Homework 2 - City Tech OpenLab

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Juan Carlos Torres
Homework 2
1-1 Calculate the free-space wavelength in meters for the following frequencies:
a) 2KHz
𝑐 3π‘₯108 π‘š/𝑠
πœ†= =
= 𝟏. πŸ“π’™πŸπŸŽπŸ“ π’Ž
3
𝑓
2π‘₯10 𝐻𝑧
b) 200KHz
𝑐 3π‘₯108 π‘š/𝑠
πœ†= =
= 𝟏. πŸ“π’™πŸπŸŽπŸ‘ π’Ž
𝑓
2π‘₯105 𝐻𝑧
c) 20MHz
𝑐 3π‘₯108 π‘š/𝑠
πœ†= =
= πŸπŸ“π’Ž
𝑓 20π‘₯106 𝐻𝑧
d) 2GHz
πœ†=
𝑐 3π‘₯108 π‘š/𝑠
=
= 𝟎. πŸπŸ“π’Ž
𝑓
2π‘₯109 𝐻𝑧
1-2 Calculate the free-space wavelength in meters for the following frequencies:
a) 80KHz
πœ†=
𝑐 3π‘₯108 π‘š/𝑠
=
= πŸ‘πŸ•πŸ“πŸŽπ’Ž
𝑓 80π‘₯103 𝐻𝑧
πœ†=
𝑐 3π‘₯108 π‘š/𝑠
=
= πŸ‘πŸ•. πŸ“π’Ž
𝑓
8π‘₯108 𝐻𝑧
b) 8MHz
c) 800MHz
𝑐
3π‘₯108 π‘š/𝑠
πœ†= =
= 𝟎. πŸ‘πŸ•πŸ“π’Ž
𝑓 800π‘₯106 𝐻𝑧
Juan Carlos Torres
d) 8GHz
𝑐 3π‘₯108 π‘š/𝑠
πœ†= =
= πŸ‘πŸ•. πŸ“π’™πŸπŸŽ−πŸ‘ π’Ž
𝑓
8π‘₯109 𝐻𝑧
1-3 Calculate the free-space wavelength in miles for a frequency of 400 Hz
πœ†=
𝑐 186000π‘šπ‘–/𝑠
=
= πŸ’πŸ”πŸ“π’Žπ’Š
𝑓
400𝐻𝑧
1-4 Calculate the free-space wavelength in miles for a frequency of 1.5KHz
πœ†=
𝑐 186000π‘šπ‘–/𝑠
=
= πŸπŸπŸ’π’Žπ‘–
𝑓
1.5π‘₯103 𝐻𝑧
1-5 A sinusoidal signal has a free-space wavelength of 80m. Calculate the frequency.
𝑐 3π‘₯108 π‘š/𝑠
𝑓= =
= πŸ‘. πŸ•πŸ“π‘²π‘―π’›
πœ†
80
𝑐
πœ†=
𝑓
1-6 A sinusoidal signal has a free-space wavelength of 6m. Calculate the frequency.
πœ†=
𝑐
𝑓
𝑓=
𝑐 3π‘₯108 π‘š/𝑠
=
= πŸ“πŸŽπ‘΄π‘―π’›
πœ†
6
1-7 A digital signal utilizes pulses whose minimum widths are about 3ns. Assuming the speed of
light, determine the longest lengths of wire-pairs that can be allowed based on the 10% rule.
𝑑1 = 0.1 π‘₯ 3𝑛𝑠 = 0.3𝑛𝑠
𝑑1 =
𝑑
=
𝑐
𝑑 = 𝑑1 π‘₯ 𝑐 = (3π‘₯108 π‘š/𝑠)π‘₯ (0.3π‘₯10−9 π‘š/𝑠) = 𝟎. πŸŽπŸ—π’Ž
1-8 The longest connecting wires in a digital system are about 20cm. Assuming the speed of
light, determine the shortest acceptable pulse width based on the 10% rule.
