UNIT 1: ELECTRICAL DRIVES – FUNDAMENTALS AND CONTROL TECHNIQUES
1. INTRODUCTION AND BASIC CONCEPTS
Definition: An electrical drive is a system that uses electrical energy to control the motion and torque of a motor for a specific load. It provides precise speed, position, and torque control.
Need: Replaces mechanical drives with advantages like:
-
Flexible control (wide speed range, quick response)
-
Energy efficiency (especially in variable load applications)
-
Automatic control and remote operation
-
Regenerative braking capability
-
Better power-to-weight ratio
Block Diagram:
[Power Supply] → [Power Converter] → [Electric Motor] → [Load]
↑ ↑ ↑
[Controller] ← [Sensors/Feedback]
-
Power Supply: AC mains or DC source.
-
Power Converter: Converts supply power to required voltage/current/frequency (e.g., rectifier, chopper, inverter).
-
Electric Motor: Converts electrical to mechanical energy (DC, IM, SM, special motors).
-
Load: The mechanical system being driven (fans, pumps, conveyors, etc.).
-
Controller: Generates switching signals for converter based on reference and feedback.
-
Sensors: Measure current, speed, position (encoders, tachogenerators, Hall sensors).
Classification:
| Basis | Types |
|---|---|
| Motor Type | DC drives, AC drives (IM, SM, PMSM, SRM) |
| Converter Type | Phase-controlled (AC-DC, AC-AC), Chopper-controlled (DC-DC), Inverter (DC-AC) |
| Quadrant Operation | One-quadrant (forward motoring), Two-quadrant (forward/reverse motoring), Four-quadrant (motoring & braking both directions) |
| Supply | AC fed, DC fed |
Advantages over Mechanical Drives:
-
Smooth speed control over wide range.
-
High efficiency at part-load.
-
Automatic fault protection.
-
Remote control and automation compatibility.
-
Energy recovery during braking.
Four-Quadrant Operation:
-
Quadrant I: Forward motoring ($$\displaystyle \omega > 0 $$, $$\displaystyle T > 0 $$)
-
Quadrant II: Forward braking ($$\displaystyle \omega > 0 $$, $$\displaystyle T < 0 $$)
-
Quadrant III: Reverse motoring ($$\displaystyle \omega < 0 $$, $$\displaystyle T < 0 $$)
-
Quadrant IV: Reverse braking ($$\displaystyle \omega < 0 $$, $$\displaystyle T > 0 $$)
-
**Two-quadrant drives:**通常用于提升机、机床(需正反转但制动能量小)。
-
Four-quadrant drives: 用于起重机、电梯、轧机(需快速制动和反转)。
Typical Load Requirements:
-
Constant Torque Loads: Conveyors, extruders ($$\displaystyle T_L \propto \text{constant} $$).
-
Constant Power Loads: Machine tools (milling, drilling) ($$\displaystyle T_L \propto 1/\omega $$).
-
Fan/Pump Loads: $$\displaystyle T_L \propto \omega^2 $$, $$\displaystyle P \propto \omega^3 $$.
2. DC MOTOR DRIVES
2.1 DC Motor Characteristics
Types:
-
Separately Excited: $$\displaystyle V_f $$ independent of $$\displaystyle V_a $$ → easy control, used in drives.
-
Shunt: $$\displaystyle V_f = V_a $$ → constant speed characteristic.
-
Series: $$\displaystyle I_f = I_a $$ → high starting torque, variable speed.
-
Compound: Cumulative (high starting torque, better speed regulation) or differential (constant speed).
Torque-Speed Equation (Separately Excited):
$$ T = K_t \phi I_a \quad \text{and} \quad E_b = K_e \phi \omega_m = V_a - I_a R_a $$
$$ \Rightarrow \omega_m = \frac{V_a}{K_e \phi} - \frac{R_a}{K_e K_t \phi^2} T $$
-
Linear torque-speed characteristic for constant $\phi$.
-
Effect of Armature Reaction: Demagnetizing effect reduces flux $\phi$ at high torque → speed rises slightly.
Basic Speed Control:
-
Armature Voltage Control ($$\displaystyle V_a $$): Speed $$\displaystyle \propto V_a $$. Used for speeds below base speed ($$\displaystyle \phi = \text{rated} $$). Requires variable voltage supply (converter/chopper).
-
Field Control ($$\displaystyle I_f $$): Speed $\propto 1/\phi$. Used for speeds above base speed ($$\displaystyle V_a = \text{rated} $$). Reduces flux → reduced torque capability (constant power region).
[!TIP]
Armature control gives constant torque capability; field control gives constant power capability. Never use field weakening at low speeds (risk of instability).
2.2 Converter-Fed DC Drives
Single-Phase Semi-Controlled Converter (Half-Controlled)
-
Circuit: Two SCRs (T1, T2) and two diodes (D1, D2) in bridge configuration.
-
Operation: SCRs fired at angle $\alpha$ ($0 \le \alpha \le \pi$). Freewheeling diode (FD) across motor armature allows current continuity.
-
Waveforms: Output voltage $$\displaystyle V_{dc} $$ has positive half-cycles only; current continuous due to FD.
-
Average Output Voltage:
$$ V_{dc} = \frac{V_m}{\pi} (1 + \cos \alpha) \quad \text{(with FD, continuous conduction)} $$
-
Speed: $$\displaystyle \omega_m \propto V_{dc} $$.
-
Discontinuous Conduction: Occurs at high $\alpha$ or low load. $$\displaystyle V_{dc} $$ formula changes; need to calculate extinction angle $\beta$.
Single-Phase Fully Controlled Converter
-
Circuit: Four SCRs (T1–T4).
-
Operation: SCRs fired in pairs (T1,T2 at $\alpha$, T3,T4 at $\alpha+\pi$). Bidirectional power flow possible (regeneration with $$\displaystyle \alpha > 90^\circ $$).
-
Average Output Voltage:
$$ V_{dc} = \frac{2V_m}{\pi} \cos \alpha \quad \text{(continuous conduction)} $$
-
Power Factor: Degrades as $\alpha$ increases (displacement and distortion).
