1 / 10

ENERGY CONVERSION ONE (Course 25741)

ENERGY CONVERSION ONE (Course 25741). CHAPTER SEVEN INDUCTION MOTORS … (Induced Torque…) . … INDUCTION MOTOR INDUCED-TORQUE EQUATION. Z TH =R TH +jX TH = jX M (R 1 +jX 1 )/[R 1 +j(X 1 +X M )] Since X M >>X 1 and X M +X 1 >>R 1 , Thevenin

saima
Télécharger la présentation

ENERGY CONVERSION ONE (Course 25741)

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. ENERGY CONVERSION ONE(Course25741) CHAPTER SEVEN INDUCTION MOTORS … (Induced Torque…)

  2. …INDUCTION MOTOR INDUCED-TORQUE EQUATION ZTH=RTH+jXTH = jXM(R1+jX1)/[R1+j(X1+XM)] • Since XM>>X1 and XM+X1>>R1 , Thevenin resistance & reactance can be approximated as: RTH ≈ R1 ( XM/ [X1+XM] ) ^2 XTH ≈ X1 • resulting equivalent circuit:

  3. …INDUCTION MOTOR INDUCED-TORQUE EQUATION • The current I2 obtained as follows: I2= VTH / (ZTH + Z2)=VTH/[RTH +R2/s + j XTH +j X2] • Magnitude of current: I2= VTH /√(RTH+R2/s)^2+(XTH+X2)^2 • Air gap power PAG = 3 I2^2 R2/s= 3 VTH^2 R2/s / [(RTH+R2/s)^2+(XTH+X2)^2] and rotor induced torque is: Tind=PAG/ ωsync Tind=3VTH^2 R2/s / {ωsync [(RTH+R2/s)^2+(XTH+X2)^2]} a plot of torque as function of speed (& slip) shown in next figure:

  4. …INDUCTION MOTOR INDUCED-TORQUE EQUATION • A typical induction motor torque-speed characteristic curve

  5. …INDUCTION MOTOR INDUCED-TORQUE EQUATION • A plot of speed above & below normal range shown below:

  6. INDUCTION MOTORTORQUE-SPEED CURVE • Torque-speed characteristics curve provides several important information 1- induced torque of motor is zero at syn. Speed 2- torque-speed curve is nearly linear between no load and full load.In this range rotor resistance is much larger than its reactance so rotor current, rotor magnetic field & induced torque increase linearly with increasing slip 3- there is a maximum possible torque that cannot be exceeded (pullout torque) is 2 to 3 times rated full-load torque of motor (calculated in next section) 4-starting torque on motor is slightly larger than its full-load torque, so this motor will start carrying any load that it can supply at full power 5- Note: that torque on motor for a given slip varies as square of applied voltage. This is useful in one form of induction motor speed control that will be described

  7. INDUCTION MOTORTORQUE-SPEED CURVE 6- if rotor of induction motor driven faster than sync. Speed, direction of Tind reverses & machine become Gen. converting Pmech to Pelec (discussed later) 7- if motor turning backward relative to direction of magnetic fields,induced torque will stop machine very rapidly & will try to rotate it in other direction since reversing direction of magnetic field rotation is simply a matter of switching any two stator phases, this fact can be used as a way to very rapidly stop an induction motor act of switching two phases in order to stop motor very rapidly is calledplugging

  8. INDUCTION MOTORTORQUE-SPEED CURVE • Power converted to mechanical in an induction motor: Pconv=Tindωm • Note:peak power supplied by induction motor occurs at a different speed than maximum torque; and of course no power is converted to mechanical form when rotor is at zero speed

  9. INDUCTION MOTORTORQUE-SPEED CURVE • Induced Torque & Power Converted versus motor Speed in r/min (4 pole induction motor)

  10. INDUCTION MOTORTORQUE-SPEED CURVE • Maximum (Pullout) Torque in induction motor • Tind=PAG/ωsync maximum possible torque occurs when air gap power is maximum • Since air-gap power = power consumed in R2/smaximum induced torque will occur when power consumed by this resistor is maximum • If angle of load impedance is fixed, maximum power transfer theorem states : maximum power transfer occur when magnitude of that impedance = source impedance magnitude • Equivalent source impedance: Zsource=RTH+jXTH+jX2 • So maximum power transfer occurs when: R2/s=√RTH^2 + (XTH+X2)^2

More Related