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Helical Antenna
Broad Spectrum of Types
• Helical
• Log Periodic
• Biconical
• Sleeve
• Spiral
Definition
• A helical antenna is an antenna consisting of a
conducting wire wound in the form of a helix.
• In most cases, helical antennas are mounted over a
ground plane.
• Provide circularly polarized wave
• Its polarization and radiation properties depend on
– Diameter
– Pitch
– No. of turns
– Wavelength
– Spacing between the helical loops
Helical Antenna
• Directional
• Circularly Polarized
– Polarization changes
with time
• Both high gain and wide
band
Geometry
D= diameter of helix
C= circumference of helix
Lo= length of one turn =
α= pitch angle =
S= spacing between turns
N= number of turns
L= length of helix
2a or d= diameter of
conductor
Helical Antenna
• (a) Basic geometry
• (b) axial-mode type yielding an endfire pattern and
• (c) omnidirectional mode yielding a broad-side pattern
Associated dimensions
• D - Diameter of the helix; (and, C = πD: Circumference of the
helix)
• s - Spacing between turns (centre-to-centre)
• L - Length of a single turn
• A - Axial length of the helix (= N × s, with N = Number of turns)
• d - Diameter of the helix conductor
• The other dimensions of importance are:
– the distance of the helix from
– the ground plane and the diameter of the (finite-sized) ground-plane.
– The pitch angle (α) of the helix is equal to [arctan(s/πD)]. Angle
between a line tangent to the helix wire and the plane normal to the
helix axis.
α = tan-1 (s/πD)
Operating modes
• 1. Transmission mode
– EM wave propagating along its length
• 2. Radiation mode
– specific far-field pattern
– normal/broad-side type (R0 mode)
– axial/end-fire type (R1mode)
Normal (broadside) mode
• The field maximum occurs in a direction
normal to the helix axis
• The radiation field will be circularly polarized.
• This normal mode occurs if the dimensions of
the helix are small compared to a wavelength
• It bears neither a wideband nor a high
efficiency capability.
Normal Mode
• Radiation pattern similar to
linear dipole
• The dimensions of the helix
are small compared to the
wavelength
• Narrow in bandwidth
• Radiation efficiency is small
• Rarely used
Antenna Theory, Constantine A. Balanis
Axial (or end-fire) mode
• The field will be maximum in the direction of
the helix axis and it will be circularly (or near-
circularly) polarised
• It occurs whenever the helix circumference is
of the order of a wavelength.
• It persists over a fairly wide frequency range
Axial Mode
• Circular Polarization
– ¾<C/λ<4/3
– C/λ=1:near optimum
– S= λ/4
• Half-Power Beam width: 50 x 50 degrees
• Directivity:
• Typical Gain: 10dB
• Bandwidth: 52%
• Frequency limit: 100MHZ to 3GHz
NS
C
2
3
52
3
2
15

S
C
N
Transmission mode - To-mode
• Describe how an electromagnetic wave propagates along
an infinitely long helix.
• In the lowest transmission mode (To-mode), a helix has
adjacent regions of positive and negative charge
separated by many turns.
• It occurs when the length L of one turn of the helix is
small as compared to the wavelength λ (that is, L << λ).
Transmission mode- To-mode
• Important mode on the helix used in the
travelling-wave devices such as the travelling
wave tube.
• In a traveling-wave tube, this transmission
mode field is deliberately excited to interact
with an electron.
Transmission mode- T1-mode
• When the helix circumference, expressed in free-
space wavelength, is of the order of one wavelength
(that is, as C/λ → 1)
• T1-mode. For small pitch angles, it has regions of
adjacent positive and negative charge separated
approximately by half a turn.
Transmission mode- T2 andT3-mode
• Higher-order transmission modes
• For small pitch angles, the approximate charge
distribution around the helix for such modes are
shown in Figure.
Radiation modes R0 mode
• For a short helix (NL << λ), the current may be
assumed to be of uniform magnitude and in
phase along the helix, and it may further be
assumed that a T0-mode is propagating.
• Helix radiates with the maximum field in a
direction normal to the helix axis as shown in
Figure(a)- designated as R0-mode
Radiation patterns of helices
(a) Normal mode (R0) (b) axial mode (R1) and (c) a
multilobed pattern
Radiation modes R1 mode
• With C/λ is of the order of a wavelength and as a T1-
transmission mode propagates along the helix, the
corresponding radiation from the helix is referred to
as the R1-mode
• The field maximum in the axial direction as shown in
Figure (b)
• A helix radiating in this axial mode is usually called a
helical beam antenna.
• Figure (c) shows a corresponding multi lobed pattern
for a helix of large dimensions.
Helix Applications
• Space Telemetry Applications of satellites,
space probes, and ballistic missiles
– Signals have undergone Faraday rotation
• Directional applications
Early Helix – 2 x 10 Turns
1989
2 x 15 Turn 70 cm Helix
1991
AO-13 Antennas
About 1994
AO-40 Antennas
2001
13 and 23 cm Helix Arrays
2003
Gain & Directivity
• An antenna may be very directive i.e. exhibit a
narrow forward beam width but due to the
configuration of the side lobes and/or degree
of losses, provide higher or lower forward gain
Kraus 12.5 cm-Increased Turns
6.5 turns 12 turns
26 turns 52 turns

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Helical.pptan antenna consisting of a conducting wire wound in the form of a helix.