-
Harmonics: Rich in odd harmonics (5th, 7th, ...).
[!TIP]
Semi-controlled converters cannot regenerate (unidirectional current). Fully controlled converters can regenerate by firing $$\displaystyle \alpha > 90^\circ $$, making $$\displaystyle V_{dc} $$ negative.
Three-Phase Converters (Overview):
-
Half-wave: Rarely used.
-
Full-wave (bridge): Six SCRs. Better performance (less ripple, higher $$\displaystyle V_{dc} $$).
-
Average Voltage: $$\displaystyle V_{dc} = \frac{3\sqrt{6}}{\pi} V_{LL} \cos \alpha = 1.654 V_{LL} \cos \alpha $$.
2.3 Chopper-Controlled DC Drives
Principle: Switch DC supply ON/OFF rapidly. Time Ratio Control (TRC): Vary duty cycle $$\displaystyle D = T_{ON}/(T_{ON}+T_{OFF}) $$.
Types:
-
Step-down (Buck): $$\displaystyle V_o = D V_{in} $$ (motoring).
-
Step-up (Boost): $$\displaystyle V_o = V_{in}/(1-D) $$ (used in regeneration).
-
Reversible (H-bridge): Four switches; can reverse voltage polarity.
Motoring Control (Buck Chopper):
-
Circuit: Switch (SCR/MOSFET) in series with motor, diode across motor for freewheeling.
-
Operation: Switch ON → motor gets $$\displaystyle V_{in} $$; Switch OFF → motor current freewheels through diode.
-
Average Voltage: $$\displaystyle V_a = D V_{in} $$.
-
Speed Control: $$\displaystyle \omega_m \propto D $$.
Regenerative Braking Control (Boost Chopper):
-
Circuit: Switch (SCR) and diode in series with motor, inductor in parallel.
-
Operation: Motor acts as generator. Switch ON → motor current builds in inductor; Switch OFF → inductor discharges through diode into supply → energy fed back.
-
Average Voltage: $$\displaystyle V_a = V_{in}/(1-D) $$ → $$\displaystyle V_a > V_{in} $$, enabling regeneration.
-
Braking Torque: $$\displaystyle T_b = K_t \phi I_a $$ (opposite to rotation).
Advantages over Converter Drives:
-
Higher efficiency (less switching losses in DC-DC).
-
Faster dynamic response.
-
Simpler control for regeneration.
-
Suitable for battery-powered vehicles (DC source).
2.4 Braking Methods for DC Motors
1. Plugging (Reverse Current Braking)
-
Circuit: Reverse armature polarity while keeping field same. Add external resistance $$\displaystyle R_{ext} $$.
-
Operation: $$\displaystyle V_a $$ reversed → $$\displaystyle E_b $$ and $$\displaystyle V_a $$ additive → high reverse current → high braking torque.
-
Braking Torque: $$\displaystyle T_b = K_t \phi I_{a,b} $$ (negative).
-
Current at start of plugging: $$\displaystyle I_{a,b0} = \frac{V_a + E_{b0}}{R_a + R_{ext}} $$ (very high!).
-
Resistance for current limit: $$\displaystyle R_{ext} = \frac{V_a + E_{b0}}{I_{a,\max}} - R_a $$.
-
Energy: All kinetic energy dissipated in resistors → inefficient.
2. Dynamic Braking
-
Circuit: Disconnect $$\displaystyle V_a $$, connect braking resistor $$\displaystyle R_b $$ across armature. Field remains excited.
-
Operation: Motor acts as generator, energy dissipated in $$\displaystyle R_b $$.
-
Torque-Speed Curve: $$\displaystyle T = -\frac{K_t^2 \phi^2}{R_a+R_b} \omega_m $$ (straight line through origin).
-
Torque zero at $$\displaystyle \omega_m=0 $$ because $$\displaystyle E_b=0 $$ → $$\displaystyle I_a=0 $$ → $$\displaystyle T=0 $$. Motor stops smoothly.
-
Braking time: Depends on inertia and $$\displaystyle R_b $$.
3. Regenerative Braking
-
Condition: $$\displaystyle E_b > V_a $$ (speed high enough for generated voltage to exceed supply).
-
Operation: Power flows from motor to supply. Requires converter that allows reverse power flow (fully controlled converter or chopper with boost mode).
-
Energy: Fed back to supply → efficient.
-
Torque: Negative (braking).
[!TIP]
Comparison:
- Plugging: High torque, high energy loss, used for quick stop (e.g., cranes).
- Dynamic: Medium torque, energy wasted, simple, used for controlled deceleration.
- Regenerative: Energy recovery, requires suitable converter, used in traction/elevators.
2.5 Stability and Dynamic Analysis
Steady-State Stability
-
Criterion: Drive stable if $$\displaystyle \frac{d(T_m - T_L)}{d\omega_m} < 0 $$ at equilibrium point.
-
Interpretation: For small disturbance in speed, net torque should restore equilibrium.
-
Dependence on Characteristics: Stability determined by relative slopes of $$\displaystyle T_m(\omega) $$ and $$\displaystyle T_L(\omega) $$, not individually.
-
If $$\displaystyle T_m $$ curve steeper than $$\displaystyle T_L $$ → stable.
-
If $$\displaystyle T_L $$ steeper → unstable.
-
If equal slopes → marginally stable.
-
Load Equalization:
-
Purpose: Limit peak motor torque during cyclic loads (e.g., punch press) by storing/releasing energy in flywheel.
-
Flywheel Design:
-
Motor torque $$\displaystyle T_m $$ limited to $$\displaystyle T_{m,\max} $$.
-
Load torque $$\displaystyle T_L $$ varies cyclally: $$\displaystyle T_{L1} $$ (high) for $$\displaystyle t_1 $$, $$\displaystyle T_{L2} $$ (low) for $$\displaystyle t_2 $$.
