homework 1 - City Tech OpenLab

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Juan Carlos Torres
6-1 The voltage between two parallel plates separated by a distance of 5mm is 200V. Determine
the electric field intensity.
𝐸=
𝑉
200 𝑉
=
= πŸ’πŸŽ, 𝟎𝟎𝟎 𝑽/π’Ž
𝑑 0.005 π‘š
6-2 The voltage between two parallel plates separated by a distance for 0.4in is 60V. Determine
the electric field intensity.
1in = 0. 254 m
0.4in = 0.01016
𝐸=
𝑉
60 𝑉
=
= πŸ“, πŸ—πŸŽπŸ“ 𝑽/π’Ž
𝑑 0.01016 π‘š
6-3 The electric field intensity in the region between two parallel plates separated by a distance
of 4cm is 2KV/m. Determine the voltage between the plates.
𝐸=
𝑉
→ 𝑉 = 𝐸 π‘₯ 𝑑 = 2000 π‘₯ 0.04 = πŸ–πŸŽπ‘½
𝑑
6-4 The electric field intensity in the region between two parallel plates separated by a distance
of 8mm is 200V/mm. Determine the voltage between the plates.
𝐸=
𝑉
→ 𝑉 = 𝐸 π‘₯ 𝑑 = 200 π‘₯ 8 = πŸπŸ”πŸŽπŸŽπ‘½
𝑑
6-5 A direct current of 5A is flowing a conductor. Determine the magnetic field intensity at a
distance of 3m from the conductor.
𝐻=
𝐼
5𝐴
=
= πŸπŸ”πŸ“π’Žπ‘¨/π’Ž
2πœ‹π‘‘ 2πœ‹. 3
6-6 A direct current of 4mA is flowing in a conductor. Determine the magnetic field intensity at
a distance of 5ft from the conductor.
1ft = 0.3048m
5ft = 1.524m
𝐻=
𝐼
0.004𝐴
=
= πŸπŸ”πŸ“π’Žπ‘¨/π’Ž
2πœ‹π‘‘ 2πœ‹. 1.524
Juan Carlos Torres
6-7 For the parallel plates of Problem 6-3 determine the electric flux density if the dielectric is
polyethylene (πœ–π‘Ÿ = 2.25).
∈=∈π‘Ÿ π‘₯ ∈° = 2.25 π‘₯ (8.842π‘₯10−12 𝐹/π‘š) = 19.895 π‘₯10−2 𝐹/π‘š
𝐷 =∈ π‘₯ 𝐸 = 19.895 π‘₯10−12 𝐹/π‘š π‘₯ 2000𝑉/π‘šπ‘š = πŸ‘πŸ—. πŸ•πŸ— 𝒏π‘ͺ/π’ŽπŸ
6-8 For the parallel plates of Problem 6-4, determine the electric flux density if the dielectric is
air.
π‘₯10−12 𝐹 200𝑉 1π‘šπ‘š
𝐷 =∈ π‘₯ 𝐸 = 8.84
π‘₯(
π‘₯
) = πŸπŸ•. πŸ”πŸ– 𝝁π‘ͺ/π’ŽπŸ
π‘š
π‘š
0.001
6-9 For the current carrying conductor of Problem 6-5, determine the magnetic flux density at a
distance of 3m from the conductor if the medium is air.
𝐡 = πœ‡ π‘₯ 𝐻 = (1.2566π‘₯10−6 )𝑋(0.265𝐴/π‘š) = πŸ‘πŸ‘πŸπ’π‘ͺ/π’ŽπŸ
6-10 For the current carrying conductor of Problem 6-6, determine the magnetic flux density at a
distance of 5ft from the conductor if the medium is air.
𝐡 = πœ‡ π‘₯ 𝐻 = (1.2566π‘₯10−6 )𝑋(0.0417/π‘š) = πŸ“πŸ. πŸ’π’π‘ͺ/π’ŽπŸ
6-11 The electric flux density normal to a rectangular surface with dimensions 8m x 75cm is
4μC/m2. Determine the value of the electric flux across the area.
πœ“ = 𝐷π‘₯𝐴 = 6π‘š2 π‘₯ 4πœ‡πΆ/π‘š2 = 𝟐. πŸ’ππ‘ͺ
6-12 The electric flux density normal to a circular surface with a diameter of 3m is 8μC/m2.
Determine the value of the electric flux across the area.
𝐴 = πœ‹ π‘₯ π‘Ÿ 2 = 3.14 π‘₯ (1.5)2 = 7.068
πœ“ = 𝐷π‘₯𝐴 = 7.068π‘š2 π‘₯ 8πœ‡πΆ/π‘š2 = 𝟎. πŸ“πŸ”ππ‘ͺ
6-13 The magnetic flux density normal to a circular surface with a radius of 5m is 4nWb/m2.