𝑑1 =
𝑑
0.2π‘š
=
= 66.6π‘₯10−8 𝑠 = πŸ”πŸ”π’π’”
𝑐 3π‘₯108 π‘š/𝑠
Juan Carlos Torres
𝑑1 = 10% π‘₯ 𝑀 =
𝑑1
66.6π‘₯10−8 𝑠
𝑀=
=
= πŸ”πŸ”πŸ”π’π’”
10%
0.1
1-9 A communication system operates at a frequency of 800MHz. Assuming the speed of light,
determine the length of connecting line that could be used without considering frequency-domain
effects based on the 10% rule.
πœ†=
𝑐
3π‘₯108 π‘š/𝑠
=
= πŸ‘πŸ•πŸ“π’Žπ’Ž
𝑓 800π‘₯106 𝐻𝑧
1-10 The length of a connecting cable between two points in a radio-frequency system is 50cm.
Assuming the speed of light, determine the highest operating frequency that should be used
without considering frequency-domain effects based on the 10% rule.
𝑐
πœ†=
𝑓
𝑐 3π‘₯108 π‘š/𝑠
𝑓= =
= πŸ”πŸŽπŸŽπ‘΄π‘―π’›
πœ†
0.5
1-11 In a coil, a current of 100mA results in a magnetic flux of 50μWb. Determine the
inductance.
𝐻=
𝛽 50πœ‡π‘Šπ‘ 50π‘₯10−6 π‘Šπ‘
=
=
= 𝟎. πŸ“π‘―
𝐼 100π‘šπ΄ 100π‘₯10−3 𝐴
1-12 A current of 4mA is flowing in a 20μH coil. Determine the magnetic flux.
𝐻=
𝛽
𝐼
𝛽 = 𝐻π‘₯𝐼 = (20π‘₯10−6 𝐻)π‘₯(4π‘₯10−3 𝐴) = πŸ–πŸŽπ’π‘Ύπ’ƒ
1-13 In a capacitor, a voltage of 20 V results in charges storages of 5μC. Determine the
capacitance.
𝐹=
π‘β„Žπ‘Žπ‘Ÿπ‘”π‘’(𝑐)
5π‘₯10−6 πΆπ‘œπ‘™
=
= πŸπŸ“πŸŽπ’π‘­
π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’ (𝑉)
20𝑉
1-14 A capacitance of 40μF is charged to a voltage of 12V. Determine the electric charge.
𝐹=
π‘β„Žπ‘Žπ‘Ÿπ‘”π‘’(𝑐)
π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’ (𝑉)
𝑐 = 𝐹 π‘₯ 𝑉 = (40π‘₯10−6 𝐹)π‘₯(12𝑉) = πŸ’πŸ–π’Žπ‘ͺ𝒐𝒍
1-15 A lossless transmission line has an inductance of 320 nH/m and a capacitance of 57pF/m.
Determine the characteristic impedance.
Juan Carlos Torres
𝐿
320π‘₯10−9 𝐻/π‘š
π‘…πœŠ = √ = √
= √5614 = πŸ•πŸ’. πŸ—πŸπ›€
𝐢
57π‘₯10−12 𝐹/π‘š
1-16 A lossless transmission line has an inductance of 1.2 μH/m and a capacitance of 15pF/m.
Determine the characteristic impedance.
𝐿
1.2π‘₯10−9 𝐻/π‘š
π‘…πœŠ = √ = √
= √80000 = πŸπŸ–πŸ. πŸ–πŸ’π›€
𝐢
57π‘₯10−12 𝐹/π‘š
1-17 The dielectric constant of mica is 6. Determine the permittivity.
∈=∈π‘Ÿ π‘₯ ∈° = 6 π‘₯ (8.842π‘₯10−12 𝐹/π‘š) = πŸ“πŸ‘. πŸŽπŸ“πŸ π’™πŸπŸŽ−𝟐 𝑭/π’Ž
1-18 The permittivity of a material is 14x10-12F/m. Determine the dielectric constant.
∈=∈π‘Ÿ π‘₯ ∈°
∈
14π‘₯10−12 𝐹/π‘š
∈π‘Ÿ = =
= 𝟏. πŸ‘πŸ“
∈° 8.842π‘₯10−12 𝐹/π‘š
1-19 The relative permeability of nickel is 800. Determine the actual permeability.