-
Speed variation $\Delta \omega$ determined by energy balance:
-
$$ \text{Energy surplus during light load} = \text{Energy deficit during heavy load} $$
$$ (T_{m,\avg} - T_{L2}) t_2 = (T_{L1} - T_{m,\avg}) t_1 $$
- Flywheel inertia $$\displaystyle J_f $$:
$$ J_f = \frac{(T_{L1} - T_{m,\avg}) t_1}{\Delta \omega} - J_m $$
where $\Delta \omega$ = allowable speed variation (from motor $$\displaystyle T_m-\omega $$ curve).
- Assumptions: Motor $$\displaystyle T_m-\omega $$ linear, losses negligible.
Equilibrium Points & Stability:
Given $$\displaystyle T_m = f(\omega_m) $$ and $$\displaystyle T_L = g(\omega_m) $$:
-
Solve $$\displaystyle f(\omega) = g(\omega) $$ → equilibrium speeds $$\displaystyle \omega_{eq} $$.
-
Compute $$\displaystyle \frac{d}{d\omega}(f-g) $$ at each $$\displaystyle \omega_{eq} $$.
-
If negative → stable; positive → unstable.
Referred Quantities:
-
Refer load inertia to motor side: $$\displaystyle J_{eq} = J_m + J_L \left( \frac{N_m}{N_L} \right)^2 $$
-
Refer load torque: $$\displaystyle T_{L,eq} = T_L \left( \frac{N_m}{N_L} \right) $$
2.6 Starting of DC Motors
Need for Starters:
-
High inrush current: At start, $$\displaystyle E_b=0 $$ → $$\displaystyle I_a = V_a/R_a $$ (5–10× rated).
-
Low starting torque: $$\displaystyle T \propto I_a^2 $$? Actually $$\displaystyle T \propto I_a \phi $$, but high $$\displaystyle I_a $$ may saturate core → $\phi$ constant → $$\displaystyle T \propto I_a $$. Still, high current damages commutator, stresses supply.
Types of Starters:
-
Manual: Series resistors manually stepped.
-
Automatic (Face-plate): Pre-set resistors, contractor sequence.
-
Electronic: Thyristor-based soft starter (ramp up $$\displaystyle V_a $$).
Starting Torque & Current:
- With starting resistor $$\displaystyle R_{st} $$:
$$ I_{a,\max} = \frac{V_a}{R_a + R_{st}} \quad ; \quad T_{st} = K_t \phi I_{a,\max} $$
- Choose $$\displaystyle R_{st} $$ to limit $$\displaystyle I_{a,\max} $$ to 1.5–2× rated.
3. INDUCTION MOTOR DRIVES
3.1 Induction Motor Fundamentals
Construction:
-
Squirrel Cage: Rotor bars short-circuited by end rings → rugged, low cost.
-
Wound Rotor: Three-phase windings connected to slip-rings → allows external rotor resistance insertion.
Equivalent Circuit (Per Phase, Stator Referred):
Rs jXs jXm
V1 ──►──[ ]───[ ]───[ ]───
│ │
│ └───► (Rr'/s) ──[ ]───
│ │
└───────────────┘
-
$$\displaystyle R_s $$: Stator resistance
-
$$\displaystyle X_s $$: Stator leakage reactance
-
$$\displaystyle R_r' $$: Rotor resistance referred to stator
-
$$\displaystyle X_r' $$: Rotor leakage reactance referred to stator
-
$$\displaystyle X_m $$: Magnetizing reactance
Torque-Speed Characteristic:
$$ T = \frac{3}{\omega_s} \frac{V_1^2 (R_r'/s)}{(R_s + R_r'/s)^2 + (X_s + X_r')^2} $$
- Maximum Torque (Breakdown Torque):
$$ T_{max} = \frac{3}{\omega_s} \frac{V_1^2}{2(R_s + \sqrt{R_s^2 + (X_s+X_r')^2})} \approx \frac{3 V_1^2}{2\omega_s X_{eq}} \quad \text{if } R_s \text{ small} $$
-
$$\displaystyle T_{max} \propto V_1^2 $$, independent of $$\displaystyle R_r' $$.
-
Slip at $$\displaystyle T_{max} $$: $$\displaystyle s_{max} = \frac{R_r'}{X_{eq}} $$ (increases with $$\displaystyle R_r' $$).
-
Effect of Rotor Resistance: Shifts $T-s$ curve rightwards → higher starting torque, reduced efficiency.
Influence of Voltage & Frequency:
-
Voltage: $$\displaystyle T \propto V^2 $$ (both $$\displaystyle T_{max} $$ and starting torque).
-
Frequency: $$\displaystyle \omega_s = 120f/P $$. Changing $f$ shifts torque curve horizontally. With constant $V/f$, flux constant → torque capability maintained.
3.2 Variable Frequency Control (V/f Control)
Principle: Maintain constant air-gap flux $$\displaystyle \phi_m $$ to avoid saturation (core loss) and maintain torque capability.
-
Flux $$\displaystyle \phi_m \propto V_1/f $$.
-
So, keep $$\displaystyle V_1/f = \text{constant} $$ below base speed.
Below Base Speed (Constant V/f):
-
$$\displaystyle V_1/f = \text{const} $$ → $$\displaystyle \phi_m = \text{const} $$.
-
Torque equation: $$\displaystyle T \propto \frac{V_1^2}{\omega_s} \cdot \frac{s/R_r'}{(R_s/R_r' + s)^2 + (X_{eq}/R_r')^2} $$
-
Since $$\displaystyle V_1 \propto f $$, $$\displaystyle \omega_s \propto f $$ → $$\displaystyle T \propto f \cdot \frac{s/R_r'}{...} $$.
-
Constant torque region: Can maintain rated current → rated torque up to base speed.
Above Base Speed (Constant Voltage):
-
$$\displaystyle V_1 = \text{rated} $$ (cannot increase beyond insulation limit).
-
$f$ increases → $$\displaystyle V_1/f $$ decreases → $$\displaystyle \phi_m $$ decreases (field weakening).
-
Torque capability decreases: $T \propto 1/f$ (approx) → Constant power region.
-
Speed range: Typically 2:1 to 4:1 above base speed.
