Difference between revisions of "Aufgaben:Exercise 1.1: ISDN Supply Lines"
Line 10: | Line 10: | ||
\hspace{0.05cm},$$ | \hspace{0.05cm},$$ | ||
:$$\frac{b_{\rm K}(f)}{\rm rad} = \left [ 32.9 \cdot \frac{f}{\rm MHz} + 2.26 \cdot \left (\frac{f}{\rm MHz}\right )^{0.5}\right ]\cdot\frac{l}{\rm km} \hspace{0.05cm}.$$ | :$$\frac{b_{\rm K}(f)}{\rm rad} = \left [ 32.9 \cdot \frac{f}{\rm MHz} + 2.26 \cdot \left (\frac{f}{\rm MHz}\right )^{0.5}\right ]\cdot\frac{l}{\rm km} \hspace{0.05cm}.$$ | ||
− | + | Here $l$ denotes the line length. | |
Line 17: | Line 17: | ||
− | '' | + | ''Notes:'' |
− | * | + | *The exercise belongs to the chapter [[Examples_of_Communication_Systems/General_Description_of_ISDN|"General Description of ISDN"]]. |
− | * | + | *In particular, reference is made to the section [[Examples_of_Communication_Systems/General_Description_of_ISDN#Network_infrastructure_for_ISDN|"Network infrastructure for ISDN"]]. |
− | * | + | *Further information on the attenuation of copper lines can be found in the chapter "Properties of Electrical Cables" of the book [[Lineare zeitinvariante Systeme|"Linear and Time Invariant Systems"]]. |
− | *[PW95] | + | *[PW95] refers to the following publication: Pollakowski, P.; Wellhausen, H.-W.: Eigenschaften symmetrischer Ortsanschlusskabel im Frequenzbereich bis 30 MHz. Deutsche Telekom AG, Forschungs- und Technologiezentrum Darmstadt, 1995. |
Line 27: | Line 27: | ||
− | === | + | ===Questions=== |
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | {How many subscribers ($N$) can be connected to an ISDN local exchange through the main cable shown? |
|type="{}"} | |type="{}"} | ||
$N \ = \ $ { 50 3% } | $N \ = \ $ { 50 3% } | ||
− | { | + | {What are the consequences of two-wire transmission? |
|type="[]"} | |type="[]"} | ||
− | + | + | + The two transmission directions interfere with each other. |
− | + | + | + Crosstalk noise may occur. |
− | - | + | - Intersymbol interference occurs. |
− | { | + | {A DC signal is attenuated by a factor of $4$. What is the cable length $l$ ? |
|type="{}"} | |type="{}"} | ||
$l \ = \ $ { 2.36 3% } $\ \rm km$ | $l \ = \ $ { 2.36 3% } $\ \rm km$ | ||
− | { | + | {Which attenuation and phase value results from this for the frequency $f = 120 \ \rm kHz$ ? |
|type="{}"} | |type="{}"} | ||
$a_{\rm K}(f = 120 \ \rm kHz) \ = \ $ { 21.7 3% } $\ \rm dB$ | $a_{\rm K}(f = 120 \ \rm kHz) \ = \ $ { 21.7 3% } $\ \rm dB$ | ||
Line 51: | Line 51: | ||
</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(1)''' Two-wire transmission is used in the connection area. The possible connections are equal to the number of pairs in the main cable: $\underline{N = 50}$. |
− | '''(2)''' | + | '''(2)''' <u>Solutions 1 and 2</u> are correct: |
− | * | + | *Two-wire transmission requires a directional separation method, namely the so-called fork circuit. This has the task that at receiver $\rm A$ only the transmitted signal of subscriber $\rm B$ arrives, but not the own transmitted signal. This is generally quite successful with narrowband signals – for example, speech – but not completely. |
− | * | + | *Due to inductive and capacitive couplings, crosstalk can occur from the twin wire located in the same star quad, whereby near-end crosstalk (i.e. the interfering transmitter and the interfered receiver are located together) leads to greater impairments than far-end crosstalk. |
− | * | + | *On the other hand, the last solution is not applicable. Intersymbol interference – i.e. the mutual interference of neighboring symbols – can certainly occur, but it is not related to two-wire transmission. The reason for this are rather (linear) distortions due to the specific attenuation and phase curves. |
− | '''(3)''' | + | '''(3)''' The DC signal attenuation by a factor of $4$ can be expressed as follows: |
:$$a_{\rm K}(f = 0) = 20 \cdot {\rm lg}\,\,(4) = 12.04\,{\rm dB}\hspace{0.05cm}.$$ | :$$a_{\rm K}(f = 0) = 20 \cdot {\rm lg}\,\,(4) = 12.04\,{\rm dB}\hspace{0.05cm}.$$ | ||
− | * | + | *With the given coefficient $\text{5.1 dB/km}$, this gives the line length $l = 12.04/5.1\hspace{0.15cm}\underline{ = 2.36 \ \rm km}$. |