πœ‡ = πœ‡π‘Ÿ π‘₯ πœ‡πœŠ = 800 π‘₯ (4πœ‹π‘₯10−7 𝐻/π‘š) = πŸπ’Žπ‘―/π’Ž
1-20 The permeability of a ferromagnetic material is 10-4H/m. Determine the relative
permeability.
πœ‡ = πœ‡ π‘Ÿ π‘₯ πœ‡πœŠ
πœ‡π‘Ÿ =
πœ‡
10−4 𝐻/π‘š
=
= πŸ•πŸ—πŸ“. πŸ•πŸ–
πœ‡° 4πœ‹π‘₯10−7 𝐻/π‘š
1-21 Determine the velocity of propagation of the transmission line of Problem 1-15.
𝑉=
1
√𝐿π‘₯𝐢
=
1
√(320π‘₯10−9 𝐻/π‘š)π‘₯(57π‘₯10−12 𝐹/π‘š)
= 𝟐. πŸ‘πŸ’π’™πŸπŸŽπŸ– π’Ž/𝒔
1-22 Determine the velocity of propagation of the transmission line of Problem 1-16.
𝑉=
1
√𝐿π‘₯𝐢
=
1
√(1.2π‘₯10−6 𝐻/π‘š)π‘₯(15π‘₯10−12 𝐹/π‘š)
= 𝟐. πŸ‘πŸ“π’™πŸπŸŽπŸ– π’Ž/𝒔
Juan Carlos Torres
1-23 The dielectric constant in a transmission line is 4.7, and μ=μo. Determine the velocity of
propagation.
∈=∈π‘Ÿ π‘₯ ∈° = 4.7 π‘₯ (8.842π‘₯10−12 𝐹/π‘š) = 41.55 π‘₯10−2 𝐹/π‘š
𝑉=
πœ‡ = πœ‡πœŠ = (4πœ‹π‘₯10−7 𝐻/π‘š)
1
1
1
1
=
=
=
√πœ‡π‘₯πœ– √(4πœ‹π‘₯10−7 𝐻/π‘š)π‘₯(41.55 π‘₯10−2 𝐹/π‘š) √5.22 π‘₯10−17 7.22 π‘₯10−9
= 𝟏. πŸ‘πŸ–π’™πŸπŸŽπŸ– π’Ž/𝒔
1-24 The dielectric constant in a transmission line 3, and μ=μo. Determine the velocity of
propagation.
∈=∈π‘Ÿ π‘₯ ∈° = 3 π‘₯ (8.842π‘₯10−12 𝐹/π‘š) = 26.52 π‘₯10−2 𝐹/π‘š
𝑉=
πœ‡ = πœ‡πœŠ = (4πœ‹π‘₯10−7 𝐻/π‘š)
1
1
1
1
=
=
=
√πœ‡π‘₯πœ– √(4πœ‹π‘₯10−7 𝐻/π‘š)π‘₯(26.52 π‘₯10−2 𝐹/π‘š) √3.33 π‘₯10−17 5.77 π‘₯10−9
= 𝟏. πŸ•πŸ‘π’™πŸπŸŽπŸ– π’Ž/𝒔
1-25 A coaxial cable has the following specifications: Ro=73Ω, and velocity of propagation is
2.1x108m/s. Determine L and C.
𝐿=
𝐢=
π‘…πœŠ
73Ω
=
= πŸ‘. πŸ’πŸ• π’™πŸπŸŽ−πŸ• 𝑯/π’Ž
8
𝑉
2.1 π‘₯10 π‘š/𝑠
1
1
=
= πŸ”πŸ“. πŸπŸ“ π’™πŸπŸŽ−𝟏𝟐 𝑭/π’Ž
π‘…πœŠ 𝑉 73Ω x (2.1 π‘₯108 π‘š/𝑠)
1-26 A transmission line has the following specifications: Ro=150Ω, and velocity of propagation
is 0.8. Determine L and C.