Derivation: Max Torque vs Frequency
From torque equation with $$\displaystyle V_1/f = \text{const} $$:
$$ T_{max} = \frac{3}{\omega_s} \frac{V_1^2}{2X_{eq}} \approx \frac{3}{2\omega_s} \frac{(k f)^2}{X_{eq}} = \text{constant} \quad (\text{since } V_1 \propto f, \omega_s \propto f) $$
Thus $$\displaystyle T_{max} $$ constant below base speed.
[!TIP]
For fan/pump loads ($$\displaystyle T_L \propto \omega^2 $$), V/f control gives energy savings at reduced speed because $$\displaystyle P = T\omega \propto \omega^3 $$.
3.3 Stator Voltage Control
Application: Fan/pump loads ($$\displaystyle T_L \propto \omega^2 $$).
-
Method: Reduce $$\displaystyle V_1 $$ using autotransformer or thyristor AC voltage controller.
-
Effect on Torque-Speed: $$\displaystyle T \propto V_1^2 $$, so curve shifts downwards.
-
Speed Reduction: For given $$\displaystyle T_L $$, speed reduces with voltage.
-
Disadvantage: Slip increases → rotor copper loss increases → efficiency low at low speeds.
Numerical Example Approach:
Given motor parameters and load $$\displaystyle T_L = k \omega^2 $$:
-
At rated: $$\displaystyle \omega_{n} $$, $$\displaystyle V_{rated} $$ → find $$\displaystyle k = T_n / \omega_n^2 $$.
-
At reduced speed $\omega$: $$\displaystyle T_L = k \omega^2 $$.
-
From $$\displaystyle T = \frac{3}{\omega_s} \frac{V^2 (R_r'/s)}{(R_s+R_r'/s)^2 + X_{eq}^2} $$, solve for $s$ and $V$ simultaneously (usually iterative).
3.4 Rotor Resistance Control (Wound Rotor IM)
Principle: Insert external resistance $$\displaystyle R_{ext} $$ in rotor circuit via slip-rings.
-
Effect: Increases slip for same torque → speed reduces.
-
Torque-Speed: $$\displaystyle T_{max} $$ unchanged, but $$\displaystyle s_{max} $$ increases.
-
Disadvantage: $$\displaystyle I_r^2 R_{ext} $$ loss in external resistor → efficiency drops.
Closed-Loop Speed Control:
-
Block Diagram:
Speed Ref ──►[Controller]──►[Rotor Resistance Circuit]──►Motor ↑ ↓ └──────────[Speed Sensor]───────┘ -
Operation: PI controller adjusts $$\displaystyle R_{ext} $$ (via converter/contactors) to maintain speed.
Numerical:
Given initial rotor copper loss $$\displaystyle P_{cu2} $$ at slip $$\displaystyle s_1 $$:
$$ P_{cu2} = s \cdot P_{ag} \quad \text{(air-gap power)} $$
With $$\displaystyle R_{r,new} = R_r + R_{ext} $$:
-
New slip for same torque: $$\displaystyle s_2 = s_1 \cdot \frac{R_{r,new}}{R_r} $$.
-
New rotor copper loss: $$\displaystyle P_{cu2,new} = s_2 \cdot P_{ag} = s_1 \cdot \frac{R_{r,new}}{R_r} \cdot P_{ag} = P_{cu2} \cdot \frac{R_{r,new}}{R_r} $$.
3.5 Slip Power Recovery Drives
Static Kramer Drive
-
Power Circuit:
Rotor Slip Rings → Diode Bridge (uncontrolled) → DC Link (inductor L) → Chopper → Fixed DC Source (or Grid via inverter in some versions) -
Operation: Slip power rectified to DC, then fed back to supply via chopper (or to DC source). Rotor resistance effectively increased → speed control below synchronous.
-
Speed Range: $$\displaystyle 0 < s < s_{max} $$ (typically up to 30% below sync speed).
-
Torque-Speed: Similar to rotor resistance control but no external resistor loss → efficient.
-
Closed-Loop: Speed sensor → controller → chopper duty cycle.
Static Scherbius Drive
-
Power Circuit:
Rotor → Thyristor Bridge (controlled rectifier) → DC Link → Inverter (thyristor) → Fixed Frequency AC Supply -
Operation: Slip power converted to fixed frequency AC and fed back. Allows super-synchronous operation ($$\displaystyle s < 0 $$) as well.
-
Range: Both sub- and super-synchronous speeds.
-
Comparison with Kramer: Scherbius allows regeneration and wider speed range (including above sync), but more complex (needs inverter).
Conventional Scherbius System (Historical): Used wound rotor with separate converter set connected to grid → bulky, expensive. Scherbius drive is static version.
3.6 Current Source Inverter (CSI) Fed Drives
Power Circuit:
-
DC Link: Large inductor $$\displaystyle L_d $$ to maintain constant current $$\displaystyle I_d $$.
-
Inverter: Thyristors (or GCTs/IGCTs) with forced commutation (or load commutation if motor has high $$\displaystyle X_d $$).
-
Motor: IM with high leakage reactance (to limit di/dt).
Operation:
-
$$\displaystyle I_d $$ constant → torque $$\displaystyle T \propto I_d \cdot \text{power factor} $$.
-
Frequency varied by inverter switching.
-
Advantage: Inherently current-limited → short-circuit proof.
-
Disadvantage: Requires motor with high leakage reactance, poor power factor at high speeds, complex commutation.
Speed Control: Vary frequency while maintaining $$\displaystyle I_d $$ constant (adjust $$\displaystyle V_d $$ via converter).
3.7 AC Dynamic Braking
Two-Lead Connection:
-
Circuit: Disconnect two supply leads from motor, connect them to a resistor $$\displaystyle R_b $$ (across two phases). Supply disconnected.
-
Operation: Motor acts as induction generator. Rotor cuts stator residual flux → generates AC voltage across $$\displaystyle R_b $$ → energy dissipated.
-
Torque-Speed: Braking torque $$\displaystyle T_b \propto \omega_m R_b/(R_b^2 + (sX_{eq})^2) $$? Actually, with two leads, equivalent circuit changes.