Determine the value of the magnetic flux across the area.
𝐴 = πœ‹ π‘₯ π‘Ÿ 2 = 3.14 π‘₯ (5)2 = 78.54
πœ™ = 𝐡π‘₯𝐴 = 4π‘›π‘Šπ‘/π‘š2 π‘₯ 78.54π‘š2 = 𝟎. πŸ‘πŸπŸ’ππ‘Ύπ’ƒ
Juan Carlos Torres
6-14 The magnetic flux density normal to a rectangular surface with dimensions 30cm x 60cm is
12nWb/m2. Determine the value of the magnetic flux across the area.
π‘Ž = 𝑏 π‘₯ β„Ž = 30π‘π‘š π‘₯ 60π‘π‘š = 1800π‘π‘š2 π‘œπ‘Ÿ 0.18π‘š2
πœ™ = 𝐡π‘₯𝐴 = 12π‘›π‘Šπ‘/π‘š2 π‘₯ 0.18π‘š2 = 𝟐. πŸπŸ”π’π‘Ύπ’ƒ
6-15 A current of 8A is uniformly distributed over a rectangular conductor with dimensions 5mm
x 4mm. Determine the current density.
π‘Ž = 𝑏 π‘₯ β„Ž = 5π‘šπ‘š π‘₯ 4π‘šπ‘š = 20π‘šπ‘š2 π‘œπ‘Ÿ 2π‘₯10−5 π‘š2
𝐽=
𝐼
8𝐴
=
= πŸ’πŸŽπŸŽπŸŽπŸŽπŸŽπ‘¨/π’ŽπŸ
π‘Ž 2π‘₯10−5 π‘š2
6-16 A current of 4A is uniformly distributed over a circular conductor with a diameter of 3cm.
Determine the current density.
𝐴 = πœ‹ π‘₯ π‘Ÿ 2 = 3.14 π‘₯ (0.15)2 = 7.06π‘₯10−4 π‘š2
𝐽=
𝐼
4𝐴
=
= πŸ“πŸ”πŸ“πŸ–. πŸ–πŸ’π‘¨/π’ŽπŸ
−4
2
π‘Ž 7.06π‘₯10 π‘š
6-17 Assume that the conductivity for the conductor of Problem 6-15 is 5MS/s. Determine the
electric field intensity.
𝐽
400𝐴/π‘š2
𝐸= =
= πŸ–πŸŽππ‘½/π’Ž
𝛿 5π‘₯106 𝑆/π‘š
6-18 Assume that the conductivity for the conductor of Problem 6-16 is 6 x107 S/m. Determine
the electric field intensity.
𝐸=
𝐽 142.85𝐴/π‘š2
=
= 𝟐. πŸ‘πŸ–ππ‘½/π’Ž
𝛿
6π‘₯107 𝑆/π‘š
Juan Carlos Torres
6-19 The rms magnitude of the magnetic field of a plane wave in air is 𝐻𝑦 = 200πœ‡π΄/π‘š.
Assuming the E is in the positive x-direction, determine the following for a circular surface of
diameter 50m in the x-y plane over which the field are constant.
a) Ex
𝐸π‘₯
=πœ‚
𝐻𝑦
𝐸π‘₯ =
πœ‚
377Ω
=
= 1.885𝑀𝑉/π‘š
𝐻𝑦 200πœ‡π΄/π‘š
b) Pz
℘𝑧 =
𝐸π‘₯ 1.885𝑀𝑉/π‘š
=
= 9425π‘€π‘Š/π‘š2
πœ‚
377Ω
c) Total power transmitted through area
𝐴 = πœ‹ π‘₯ π‘Ÿ 2 = 3.14 π‘₯ (25π‘š)2 = 78.58π‘š2
𝑃 = ℘𝑧 π‘₯ 𝐴 = 9425π‘€π‘Š/π‘š2 π‘₯ 78.54π‘š2 = 740π‘€π‘Š
6-20 The rms magnitude of the electric field of a plane wave in a sea water (πœ–π‘Ÿ = 2.25) is Ex =
3V/m. Assuming that H is in the positive y-direction, determine the following for a square
surface with sides of 15m each in the x-y plane over which the fields are constant:
a) Hy
𝐸π‘₯
=πœ‚
𝐻𝑦
𝐻𝑦 =
𝐸π‘₯
3𝑉/π‘š
=
= 7.95π‘šπ΄/π‘š
πœ‚
377Ω
b) Pz
℘𝑧 =
𝐸π‘₯ 3𝑉/π‘š
=
= 23.8π‘šπ‘Š/π‘š2
πœ‚
377Ω
c) Total power transmitted through area
𝐴 = 𝐿2 = (15π‘š)2 = 225π‘š2
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