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Parallel and Series Parallel Configurations

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Lesson 4P

PARALLEL AND SERIES-PARALLEL CONFIGURATIONS

Illustrative Problems

1. Determine Vo, I1, ID1, and ID2 for the parallel diode configuration.

Solution:
Since the resulting current direction matches that of the arrow in each symbol and the applied voltage
is greater than 0.7 V, both diodes are in the “on” state. The voltage across parallel elements is always the
same and
Vo = 0.7 V
The current
𝑉𝑅 𝐸−𝑉𝐷 10 𝑉−0.7 𝑉
𝐼 =
1 = = = 28.18 mA
𝑅 𝑅 0.33 𝑘𝛺

This problem demonstrated one reason for placing diodes in parallel. If the current rating of the
diodes is only 20 mA, a current of 28.18 mA would damage the device if it appeared alone. By placing two
in parallel, the current is limited to a safe value of 14.09 mA with the same terminal voltage.

2. Determine the current I for the following network.


Solution:

Redrawing the network reveals that the resulting current direction is such as to turn on diode D 1 and
turn off diode D2. The resulting current I is then

𝐸1 −𝐸2 −𝑉𝐷 20 𝑉−4𝑉−0.7 𝑉


I= = ≅ 6.95 𝑚𝐴
𝑅 2.2 𝑘𝛺

3. Determine the voltage Vo for the network shown.

Solution:
Initially, it would appear that the applied voltage will turn both diodes “on”. However, if both were
“on”, the 0.7-V drop across the silicon diode would not match the 0.3 V across the germanium diode as
required by the fact that the voltage across parallel elements must be the same. At the instant during the
rise that 0.3 V is established across the germanium diode, it will turn “on” and maintain a level of 0.3 V.
The silicon diode will never have the opportunity to capture its required 0.7 V and therefore remains in its
open-circuit state as shown. The result
Vo = 12 V – 0.3 V = 11.7 V

4. Determine the currents I1, I2, and ID for the network.


Solution:

The applied voltage (pressure) is such as to turn both diodes on, as noted by the resulting current
directions in the network. Note the use of the abbreviated notation for “on” diodes and that the solution is
obtained through an application of techniques applied to dc series-parallel networks.

𝑉𝑇2 0.7 𝑉
𝐼1 = = = 0.212 mA
𝑅1 3.3 𝑘𝛺

Applying Kirchhoff’s voltage law around the indicated loop in clockwise direction yields
−𝑉2 + 𝐸 − 𝑉𝑇1 − 𝑉𝑇2 = 0
and 𝑉2 = 𝐸 − 𝑉𝑇1 − 𝑉𝑇2 = 20𝑉 − 0.7𝑉 = 18.6 𝑉
𝑉2 18.6 𝑉
with 𝐼2 = = = 3.32 mA
𝑅2 5.6 𝑘𝛺
At the bottom node (a),
𝐼𝐷2 + 𝐼1 = 𝐼2
and 𝐼𝐷2 = 𝐼2 −𝐼1 = 3.32 𝑚𝐴 − 0.212 𝑚𝐴 = 3.108 𝑚𝐴

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