,RadioFrequencyIntegrated
Circuits and Systems
po po po
SolutionManual
Hooman Darabi
po
,Solutions to Problem Sets p o p o p o
The selected solutions to all
po po p o po p o 12 chapters problem sets are presented in this
p o p o p o p o po po po
manual. The problem sets
p o p o po p o p o depict examples of practical applications of the
p o p o p o p o p o p o
concepts described in the
p o p o p o p o po book, more detailed analysis of some of the
p o p o p o p o p o p o p o
ideas, or in some cases
p o p o p o p o p o p o present a new concept.
p o p o po
Note that selected problems have been
po p o p o p o po p o given answers already in the book.
p o p o po p o po
, 1 Chapter One po
1. Using spherical coordinates, find the capacitance formed by two
p o p o p o p o p o p o p o p o
concentric spherical conducting shells of radius a, and b. What is
p o po p o po p o p o p o p o p o p o p o
the capacitance of a metallic marble with a diameter of 1cm in free
p o p o p o p o po po po po p o p o p o p o p o
space? Hint: let 𝑏 → ∞, thus, 𝐶
p o p o p o p o p o p o p o p o
= 4𝜋𝜀𝜀0𝑎 = 0.55𝑝𝐹.
p o p o p o
Solution: Suppose the inner sphere has a surface charge density of +𝜌𝑆.
p o po p o p o p o p o p o p o p o po p o
The outer surface charge density is negative, and proportionally smaller (by
p o p o po po po po po po po po po
(𝑎/𝑏)2) to keep the total charge the same.
po po po po p o p o p o p o
-
+
+S + -
- + a
b
+
-
From Gauss’s law: po po
ф𝐷 ⋅ 𝑑𝑆 po p o p o = 𝑄𝑄 po p o = +𝜌𝑆4𝜋𝑎2
po
𝑆
Thus, inside the sphere (𝑎
po po p o p o
p o≤ 𝑟 p o p o
≤ 𝑏): p o
𝑎2
𝐷 = 𝜌𝑆 𝑎𝑟 p o
𝑟2 o uter
p o p o p o
p o
Assuming a potential of 𝑉0 betw𝑎 e 1e n the 𝑎i2nn er and
po po
𝜌 s2ur f a1ces, w1e have:
po po po pon npo po n pon po po po n po n p o po po
𝑉 = − 𝜌 𝑑𝑟 𝑆 𝑎 p o po p o p o p o
= p o
0 𝑆 ( − ) p o p o p o
2
𝑏 𝑟 𝜖 𝑎 𝑏
Thus: 𝜖
𝜌𝑆4𝜋𝑎2 = 4𝜋𝜖
𝑄𝑄
𝐶 = 𝑉 = 𝜌 1 1 1 p o 1 p o p o po ponn po p o
−
p o
𝑆
𝜖 𝑎 (𝑎 − ) 𝑎
0 2
𝑏 p o
p o
𝑏 p o
1
In the case of a metallic marble, 𝑏
po p o → ∞,
p o 𝑎.
p o po
= p o p o p o p o p o
and hence: 𝐶
p o p o p o Letting × po
p o n pon p o
36𝜋
= 4𝜋𝜀𝜀0 p o 𝜀𝜀0
−9 5
10 , and 𝑎 = 0.5𝑐𝑚,
po p o
𝑝𝐹
p o
= 0.55𝑝𝐹.
p o p o
p o p o p o p o
9
it yields
p o p o
2. Consider the parallel plate capacitor containing two different dielectrics. Find
po po po po po po po po po
Circuits and Systems
po po po
SolutionManual
Hooman Darabi
po
,Solutions to Problem Sets p o p o p o
The selected solutions to all
po po p o po p o 12 chapters problem sets are presented in this
p o p o p o p o po po po
manual. The problem sets
p o p o po p o p o depict examples of practical applications of the
p o p o p o p o p o p o
concepts described in the
p o p o p o p o po book, more detailed analysis of some of the
p o p o p o p o p o p o p o
ideas, or in some cases
p o p o p o p o p o p o present a new concept.
p o p o po
Note that selected problems have been
po p o p o p o po p o given answers already in the book.
p o p o po p o po
, 1 Chapter One po
1. Using spherical coordinates, find the capacitance formed by two
p o p o p o p o p o p o p o p o
concentric spherical conducting shells of radius a, and b. What is
p o po p o po p o p o p o p o p o p o p o
the capacitance of a metallic marble with a diameter of 1cm in free
p o p o p o p o po po po po p o p o p o p o p o
space? Hint: let 𝑏 → ∞, thus, 𝐶
p o p o p o p o p o p o p o p o
= 4𝜋𝜀𝜀0𝑎 = 0.55𝑝𝐹.
p o p o p o
Solution: Suppose the inner sphere has a surface charge density of +𝜌𝑆.
p o po p o p o p o p o p o p o p o po p o
The outer surface charge density is negative, and proportionally smaller (by
p o p o po po po po po po po po po
(𝑎/𝑏)2) to keep the total charge the same.
po po po po p o p o p o p o
-
+
+S + -
- + a
b
+
-
From Gauss’s law: po po
ф𝐷 ⋅ 𝑑𝑆 po p o p o = 𝑄𝑄 po p o = +𝜌𝑆4𝜋𝑎2
po
𝑆
Thus, inside the sphere (𝑎
po po p o p o
p o≤ 𝑟 p o p o
≤ 𝑏): p o
𝑎2
𝐷 = 𝜌𝑆 𝑎𝑟 p o
𝑟2 o uter
p o p o p o
p o
Assuming a potential of 𝑉0 betw𝑎 e 1e n the 𝑎i2nn er and
po po
𝜌 s2ur f a1ces, w1e have:
po po po pon npo po n pon po po po n po n p o po po
𝑉 = − 𝜌 𝑑𝑟 𝑆 𝑎 p o po p o p o p o
= p o
0 𝑆 ( − ) p o p o p o
2
𝑏 𝑟 𝜖 𝑎 𝑏
Thus: 𝜖
𝜌𝑆4𝜋𝑎2 = 4𝜋𝜖
𝑄𝑄
𝐶 = 𝑉 = 𝜌 1 1 1 p o 1 p o p o po ponn po p o
−
p o
𝑆
𝜖 𝑎 (𝑎 − ) 𝑎
0 2
𝑏 p o
p o
𝑏 p o
1
In the case of a metallic marble, 𝑏
po p o → ∞,
p o 𝑎.
p o po
= p o p o p o p o p o
and hence: 𝐶
p o p o p o Letting × po
p o n pon p o
36𝜋
= 4𝜋𝜀𝜀0 p o 𝜀𝜀0
−9 5
10 , and 𝑎 = 0.5𝑐𝑚,
po p o
𝑝𝐹
p o
= 0.55𝑝𝐹.
p o p o
p o p o p o p o
9
it yields
p o p o
2. Consider the parallel plate capacitor containing two different dielectrics. Find
po po po po po po po po po