-
Characteristic: Braking torque zero at $$\displaystyle \omega_m=0 $$ and at $$\displaystyle \omega_m = \omega_s $$? Actually, maximum braking torque occurs at $$\displaystyle s \approx R_b/X_{eq} $$ (positive slip for generator action?).
-
Note: Requires residual magnetism in rotor (cage motor has it) or initial DC injection.
3.8 Starting of Induction Motors
Direct-On-Line (DOL):
-
Current: $$\displaystyle I_{start} = 5–7 \times I_{rated} $$.
-
Torque: $$\displaystyle T_{start} = 1.5–2.5 \times T_{rated} $$.
-
Used for: Small motors (< 5 kW) where supply capacity is high.
Reduced Voltage Starting:
-
Star-Delta:
-
Start in star: $$\displaystyle V_{phase} = V_{line}/\sqrt{3} $$ → $$\displaystyle I_{start} $$ and $$\displaystyle T_{start} $$ reduce to 1/3.
-
After time, switch to delta.
-
-
Autotransformer:
- Tap at 50%, 65%, 80% → $$\displaystyle I_{start} \propto V^2 $$, $$\displaystyle T_{start} \propto V^2 $$.
-
Stator Resistor/Air-Cooled Reactor:
-
Series impedance limits current.
-
Calculations: For voltage $$\displaystyle V_{applied} $$:
-
$$ I_{start} = \frac{V_{applied}}{Z_{eq}} \quad ; \quad T_{start} \propto V_{applied}^2 $$
4. SYNCHRONOUS MOTOR DRIVES
4.1 Synchronous Motor Fundamentals
Construction:
-
Salient Pole: Large diameter, few poles → hydro generators.
-
Cylindrical (Round Rotor): Small diameter, many poles → turbo generators.
Principle: DC field on rotor locks with rotating stator field → synchronous speed $$\displaystyle \omega_s = 120f/P $$.
-
Torque Production: $$\displaystyle T = \frac{3}{\omega_s} \frac{V E_f}{X_s} \sin \delta $$ (for negligible $$\displaystyle R_a $$), where $\delta$ = load angle.
-
V-Curves: Plot of armature current $$\displaystyle I_a $$ vs field current $$\displaystyle I_f $$ at constant load. Shows power factor variation (over-excited → leading, under-excited → lagging).
4.2 VSI-Fed Synchronous Drives
Block Diagram:
Speed Ref ──►[Controller]──►[PWM Inverter (VSI)]──►Synchronous Motor
↑ ↓
└──────────[Speed/Position Sensor]┘
-
Operation: Inverter provides variable voltage/frequency. $V/f$ controlled to maintain flux.
-
Speed-Torque: Similar to IM V/f control but with synchronous operation (no slip).
-
Regenerative Braking: Motor operates as generator → power flows back through inverter to DC bus → requires regenerative converter (or braking resistor).
4.3 Self-Controlled Synchronous Drives
Load-Commutated Inverter (LCI)
-
Construction: Thyristor bridge (6-pulse or 12-pulse) directly connected to synchronous motor.
-
Commutation: Uses motor back EMF (synchronous motor acts as commutating source). Requires leading power factor → motor over-excited.
-
Switching Scheme: 120° conduction (like thyristor CSI).
-
Advantage: No forced commutation needed → simple for high power.
-
Disadvantage: Requires leading power factor, poor power factor at light loads, low speed operation difficult (back EMF small → commutation fails).
Comparison LCI vs VSI:
| Feature | LCI | VSI |
|---|---|---|
| Commutation | Load-commutated (motor EMF) | Self-commutated (IGBTs/MOSFETs) |
| Power Factor | Leading (over-excited motor) | Can be controlled (PWM) |
| Speed Range | Limited at low speed | Wide (down to zero) |
| Complexity | Simple switches, complex control | Complex PWM, simple control |
| Application | High power, constant speed | General purpose, wide range |
4.4 Variable Frequency Control
Below Base Speed (Constant V/f):
-
$$\displaystyle V/f = \text{const} $$ → constant flux $\phi$.
-
Torque $$\displaystyle T \propto I_a $$ (since $$\displaystyle T \propto \phi I_a \sin \delta $$, $\phi$ const).
-
Can operate at rated current → constant torque region.
Above Base Speed (Constant Voltage):
-
$$\displaystyle V = \text{rated} $$ → $\phi \propto 1/f$ (field weakening).
-
Torque $$\displaystyle T \propto \phi I_a \propto (1/f) I_a $$.
-
To limit $$\displaystyle I_a $$ to rated, $T \propto 1/f$ → constant power region.
Range of Constant Power Operation:
-
Limited by:
-
Current limit: $$\displaystyle I_a \le I_{rated} $$.
-
Voltage limit: $$\displaystyle V \le V_{rated} $$.
-
Stability: $\delta$ must be less than pull-out angle (typically 70°–80°).
-
-
Typically 2:1 to 3:1 above base speed.
4.5 Synchronous Reluctance Motor (SynRM)
Construction: Salient pole rotor without field winding (or with DC excitation for d-axis). $$\displaystyle X_d \ne X_q $$ (difference due to saliency).
-
Torque Production: $$\displaystyle T = \frac{3}{\omega_s} \frac{V^2}{2} \left( \frac{1}{X_q} - \frac{1}{X_d} \right) \sin 2\delta $$
- Reluctance torque due to $$\displaystyle X_d > X_q $$ (d-axis aligned with field, higher reluctance).
-
Control: Adjust load angle $\delta$ via $$\displaystyle I_d $$ and $$\displaystyle I_q $$ (vector control).
-
Power Factor: Can be improved by proper $\delta$.
Numerical Problem (Given $$\displaystyle X_d, X_q $$, Load Torque):
-
Torque equation: $$\displaystyle T = \frac{3}{\omega_s} \frac{V^2}{2} \left( \frac{1}{X_q} - \frac{1}{X_d} \right) \sin 2\delta $$.
-
Solve for $\delta$.