  • 2. Broad Spectrum of Types • Helical • Log Periodic • Biconical • Sleeve • Spiral
  • 3. Definition • A helical antenna is an antenna consisting of a conducting wire wound in the form of a helix. • In most cases, helical antennas are mounted over a ground plane. • Provide circularly polarized wave • Its polarization and radiation properties depend on – Diameter – Pitch – No. of turns – Wavelength – Spacing between the helical loops
  • 4. Helical Antenna • Directional • Circularly Polarized – Polarization changes with time • Both high gain and wide band
  • 5. Geometry D= diameter of helix C= circumference of helix Lo= length of one turn = α= pitch angle = S= spacing between turns N= number of turns L= length of helix 2a or d= diameter of conductor
  • 6. Helical Antenna • (a) Basic geometry • (b) axial-mode type yielding an endfire pattern and • (c) omnidirectional mode yielding a broad-side pattern
  • 7. Associated dimensions • D - Diameter of the helix; (and, C = πD: Circumference of the helix) • s - Spacing between turns (centre-to-centre) • L - Length of a single turn • A - Axial length of the helix (= N × s, with N = Number of turns) • d - Diameter of the helix conductor • The other dimensions of importance are: – the distance of the helix from – the ground plane and the diameter of the (finite-sized) ground-plane. – The pitch angle (α) of the helix is equal to [arctan(s/πD)]. Angle between a line tangent to the helix wire and the plane normal to the helix axis. α = tan-1 (s/πD)
  • 8. Operating modes • 1. Transmission mode – EM wave propagating along its length • 2. Radiation mode – specific far-field pattern – normal/broad-side type (R0 mode) – axial/end-fire type (R1mode)
  • 9. Normal (broadside) mode • The field maximum occurs in a direction normal to the helix axis • The radiation field will be circularly polarized. • This normal mode occurs if the dimensions of the helix are small compared to a wavelength • It bears neither a wideband nor a high efficiency capability.
  • 10. Normal Mode • Radiation pattern similar to linear dipole • The dimensions of the helix are small compared to the wavelength • Narrow in bandwidth • Radiation efficiency is small • Rarely used Antenna Theory, Constantine A. Balanis
  • 11. Axial (or end-fire) mode • The field will be maximum in the direction of the helix axis and it will be circularly (or near- circularly) polarised • It occurs whenever the helix circumference is of the order of a wavelength. • It persists over a fairly wide frequency range
  • 12. Axial Mode • Circular Polarization – ¾<C/λ<4/3 – C/λ=1:near optimum – S= λ/4 • Half-Power Beam width: 50 x 50 degrees • Directivity: • Typical Gain: 10dB • Bandwidth: 52% • Frequency limit: 100MHZ to 3GHz NS C 2 3 52 3 2 15  S C N
  • 13. Transmission mode - To-mode • Describe how an electromagnetic wave propagates along an infinitely long helix. • In the lowest transmission mode (To-mode), a helix has adjacent regions of positive and negative charge separated by many turns. • It occurs when the length L of one turn of the helix is small as compared to the wavelength λ (that is, L << λ).
  • 14. Transmission mode- To-mode • Important mode on the helix used in the travelling-wave devices such as the travelling wave tube. • In a traveling-wave tube, this transmission mode field is deliberately excited to interact with an electron.
  • 15. Transmission mode- T1-mode • When the helix circumference, expressed in free- space wavelength, is of the order of one wavelength (that is, as C/λ → 1) • T1-mode. For small pitch angles, it has regions of adjacent positive and negative charge separated approximately by half a turn.
  • 16. Transmission mode- T2 andT3-mode • Higher-order transmission modes • For small pitch angles, the approximate charge distribution around the helix for such modes are shown in Figure.
  • 17. Radiation modes R0 mode • For a short helix (NL << λ), the current may be assumed to be of uniform magnitude and in phase along the helix, and it may further be assumed that a T0-mode is propagating. • Helix radiates with the maximum field in a direction normal to the helix axis as shown in Figure(a)- designated as R0-mode
  • 18. Radiation patterns of helices (a) Normal mode (R0) (b) axial mode (R1) and (c) a multilobed pattern
  • 19. Radiation modes R1 mode • With C/λ is of the order of a wavelength and as a T1- transmission mode propagates along the helix, the corresponding radiation from the helix is referred to as the R1-mode • The field maximum in the axial direction as shown in Figure (b) • A helix radiating in this axial mode is usually called a helical beam antenna. • Figure (c) shows a corresponding multi lobed pattern for a helix of large dimensions.
  • 20. Helix Applications • Space Telemetry Applications of satellites, space probes, and ballistic missiles – Signals have undergone Faraday rotation • Directional applications
  • 21. Early Helix – 2 x 10 Turns 1989
  • 22. 2 x 15 Turn 70 cm Helix 1991
  • 25. 13 and 23 cm Helix Arrays 2003
  • 26. Gain & Directivity • An antenna may be very directive i.e. exhibit a narrow forward beam width but due to the configuration of the side lobes and/or degree of losses, provide higher or lower forward gain
  • 27. Kraus 12.5 cm-Increased Turns 6.5 turns 12 turns 26 turns 52 turns