]Y(z) = (1 + z)X(z)
\]
\[
H(z) = \frac{Y(z)}{X(z)} = \frac{1 + z}{0.6 + 0.1z^{-9} - 0.2z^{-8} - 0.8z^{-1}}
\]
Multiply numerator and denominator by \( z^9 \) to get a polynomial in \( z \):
\[
H(z) = \frac{z^9 + z^{10}}{0.6 z^9 + 0.1 - 0.2z + (-0.8)z^{8}}
\]
or
\[
H(z) = \frac{z^9 (1 + z)}{0.6 z^9 + 0.1 - 0.2z - 0.8z^8}
\]
Or, collect terms in descending powers:
\[
\text{Numerator: } z^{10} + z^9
\]
\[
\text{Denominator: } 0.6z^9 - 0.8z^8 - 0.2z + 0.1
\]
---
## d) **Poles and Zeros on the z-plane**
- **Zeros:** Roots of numerator \( z^{10} + z^9 = z^9(z + 1) \)
- \( z = 0 \) (multiplicity 9)
- \( z = -1 \) (multiplicity 1)
- **Poles:** Roots of denominator \( 0.6z^9 - 0.8z^8 - 0.2z + 0.1 = 0 \)
Factor if possible; otherwise, solve numerically for roots.
---
## e) **Stability**
- A discrete system is **stable** if all poles are **inside the unit circle** (i.e., \( |z_p| < 1 \) for all poles).
---
## f) **Magnitude Response**
- \( |H(e^{j\omega})| \): Substitute \( z = e^{j\omega} \) into \( H(z) \).
---
## g) **Phase Response**
- \( \angle H(e^{j\omega}) \): Argument of \( H(e^{j\omega}) \).
---
## **Summary Table**
| Part | Step-by-step | Final Answer |
|------|--------------|--------------|
| a | See above | \( h(n) = 1.6667 \cdot (1.3333)^n \) for \( n < 8 \); for \( n \geq 8 \), see recursion. |
| b | As above | \( y(n) \) for step input: Same recursion as in (a) but with right side = 2. |
| c | Z-transform | \( H(z) = \frac{z^{10} + z^9}{0.6z^9 - 0.8z^8 - 0.2z + 0.1} \) |
| d | Roots | Zeros at \( z = 0 \) (×9), \( z = -1 \); poles are roots of denominator. |
| e | Check roots | Stable if all poles inside unit circle. |
| f | Substitute | \( |H(e^{j\omega})| = \left|\frac{e^{j10\omega} + e^{j9\omega}}{0.6e^{j9\omega} - 0.8e^{j8\omega} - 0.2e^{j\omega} + 0.1}\right| \) |
| g | Arg | \( \angle H(e^{j\omega}) = \arg\left(\frac{e^{j10\omega} + e^{j9\omega}}{0.6e^{j9\omega} - 0.8e^{j8\omega} - 0.2e^{j\omega} + 0.1}\right) \) |
---
## **If you need:**
- A MATLAB or Python script to plot poles/zeros or magnitude/phase, let me know!
- Step-by-step calculation for \( y(n) \) for the step input (part b) for a few n.
- Details on how to find pole locations numerically.
Let me know which you want to expand!
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