-
Current phasor: $$\displaystyle I = \frac{V}{jX_d \cos \delta + jX_q \sin \delta} $$? Actually, from phasor diagram:
$$ I_d = \frac{V}{X_d} \sin \delta \quad ; \quad I_q = \frac{V}{X_q} \cos \delta - \frac{E_f}{X_d} \text{ (if excited)} $$
For unexcited SynRM, $$\displaystyle E_f=0 $$: $$\displaystyle I_q = \frac{V}{X_q} \cos \delta $$.
-
Line current $$\displaystyle I_L = \sqrt{I_d^2 + I_q^2} $$.
-
Power factor: $$\displaystyle \cos \phi = I_q / I_L $$.
4.6 Starting of Synchronous Motors
Methods:
-
Using Damper Windings (Amortisseur):
-
Damper bars act like squirrel cage → motor starts as IM.
-
At near sync speed ($\approx 95\%$), apply DC field → pull-in into synchronism.
-
Pull-in Torque: Torque at which motor locks into synchronism.
-
-
Using Pony Motor: Small auxiliary motor brings rotor near sync speed.
-
Variable Frequency Starting: Start with low $f$ → smooth acceleration to sync speed.
-
Direct On-Line (with damper): DOL starting, damper provides starting torque.
Why field applied near sync speed?
-
At low speed, back EMF $$\displaystyle E_f $$ small → stator current $$\displaystyle I_a $$ large when field applied (high $$\displaystyle V - E_f $$).
-
Near sync speed, $$\displaystyle E_f \approx V $$ → small inrush current, smooth pull-in.
5. SPECIAL MOTORS AND DRIVES
5.1 Switched Reluctance Motor (SRM)
Construction:
-
Stator: Salient poles with concentrated windings.
-
Rotor: Salient poles, no windings or magnets (laminated iron).
-
Number of poles: Typically 6/4, 8/6, etc. (stator/rotor poles).
Principle of Operation:
-
Torque Production: Due to variation of inductance with rotor position.
-
Inductance $L(\theta)$ maximum when poles aligned (d-axis), minimum when unaligned (q-axis).
-
Energize phase when rotor moves from unaligned to aligned → rising inductance → positive torque.
-
Sequence: Energize phases in sequence to produce continuous rotation.
-
-
Rotor Position Sensing: Hall sensors, resolvers, or sensorless control (using inductance measurement).
Power Converter: Typically asymmetric bridge (4 switches per phase) for independent phase control.
Advantages over IM/SM:
-
Simple, rugged, low cost (no magnets, no windings on rotor).
-
High torque/inertia ratio → good for high acceleration.
-
Wide speed range.
-
Fault tolerant (phase failure still operates).
-
High efficiency at high speeds.
Torque-Speed Characteristics:
-
Low speed: Constant torque region (current limited by voltage).
-
High speed: Constant power (flux weakening by advancing turn-on angle).
5.2 Permanent Magnet Synchronous Motor (PMSM)
Construction:
-
Rotor: Permanent magnets (NdFeB, SmCo) surface-mounted or interior (IPM).
-
Stator: Three-phase windings (similar to SM).
Working Principle:
-
Back EMF $$\displaystyle E \propto \omega \phi_{pm} $$.
-
Torque $$\displaystyle T = \frac{3}{\omega_s} \frac{V E}{\omega_s L_d} \sin \delta + \frac{3}{\omega_s} \frac{3}{2} (L_d - L_q) I_d I_q $$ (for IPM, reluctance torque).
-
Comparison with BLDC: PMSM sinusoidal back EMF, sinusoidal current; BLDC trapezoidal back EMF, rectangular current.
5.3 Brushless DC Motor (BLDC)
Construction:
-
Stator: Three-phase windings.
-
Rotor: Permanent magnets.
-
Electronic Commutator: Position sensors (Hall) + power converter (3-phase bridge).
Operation (Six-Step Commutation):
-
60° conduction per phase.
-
Hall sensors determine rotor position → switch phases in sequence.
-
Torque ripple higher than PMSM.
Switching Scheme:
-
6-step (120°) or sinusoidal (FOC).
-
Drive Circuit: DC bus → 3-phase inverter (MOSFET/IGBT) → motor.
5.4 Stepper Motor
Variable Reluctance Stepper Motor
-
Construction: Stator with multiple phases (e.g., 2-phase), rotor with teeth (no windings).
-
Operation: Energize phases sequentially → rotor aligns to minimum reluctance position.
-
Step Angle: $$\displaystyle \theta_s = \frac{360^\circ}{N_r \cdot N_s} $$? Actually, for VR stepper:
$$ \theta_s = \frac{(N_r - N_s) \times 360^\circ}{N_r N_s} $$
where $$\displaystyle N_r $$ = rotor teeth, $$\displaystyle N_s $$ = stator teeth per phase.
-
Micro-stepping: Divide full step into smaller steps by proportioning phase currents sinusoidally.
-
Example: Half-stepping → alternate between one-phase-on and two-phase-on.
-
Currents: $$\displaystyle I_a = I_m \sin \theta $$, $$\displaystyle I_b = I_m \cos \theta $$ for smooth rotation.
-
Load Angle Control:
-
Torque $$\displaystyle T \propto \sin(\theta_{load}) $$, where $$\displaystyle \theta_{load} $$ = displacement from equilibrium position.
-
Maximum torque at $$\displaystyle \theta_{load} = 90^\circ $$ (pull-out torque).
6. BRAKING METHODS (COMPREHENSIVE)
| Method | Energy Flow | Torque-Speed | Efficiency | Applications |
|---|---|---|---|---|
| Regenerative | Back to supply | Negative torque, extends to $$\displaystyle \omega=0 $$? Actually, regen torque exists at $$\displaystyle \omega>0 $$, but at $$\displaystyle \omega=0 $$, $$\displaystyle E_b=0 $$ → no torque. | High | Traction, elevators, cranes |
| Dynamic | Dissipated in resistor | $T \propto -\omega$ (through origin) | Low | Controlled deceleration |
| Plugging | Dissipated in resistors | High negative torque, independent of $\omega$? Actually, $$\displaystyle T_b \approx \text{const} $$ at start, decreases as $\omega$ drops. | Very Low | Quick stop (emergency) |
DC Motor Braking Calculations (Plugging):
-
Initial braking current: $$\displaystyle I_{b0} = \frac{V_a + E_{b0}}{R_a + R_{ext}} $$
-
Braking torque: $$\displaystyle T_b = K_t \phi I_b $$ (negative).
