I lags/leads V by an angle ϕ and lags behind Er, by an angle Ɵ. Ɵ = tan-1 (Xs /Ra)
TORQUE
EQUATION OF THE SYNCHRONOUS MOTOR
OL
= Supply voltage/phase
I
= Armature current
LM
= Back emf at a load angle of δ
OM
= Resultant voltage, ER
Er
= IZs(or I Xs if Ra is negligible)
I
lags/leads V by an angle ϕ and lags behind Er, by an angle Ɵ.
Ꮎ = tan-1
(Xs /Ra)
✓ Line NS is drawn at angle ϕ to LM
✓ LN and QS are perpendicular to NS
✓ Mechanical power developed per phase in
the rotor,
Pmech
=EbI cos Ψ
Δ
OMS, MS = I Zs cos Ψ
MS
= NS - NM = LQ - NM
I
Zs cos Ψ = Vcos (Ɵ - δ) - Eb cos Ɵ
(or) I cos Ψ = V/Zs cos (Ɵ - δ) - Eb/Zs
cos Ɵ
Pmech/phase
= Eb [V/Zs cos (Ɵ - δ) - Eb/Zs cos
Ɵ]
Pmech/phase
= EbV/Zs cos (Ɵ - δ) - Eb2/Zs
cos Ɵ]
✓ This is the expression for the mechanical power developed
in terms of load angle (α) and the internal angle of the motor for a constant
voltage V & Eb.
✓ Condition for maximum power developed can be found
by differentiating the above expression with respect to load angle and then
equating it is zero.
sin
(Ɵ - δ) = 0 (or) Ɵ = δ
Value
of maximum power,
This shows that the maximum power and hence torque depends on V and Eb that is excitation.
Maximum
value of Ꮎ
and hence α is 90° for all values of V and Eb, this limiting value of
α is the same but maximum torque will be proportional to the maximum power
developed.
If
Ra is neglected, then Zs = Xs and Ɵ = 90°.
COS
Ɵ = 0
This
gives the value of mechanical power developed in terms of δ - the basic
variable of a synchronous machine.
Pmech(max)
= EbV/Xs when (δ = 90°)
This
corresponds to the 'pull out' torque.
To
determine the value of exitation or induced emf Eb to give maximum
power developed possible, differentiate with respect to Eb and equal
to zero.
Where
Ra
→ eflective resistance of the motor
Hence
(P mech)max = V2/4Ra
Basic Electrical and Electronics Engineering: Unit II: Electrical Machines : Tag: : - Torque Equation of the Synchronous Motor
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