Axial Electric Field and Wave Modes in TWT

Axial Electric Field in TWT:

It defines how the electric field changes with convection current.

Let ‘L’ be the inductance, ‘C’ be the capacitance, ‘I’ be the alternating current, ‘V’ be the alternating voltage and ‘i’ be the convection current. The current flowing is defined by the Equation,

∂I/ ∂z = -C∂V/ ∂t - ∂i/ ∂z -------------------------- (1)

∂/ ∂z = -γ and ∂/ ∂t = jω

Therefore equation (1) becomes,
-γ I = - jωCV + γi ---------------------------- (2)

The voltage across the electric field is defined as,

∂V/ ∂z = -L∂I/ ∂t
-γV = - jωLI
I = γV/ jωL --------------------------- (3)

Sub eq (3) in (1)

2V/ jωL = -jωCV + γi
γ2V = -jωL(-jωCV + γi)
= -CVω2L - jωL γi

When the convection current, i = 0

γ2V = -CVω2L
γ2 = -Cω2L
γ =√(-Cω2L)
γ = jω√(LC)

This equation represents propagation constant γ for an ideal transmission line.

ie, γ0 = jω√(LC)

γ02 = -ω2LC ---------------------------- (4)

When the convection current is not zero,

γ2V = -ω2LCV – γijωL
γ2V + ω2LCV = -γijωL
V(γ2 + ω2LC) = -γijωL
V = -γijωL/(γ2 + ω2LC)

Sub in eqn (4)

V = -γωLij/(γ2 - γ02) ------------------------- (5)

Characteristic impedance,
Zo = √(L/C)

Multiplying both sides by γ0
γ0 Zo = γ0√(L/C)

Sub for γ0 from eq (4)
γ0 Zo = jω√(LC). √(L/C)
= jωL

Sub the value of γ0 Zo in eq (5)
V = -iγ γ0 Z0 /(γ2 - γ02)

The electric field is defined as,

Ez = -∇. V
Ez = -∂V/ ∂z  (we have, ∂/ ∂z = )
Ez = γV

Sub. for V.

Therefore, Ez = 2 γ0 Z0 i/(γ2 - γ02)

This equation is called circuit equation as it determines the electric field from the convection current, i.

Wave Modes in TWT:

The solution for propagation constant ‘γ’ in the electronic and circuit equations provides four distinct solutions. These four solutions represent four modes of propagation in a travelling wave tube. The values of four propagation constants are given by,

γ1 = -βe c √(3/2) + jβe [1 + (c/2)]
γ2 = βe c √(3/2) + jβe [1 + (c/2)]
γ3 = e [1 - c]
γ4 = -e [1 – c3/4]

The wave corresponding to γ1 is a forward wave and its amplitude grows exponentially with distance. The wave corresponding to γ2 is a forward wave whose amplitude decays exponentially. The wave corresponding to γ3 is a forward wave whose amplitude remains constant. The wave corresponding to γ4 is a backward wave whose amplitude remains constant. The growing wave propagates at a velocity slightly lower than electron velocity and energy flows from electron beam to travelling wave. The decaying wave propagates in the same manner as that of the growing wave but the energy flows from travelling wave to electron beam. The constant amplitude wave travels with a velocity higher than electron velocity and no energy transfer occurs. The backward wave propagates in negative z direction with a velocity higher than electron velocity.

Gain Characteristics:

The gain of the travelling wave tube is defined as,

Ap = 10 log |output voltage/input voltage|2
Ap = -9.54 + 47.3 NC dB

Where, N is length and C is gain parameter.

Sreejith Hrishikesan

Sreejith Hrishikesan is a ME post graduate and has been worked as an Assistant Professor in Electronics Department in KMP College of Engineering, Ernakulam. For Assignments and Projects, Whatsapp on 8289838099.

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