-
At $$\displaystyle \omega=0 $$, $$\displaystyle E_b=0 $$ → $$\displaystyle I_b = V_a/(R_a+R_{ext}) $$ (still high).
7. STABILITY AND LOAD CHARACTERISTICS
Steady-State Stability Criterion:
For drive with motor torque $$\displaystyle T_m(\omega) $$ and load torque $$\displaystyle T_L(\omega) $$:
-
Equilibrium: $$\displaystyle T_m(\omega) = T_L(\omega) $$.
-
Stable if $$\displaystyle \frac{d(T_m - T_L)}{d\omega} < 0 $$ at equilibrium.
-
Physical Meaning: If speed increases slightly, net torque should become negative (decelerating) to restore equilibrium.
Effect of Characteristics:
-
Stable: $$\displaystyle T_m $$ curve steeper than $$\displaystyle T_L $$.
-
Unstable: $$\displaystyle T_L $$ steeper than $$\displaystyle T_m $$.
-
Marginally stable: Equal slopes.
Load Equalization (Flywheel Design):
Given:
-
Motor torque limit $$\displaystyle T_{m,\max} $$.
-
Load torque $$\displaystyle T_{L1} $$ for time $$\displaystyle t_1 $$, $$\displaystyle T_{L2} $$ for $$\displaystyle t_2 $$ ($$\displaystyle T_{L1} > T_{L2} $$).
-
Motor inertia $$\displaystyle J_m $$, no-load speed $$\displaystyle \omega_0 $$, slip at $$\displaystyle T_{L1} $$? Actually, from linear $$\displaystyle T_m-\omega $$:
$$ T_m = T_{m0} - \frac{T_{m0} - T_{L1}}{\omega_0 - \omega_1} (\omega - \omega_1) \quad \text{?} $$
Standard approach:
-
Average motor torque: $$\displaystyle T_{m,\avg} = \frac{T_{L1} t_1 + T_{L2} t_2}{t_1 + t_2} $$.
-
Energy balance:
$$ \text{Energy stored in flywheel during light load} = \frac{1}{2} (J_m + J_f) (\omega_{max}^2 - \omega_{min}^2) \approx (J_m+J_f) \omega_0 \Delta \omega $$
$$ \text{Energy deficit during heavy load} = (T_{L1} - T_{m,\avg}) t_1 $$
Equate: $$\displaystyle (J_m+J_f) \omega_0 \Delta \omega = (T_{L1} - T_{m,\avg}) t_1 $$
- From motor characteristic, $\Delta \omega$ related to torque deviation:
$$ \Delta T = \frac{R_a}{K_e K_t \phi^2} \Delta \omega \quad \text{or from linear approx:} \quad \Delta \omega = \frac{\Delta T}{K} $$
where $$\displaystyle K = \text{slope of } T_m-\omega $$.
- Given: slip $s$ at torque $T$ → from $$\displaystyle T = K_t \phi I_a $$, and $$\displaystyle I_a = (V_a - K_e \phi \omega)/R_a $$, derive slope.
Example Problem (May 2024):
Given $$\displaystyle T_m = (1+2a_m) $$? That seems odd. Possibly $$\displaystyle T_m = (1+2a)\omega_m $$? Actually, past paper: $$\displaystyle T_m = (1+2a_m) $$ and $$\displaystyle T_l = 3\sqrt{\omega_m} $$. Likely typo? Should be $$\displaystyle T_m = f(\omega_m) $$. Assume $$\displaystyle T_m = a_0 + a_1 \omega_m $$? Let's interpret: Maybe $$\displaystyle T_m = (1 + 2\alpha) \omega_m $$? Not clear. Standard method: equate $$\displaystyle T_m = T_L $$, solve for $\omega$, then check derivative.
8. CLOSED-LOOP AND DIGITAL CONTROL
Closed-Loop Schemes:
-
Static Kramer Drive: Speed sensor → slip power controller (chopper duty cycle) → maintain speed.
-
Scherbius Drive: Speed sensor → inverter frequency/phase control.
-
VSI-Synchronous Drive: Speed/position sensor → current controllers (FOC) → PWM.
Digital Control of Drives:
-
Block Diagram:
Ref ──►[Digital Controller (DSP/FPGA)]──►[PWM Generator]──►[Power Converter]──►Motor ↑ ↓ └──────────[ADC: Current, Speed, Position]┘ -
Advantages:
-
Flexible control algorithms (FOC, DTC).
-
Precise tuning, adaptive control.
-
Diagnostics, communication (fieldbus).
-
Cost-effective for complex control.
-
-
Implementation: Sample times, quantization, anti-aliasing filters.
Constant Torque & Constant Power Operation:
-
Constant Torque: Below base speed (DC: armature control; IM: V/f constant; SM: V/f constant). Maintain rated current.
-
Constant Power: Above base speed (DC: field control; IM: constant V; SM: constant V). Torque inversely proportional to speed.
-
Range: Determined by maximum voltage and current limits, and stability limits (for SM, $$\displaystyle \delta_{max} $$).
9. INDUSTRIAL APPLICATIONS AND SYSTEM CONSIDERATIONS
Cement Industries:
-
Drives: Crushers, mills, fans, conveyors.
-
Requirements: High torque, dusty environment, constant speed (for mills) or variable speed (for fans).
-
Schemes: IM drives with V/f control for fans; DC drives or slip-power recovery for mills (high torque, low speed).
Steel Industries:
-
Drives: Rolling mills (reversing, non-reversing), cranes, conveyors.
-
Requirements: High power (MW), high torque, rapid reversal, regenerative braking.
-
Schemes:
-
Rolling Mills: DC drives (armature control) or slip-power recovery IM drives for wide speed range and regeneration.
-
Cranes: Four-quadrant DC or AC drives with regenerative braking.