− | '''(4)''' | + | '''(4)''' Using the given equations and $ l = 2.36 \ \rm km$, we obtain: |
:$$a_{\rm K}(f = 120\,{\rm kHz})= (5.1 + 14.3 \cdot 0.12^{\hspace{0.05cm}0.59}) \cdot 2.36\,{\rm dB} \hspace{0.15cm}\underline{\approx 21.7\,{\rm dB}}\hspace{0.05cm},$$ | :$$a_{\rm K}(f = 120\,{\rm kHz})= (5.1 + 14.3 \cdot 0.12^{\hspace{0.05cm}0.59}) \cdot 2.36\,{\rm dB} \hspace{0.15cm}\underline{\approx 21.7\,{\rm dB}}\hspace{0.05cm},$$ | ||
:$$b_{\rm K}(f = 120\,{\rm kHz}) = (32.9 \cdot 0.12 + 2.26 \cdot 0.12^{\hspace{0.05cm}0.5}) \cdot 2.36\,{\rm rad}\hspace{0.15cm}\underline{ \approx 11.2\,{\rm rad}}\hspace{0.05cm}.$$ | :$$b_{\rm K}(f = 120\,{\rm kHz}) = (32.9 \cdot 0.12 + 2.26 \cdot 0.12^{\hspace{0.05cm}0.5}) \cdot 2.36\,{\rm rad}\hspace{0.15cm}\underline{ \approx 11.2\,{\rm rad}}\hspace{0.05cm}.$$ |
Revision as of 08:47, 2 October 2022
In ISDN (Integrated Services Digital Network) the final branch (near the subscriber) is connected to a local exchange (OVSt) by a copper twisted pair, whereby two twisted pairs are twisted into a so-called star quad. Several such star quads are then combined to form a basic bundle, and several basic bundles are combined to form a main bundle (see graphic).
In the network of Deutsche Telekom (formerly: Deutsche Bundespost), mostly copper lines with 0.4 mm core diameter are found, for whose attenuation and phase function the following equations are given in [PW95]:
- $$\frac{a_{\rm K}(f)}{\rm dB} = \left [ 5.1 + 14.3 \cdot \left (\frac{f}{\rm MHz}\right )^{0.59}\right ]\cdot\frac{l}{\rm km} \hspace{0.05cm},$$
- $$\frac{b_{\rm K}(f)}{\rm rad} = \left [ 32.9 \cdot \frac{f}{\rm MHz} + 2.26 \cdot \left (\frac{f}{\rm MHz}\right )^{0.5}\right ]\cdot\frac{l}{\rm km} \hspace{0.05cm}.$$
Here $l$ denotes the line length.
Notes:
- The exercise belongs to the chapter "General Description of ISDN".
- In particular, reference is made to the section "Network infrastructure for ISDN".
- Further information on the attenuation of copper lines can be found in the chapter "Properties of Electrical Cables" of the book "Linear and Time Invariant Systems".
- [PW95] refers to the following publication: Pollakowski, P.; Wellhausen, H.-W.: Eigenschaften symmetrischer Ortsanschlusskabel im Frequenzbereich bis 30 MHz. Deutsche Telekom AG, Forschungs- und Technologiezentrum Darmstadt, 1995.
Questions
Solution
(2) Solutions 1 and 2 are correct:
- Two-wire transmission requires a directional separation method, namely the so-called fork circuit. This has the task that at receiver $\rm A$ only the transmitted signal of subscriber $\rm B$ arrives, but not the own transmitted signal. This is generally quite successful with narrowband signals – for example, speech – but not completely.
- Due to inductive and capacitive couplings, crosstalk can occur from the twin wire located in the same star quad, whereby near-end crosstalk (i.e. the interfering transmitter and the interfered receiver are located together) leads to greater impairments than far-end crosstalk.
- On the other hand, the last solution is not applicable. Intersymbol interference – i.e. the mutual interference of neighboring symbols – can certainly occur, but it is not related to two-wire transmission. The reason for this are rather (linear) distortions due to the specific attenuation and phase curves.
(3) The DC signal attenuation by a factor of $4$ can be expressed as follows:
- $$a_{\rm K}(f = 0) = 20 \cdot {\rm lg}\,\,(4) = 12.04\,{\rm dB}\hspace{0.05cm}.$$
- With the given coefficient $\text{5.1 dB/km}$, this gives the line length $l = 12.04/5.1\hspace{0.15cm}\underline{ = 2.36 \ \rm km}$.
(4) Using the given equations and $ l = 2.36 \ \rm km$, we obtain:
- $$a_{\rm K}(f = 120\,{\rm kHz})= (5.1 + 14.3 \cdot 0.12^{\hspace{0.05cm}0.59}) \cdot 2.36\,{\rm dB} \hspace{0.15cm}\underline{\approx 21.7\,{\rm dB}}\hspace{0.05cm},$$
- $$b_{\rm K}(f = 120\,{\rm kHz}) = (32.9 \cdot 0.12 + 2.26 \cdot 0.12^{\hspace{0.05cm}0.5}) \cdot 2.36\,{\rm rad}\hspace{0.15cm}\underline{ \approx 11.2\,{\rm rad}}\hspace{0.05cm}.$$