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EX-801 · Electrical Drives/Quick Revision Short Notes

Electrical Drives (EX-801) - Unit 1 Short Notes

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 $$\displaystyle T_L = g(\omega_m) $$:

  1. Solve $$\displaystyle f(\omega) = g(\omega) $$ → equilibrium speeds $$\displaystyle \omega_{eq} $$.

  2. Compute $$\displaystyle \frac{d}{d\omega}(f-g) $$ at each $$\displaystyle \omega_{eq} $$.

  3. 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 $$\displaystyle T_L = k \omega^2 $$:

  1. At rated: $$\displaystyle \omega_{n} $$, $$\displaystyle V_{rated} $$ → find $$\displaystyle k = T_n / \omega_n^2 $$.

  2. At reduced speed $\omega$: $$\displaystyle T_L = k \omega^2 $$.

  3. 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:

  1. 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.

  2. Autotransformer:

    • Tap at 50%, 65%, 80% → $$\displaystyle I_{start} \propto V^2 $$, $$\displaystyle T_{start} \propto V^2 $$.
  3. 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:

    1. Current limit: $$\displaystyle I_a \le I_{rated} $$.

    2. Voltage limit: $$\displaystyle V \le V_{rated} $$.

    3. 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):

  1. Torque equation: $$\displaystyle T = \frac{3}{\omega_s} \frac{V^2}{2} \left( \frac{1}{X_q} - \frac{1}{X_d} \right) \sin 2\delta $$.

  2. Solve for $\delta$.

  3. 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, $$\displaystyle E_f=0 $$: $$\displaystyle I_q = \frac{V}{X_q} \cos \delta $$.

  1. Line current $$\displaystyle I_L = \sqrt{I_d^2 + I_q^2} $$.

  2. Power factor: $$\displaystyle \cos \phi = I_q / I_L $$.


4.6 Starting of Synchronous Motors

Methods:

  1. 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.

  2. Using Pony Motor: Small auxiliary motor brings rotor near sync speed.

  3. Variable Frequency Starting: Start with low $f$ → smooth acceleration to sync speed.

  4. 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:

  1. Average motor torque: $$\displaystyle T_{m,\avg} = \frac{T_{L1} t_1 + T_{L2} t_2}{t_1 + t_2} $$.

  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: $$\displaystyle (J_m+J_f) \omega_0 \Delta \omega = (T_{L1} - T_{m,\avg}) t_1 $$

  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 $$\displaystyle K = \text{slope of } T_m-\omega $$.

  1. 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:

  1. Load Equalization: Always draw torque-time diagram, mark $$\displaystyle T_{m,\max} $$, $\Delta \omega$, use energy balance.

  2. Converter Output Voltage: Remember formulas for semi/full converters with/without freewheeling.

  3. Braking: Distinguish plugging (reverse voltage), dynamic (resistor across armature), regenerative ($$\displaystyle E_b > V_a $$).

  4. V/f Control: Below base: constant $V/f$ → constant torque; above: constant $V$ → constant power.

  5. Stability: Always compare slopes of $$\displaystyle T_m $$ and $$\displaystyle T_L $$ at equilibrium.

  6. 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

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