-
Electric Traction:
-
Requirements: High starting torque, wide speed range, regenerative braking, ruggedness.
-
DC vs AC: Historically DC (simple control). Now AC (IM with V/f or vector control) for lower maintenance.
-
Control: Series DC motor with rheostatic or chopper control; IM with V/f and vector control.
Group vs Individual Drives:
-
Group Drive: One motor drives multiple machines via line shaft. Advantages: lower cost, simpler. Disadvantages: inefficient, no individual control, all stop if one fails.
-
Individual Drive: Each machine has its own motor. Advantages: flexible, efficient, independent control. Modern trend.
CNC Machines:
-
Axes: Spindle (constant power) and feed axes (servo drives).
-
Drives: AC servo motors (PMSM) with digital controllers, high resolution encoders.
-
Integration: Motion controller coordinates axes, trajectory planning.
Energy Recovery Systems:
-
Principle: Capture kinetic energy during braking and feed back to supply or store.
-
Implementation: Regenerative converters (fully controlled rectifier, active front end), batteries, supercapacitors.
-
Applications: Elevators, cranes, electric vehicles.
10. STARTING AND MISCELLANEOUS TOPICS
Starters for DC Motors:
-
Necessity: Limit starting current, provide sufficient starting torque.
-
Types:
-
Manual: Face-plate starter with series resistors.
-
Automatic: Time-delay relays, current relays to step out resistors.
-
Solid-state: Thyristor-based soft starter (ramp voltage).
-
Conventional Methods (Historical):
-
Starting: Rheostats in armature/field.
-
Braking: Mechanical brakes, plugging.
-
Speed Control: Ward-Leonard (motor-generator set), metadyne, amplidyne.
Two-Phase and Three-Phase Converters:
-
Two-Phase: Rarely used, for special applications.
-
Three-Phase: Common for high power DC drives (6-pulse, 12-pulse to reduce harmonics).
Phase-Controlled vs Chopper-Controlled Drives:
| Aspect | Phase-Controlled | Chopper-Controlled |
|---|---|---|
| Supply | AC | DC (battery, rectified AC) |
| Frequency | Line frequency (50/60 Hz) | High switching (kHz) |
| Ripple | High (100 Hz for single-phase) | Low (depends on switching freq) |
| Regeneration | Possible with full converter | Easy with boost chopper |
| Application | High power AC-fed drives | Battery vehicles, DC sources |
Energy Recovery Systems (Detailed):
-
Regenerative Braking: Motor as generator → power back to AC supply via inverter with regenerative capability (DC bus voltage rise controlled by PWM).
-
Storage: Supercapacitors for short bursts, batteries for longer.
-
Control: During braking, torque command negative, power flow monitored, DC bus voltage regulated.
Slip-Controlled IM Drives:
-
Synonym for slip power recovery drives (Kramer, Scherbius).
-
Control slip frequency/power to adjust speed.
EXAM TIPS:
-
Load Equalization: Always draw torque-time diagram, mark $$\displaystyle T_{m,\max} $$, $\Delta \omega$, use energy balance.
-
Converter Output Voltage: Remember formulas for semi/full converters with/without freewheeling.
-
Braking: Distinguish plugging (reverse voltage), dynamic (resistor across armature), regenerative ($$\displaystyle E_b > V_a $$).
-
V/f Control: Below base: constant $V/f$ → constant torque; above: constant $V$ → constant power.
-
Stability: Always compare slopes of $$\displaystyle T_m $$ and $$\displaystyle T_L $$ at equilibrium.
-
Special Motors: SRM (no magnets/rotor windings), PMSM (sinusoidal), BLDC (trapezoidal, Hall sensors).
KEY FORMULAS BOX:
-
DC Motor Speed: $$\displaystyle \omega_m = \frac{V_a}{K_e \phi} - \frac{R_a}{K_e K_t \phi^2} T $$
-
Semi-Converter $$\displaystyle V_{dc} $$ (with FD): $$\displaystyle V_{dc} = \frac{V_m}{\pi}(1+\cos\alpha) $$
-
Full Converter $$\displaystyle V_{dc} $$: $$\displaystyle V_{dc} = \frac{2V_m}{\pi}\cos\alpha $$
-
Chopper $$\displaystyle V_{avg} $$: $$\displaystyle V_{avg} = D V_{in} $$ (buck), $$\displaystyle V_{avg} = V_{in}/(1-D) $$ (boost)
-
IM Torque: $$\displaystyle T = \frac{3}{\omega_s} \frac{V^2 (R_r'/s)}{(R_s+R_r'/s)^2 + X_{eq}^2} $$
-
IM $$\displaystyle T_{max} $$: $$\displaystyle T_{max} \approx \frac{3 V^2}{2 \omega_s X_{eq}} $$
-
SynRM Torque: $$\displaystyle T = \frac{3}{\omega_s} \frac{V^2}{2} \left( \frac{1}{X_q} - \frac{1}{X_d} \right) \sin 2\delta $$
-
Flywheel Inertia: $$\displaystyle J_f = \frac{(T_{L1} - T_{m,\avg}) t_1}{\Delta \omega} - J_m $$
DIAGRAM REFERENCES:
-
Block Diagram of Electrical Drives:
DiagramSEARCH: "electrical drive block diagram power converter controller" -
Single-Phase Semi-Controlled Converter:
DiagramCANVAS: "Two SCRs (T1,T2) and two diodes (D1,D2) in bridge, freewheeling diode across motor, AC source" -
DC Motor Torque-Speed Characteristics:
DiagramSEARCH: "dc motor torque speed curve armature control field control" -
IM V/f Control Characteristics:
DiagramSEARCH: "induction motor v/f control torque speed curves constant torque constant power" -
Static Kramer Drive Power Circuit:
DiagramCANVAS: "Rotor slip rings → diode bridge → DC link inductor → chopper → DC source" -
SRM Construction:
DiagramSEARCH: "switched reluctance motor stator rotor salient poles" -
Stepper Motor Micro-stepping Currents:
DiagramSEARCH: "stepper motor microstepping sine cosine current waveforms"
END OF UNIT 1 SHORT NOTES