,RadioFrequencyIntegrated
Circuits and Systems
bb bb bb
SolutionManual
Hooman Darabi
bb
,Solutions to Problem Sets b b b b b b
The selected solutions to all
bb bb b b bb b b 12 chapters problem sets are presented in this
b b b b b b b b bb bb bb
manual. The problem sets
b b b b bb b b b b depict examples of practical applications of the
b b b b b b b b b b b b
concepts described in the
b b b b b b b b bb book, more detailed analysis of some of the
b b b b b b b b b b b b b b
ideas, or in some cases
b b b b b b b b b b b b present a new concept.
b b b b bb
Note that selected problems have been
bb b b b b b b bb b b given answers already in the book.
b b b b bb b b bb
, 1 Chapter One bb
1. Using spherical coordinates, find the capacitance formed by two
b b b b b b b b b b b b b b b b
concentric spherical conducting shells of radius a, and b. What is
b b bb b b bb b b b b b b b b b b b b b b
the capacitance of a metallic marble with a diameter of 1cm in free
b b b b b b b b bb bb bb bb b b b b b b b b b b
space? Hint: let 𝑏 → ∞, thus, 𝐶
b b b b b b b b b b b b b b b b
= 4𝜋𝜀𝜀0𝑎 = 0.55𝑝𝐹.
b b b b b b
Solution: Suppose the inner sphere has a surface charge density of +𝜌𝑆.
b b bb b b b b b b b b b b b b b b bb b b
The outer surface charge density is negative, and proportionally smaller (by
b b b b bb bb bb bb bb bb bb bb bb
(𝑎/𝑏)2) to keep the total charge the same.
bb bb bb bb b b b b b b b b
-
+
+S + -
- + a
b
+
-
From Gauss’s law: bb bb
ф𝐷 ⋅ 𝑑𝑆 bb b b b b = 𝑄𝑄 bb b b = +𝜌𝑆4𝜋𝑎2
bb
𝑆
Thus, inside the sphere (𝑎
bb bb b b b b
b b≤ 𝑟 b b b b
≤ 𝑏): b b
𝑎2
𝐷 = 𝜌𝑆 𝑎𝑟 b b
𝑟2 o uter
b b b b b b
b b
Assuming a potential of 𝑉0 betw𝑎 e 1e n the 𝑎i 2nn er and
bb bb
𝜌 s2ur f a1ces, w1e have:
bb bb bb bbn nbb bb n b bn bb bb bb n bb n b b bb bb
𝑉 = − 𝜌 𝑑𝑟 𝑆 𝑎 b b bb b b b b b b
= b b
0 𝑆 ( − ) b b b b b b
2
𝑏 𝑟 𝜖 𝑎 𝑏
Thus: 𝜖
𝜌𝑆4𝜋𝑎2 = 4𝜋𝜖
𝑄𝑄
𝐶 = 𝑉 = 𝜌 1 1 1 b b 1 b b b b bb bbnn bb b b
−
b b
𝑆
𝜖 𝑎 (𝑎 − ) 𝑎
0 2
𝑏 b b
b b
𝑏 b b
1
In the case of a metallic marble, 𝑏
bb b b → ∞,
b b 𝑎.
b b bb
= b b b b b b b b b b
and hence: 𝐶
b b b b b b Letting × bb
b b n bbn b b
36𝜋
= 4𝜋𝜀𝜀0 b b 𝜀𝜀0
−9 5
10 , and 𝑎 = 0.5𝑐𝑚,
bb b b
𝑝𝐹
b b
= 0.55𝑝𝐹.
b b b b
b b b b b b b b
9
it yields
b b b b
2. Consider the parallel plate capacitor containing two different dielectrics. Find
bb bb bb bb bb bb bb bb bb
Circuits and Systems
bb bb bb
SolutionManual
Hooman Darabi
bb
,Solutions to Problem Sets b b b b b b
The selected solutions to all
bb bb b b bb b b 12 chapters problem sets are presented in this
b b b b b b b b bb bb bb
manual. The problem sets
b b b b bb b b b b depict examples of practical applications of the
b b b b b b b b b b b b
concepts described in the
b b b b b b b b bb book, more detailed analysis of some of the
b b b b b b b b b b b b b b
ideas, or in some cases
b b b b b b b b b b b b present a new concept.
b b b b bb
Note that selected problems have been
bb b b b b b b bb b b given answers already in the book.
b b b b bb b b bb
, 1 Chapter One bb
1. Using spherical coordinates, find the capacitance formed by two
b b b b b b b b b b b b b b b b
concentric spherical conducting shells of radius a, and b. What is
b b bb b b bb b b b b b b b b b b b b b b
the capacitance of a metallic marble with a diameter of 1cm in free
b b b b b b b b bb bb bb bb b b b b b b b b b b
space? Hint: let 𝑏 → ∞, thus, 𝐶
b b b b b b b b b b b b b b b b
= 4𝜋𝜀𝜀0𝑎 = 0.55𝑝𝐹.
b b b b b b
Solution: Suppose the inner sphere has a surface charge density of +𝜌𝑆.
b b bb b b b b b b b b b b b b b b bb b b
The outer surface charge density is negative, and proportionally smaller (by
b b b b bb bb bb bb bb bb bb bb bb
(𝑎/𝑏)2) to keep the total charge the same.
bb bb bb bb b b b b b b b b
-
+
+S + -
- + a
b
+
-
From Gauss’s law: bb bb
ф𝐷 ⋅ 𝑑𝑆 bb b b b b = 𝑄𝑄 bb b b = +𝜌𝑆4𝜋𝑎2
bb
𝑆
Thus, inside the sphere (𝑎
bb bb b b b b
b b≤ 𝑟 b b b b
≤ 𝑏): b b
𝑎2
𝐷 = 𝜌𝑆 𝑎𝑟 b b
𝑟2 o uter
b b b b b b
b b
Assuming a potential of 𝑉0 betw𝑎 e 1e n the 𝑎i 2nn er and
bb bb
𝜌 s2ur f a1ces, w1e have:
bb bb bb bbn nbb bb n b bn bb bb bb n bb n b b bb bb
𝑉 = − 𝜌 𝑑𝑟 𝑆 𝑎 b b bb b b b b b b
= b b
0 𝑆 ( − ) b b b b b b
2
𝑏 𝑟 𝜖 𝑎 𝑏
Thus: 𝜖
𝜌𝑆4𝜋𝑎2 = 4𝜋𝜖
𝑄𝑄
𝐶 = 𝑉 = 𝜌 1 1 1 b b 1 b b b b bb bbnn bb b b
−
b b
𝑆
𝜖 𝑎 (𝑎 − ) 𝑎
0 2
𝑏 b b
b b
𝑏 b b
1
In the case of a metallic marble, 𝑏
bb b b → ∞,
b b 𝑎.
b b bb
= b b b b b b b b b b
and hence: 𝐶
b b b b b b Letting × bb
b b n bbn b b
36𝜋
= 4𝜋𝜀𝜀0 b b 𝜀𝜀0
−9 5
10 , and 𝑎 = 0.5𝑐𝑚,
bb b b
𝑝𝐹
b b
= 0.55𝑝𝐹.
b b b b
b b b b b b b b
9
it yields
b b b b
2. Consider the parallel plate capacitor containing two different dielectrics. Find
bb bb bb bb bb bb bb bb bb