𝑉𝑓 =
𝑉
𝑐
𝑉 = 𝑉𝑓 π‘₯ 𝑐 = 0.8 π‘₯ (3π‘₯108 ) = 2.4π‘₯108 π‘š/𝑠
𝐿=
𝐢=
π‘…πœŠ
150Ω
=
= πŸ“. πŸ‘πŸ“ π’™πŸπŸŽ−πŸ• 𝑯/π’Ž
𝑉
2.4 π‘₯108 π‘š/𝑠
1
1
=
= πŸπŸ•. πŸ•πŸ“ π’™πŸπŸŽ−𝟏𝟐 𝑭/π’Ž
8
π‘…πœŠ 𝑉 150Ω x (2.4 π‘₯10 π‘š/𝑠)
Juan Carlos Torres
1-27 The lower end of the commercial amplitude-modulation (AM) band is about 550KHz. AM
stations use "quarter-wave" vertical antennas whose lengths are 0.25λ. Determine the length in
meters of a vertical antenna operating at the lower end.
πœ†=
𝑐
𝑓
3π‘₯108 π‘š/𝑠
= 545.45π‘š
550π‘₯103 𝐻𝑧
0.25πœ† =
0.25πœ† = 545.45π‘š
πœ†=
545.45π‘š
= πŸπŸπŸ–πŸŽπ’Ž
0.25
1-28 The upper end of the commercial AM band referred to in Problem 1-27 is about 1610KHz.
Determine the length in meters of a vertical antenna operating at the upper end.
3π‘₯108 π‘š/𝑠
0.25πœ† =
= 186.3π‘š
1610π‘₯103 𝐻𝑧
𝑐
πœ†=
𝑓
0.25πœ† = 186.3π‘š
πœ†=
186.3π‘š
= πŸ•πŸ’πŸ“π’Ž
0.25
1-29 One popular simple antenna is the "half-wave" horizontal antenna whose theoretical length
is 0.5λ at the operating frequency. In practice, however, the antenna is usually shorted by about
5% due to end effects. Determine the practical length in meters for a half-wave antenna to
provide optimum reception at the lower end of the commercial FM band, which is about 88 MHz
πœ†=
𝑐
𝑓
0.5πœ† = 186.3π‘š
πœ† = 3.4π‘š π‘₯ 0.05 = 0.17
πœ†=
3π‘₯108 π‘š/𝑠
= 3.4π‘š
88π‘₯103 𝐻𝑧
πœ†=
186.3π‘š
= 372.6π‘š
0.5
πœ† = 3.4π‘š π‘₯ 0.17 = πŸ‘. πŸπŸπ’Ž
1-30 Based on the discussion of Problem 1-29, determine the practical length in meters for a
half-wave antenna to provide optimum reception at the upper end of the FM band, which is about
108MHz.
πœ†=
𝑐
𝑓
πœ†=
3π‘₯108 π‘š/𝑠
= 2.77π‘š
108π‘₯103 𝐻𝑧
πœ† = 5.55π‘š π‘₯ 0.05 = 0.27
πœ†=
2.77
= 5.55π‘š
0.5
πœ† = 5.55π‘š π‘₯ 0.27 = πŸ“. πŸπŸ•π’Ž
Juan Carlos Torres
1-31Show that the free-space velocity of light in feet/second is very close to c=982x106ft/s.
3π‘₯108 π‘š
𝑐 = 3π‘₯108 π‘š/𝑠
1𝑓𝑑 = π‘š π‘₯ 3.2808
? 𝑓𝑑 =
𝑠
1π‘š
1-32 Show that the free-space wavelength in feet can be expressed as
πœ†(𝑓𝑑) =
𝑐
982
=
𝑓 𝑓(π‘šπ»π‘§)
𝑐 984.25197π‘₯106 𝑓𝑑 10−6 πŸ—πŸ–πŸ’. πŸπŸ“π’‡π’•
πœ†= =
π‘₯
=
𝑓
𝑓(𝐻𝑧)
106
𝒇(𝑴𝒛)
You may use the result of Problem 1-31
= πŸ—. πŸ–πŸ’πŸπŸ“π’™πŸπŸŽπŸ–
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