TESTING OF DC MOTORS DEPARTMENT OF ELECTRICAL & ELECTRONICS ENGG.

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Presentation transcript:

TESTING OF DC MOTORS DEPARTMENT OF ELECTRICAL & ELECTRONICS ENGG. SESSION-2012-13

CONTENTS 1. Testing method of dc m/c. 2. simple/direct test . (a) Explanation,(b) Numerical (C) Disadvantage . 3 .Swinburne’s test. 4.Hopkinsion’s test

TESTING OF DC MACHINE Q:- Why testing are required ? Ans-Machines are tested for finding out losses, efficiency and temperature rise. For small m/c we used DIRECT LOADING test and for large shunt m/c, INDIRECT MET- HOD are used.

TESTING METHOD ARE Simple / Direct test. Swinburne’s / Indirect Method test. Hopkinson’s / Regenerative / Back - to - Back / Heat –run test.

Simple / Direct test This method is suitable only for SMALL DC m/c. In direct, method the DC m/c is subjected to rated load and the entire o/p power is wasted. The ratio of o/p power to i/p power gives the efficiency of DC m/c.

EFFICIENCY MOTOR Motor o/p={ω(s1-s2)r× 9. 81} Motor i/p= VtI. ή(motor)={o/p}/{i/p}. = [{ω(s1-s2)r× 9. 81}×100]/VtI where; s1&s2 are the tension on the belt. ω=2πn(motor speed in rad/sec r=radius of pulley in meters(=1/2 out side pulley dia+1/2 belt thickness) Vt=terminal voltage & I=line current.

NUMERICAL A full load break test on a small d.c m/c shunt motor ,give the following data Spring balance readings 25 kg & 9 kg Out side pulley diameter 19.5 cm Belt thickness 0.50 cm Motor speed 1500 rpm Applied voltage 230 v Line current 12.5 A Calculate the shaft torque, shaft power & motor efficiency at rated load.

SOLUTION Shaft torque=(S1-S2)×Effective radius =(25.9)[(19.5/2)+(0.5/2)]×(1/100)kg-m =16×0.1×9.81 Nm=15.7 Nm Shaft power=ω×Shaft torque =[(2π×1500)/60]×15.7=2470w Motor i/p=Vti=230×12.5=2875w ή(motor efficiency at rated load)=[2470/2875]×100=85.6%

DISADVANTAGES The spring balance readings are not steady. Friction torque does not const. At a particular setting of handwheels H1&H2

INDIRECT METHOD In this method ,no load m/c losses are first measured by a suitable test and then additional losses on load are determined from the m/c data ,in order to calculate the m/c efficiency . The simplest method of measuring the no load m/c losses is by SWINBURNE’S METHOD.

SWINBURNE’S METHOD As this is no load test ,it can’t be performed on a dc series motor In this method, the m/c whether it is a MOTOR or GENERATOR, is run as a no load shunt motor at rated speed

If Ia0 and If are the no load armature and field current respectively If Ia0 and If are the no load armature and field current respectively .Then power absorbed by the armature (=Vt×Iao) is equal to the no load rotational loss W0 plus a small amount armature circuit loss Ia0^2 ×ra. No load rotational loss W0=Vt×Iao- Ia0^2 ×ra. Here armature circuit resistance ra includes the brush contact resistance also. Shunt field loss=Vt×If.

Let IL be the load current at which m/c efficiency is required. Generator efficiency Generator o/p=Vt×IL Armature current Ia=IL+If Armature circuit loss= Ia^2×ra ra=armature circuit resistance when hot. Total loss=W0+ Ia^2×ra+Vt×If ή(Generator)=[1-{(W0+ Ia^2×ra+Vt×If)}/{(Vt×IL+ W0+ Ia^2×ra+Vt×If)}]

When m/c is working as a motor then Motor efficiency When m/c is working as a motor then Ia=IL-If Motor i/p=Vt×IL ή(motor efficiency)=[1-{(W0+Ia^2×ra+If×Vt)}/{(Vt×IL)}]

NUMERICAL A 400 v,20kw dc shunt motor takes 2.5 A when running light. For an armature resistance of 800Ω and brush drop 2V,find full load efficiency.

SOLUTION Field current If=400/800=.5A No load armature current Ia0=2.5-0.5=2.0A Constant no load rotational loss W0=Vt×Ia0-Ia0^2×ra-Vb×Ia. =400×2.0-2^2×0.5-2×2=794w. Total constant loss=W0+Vt×If=794+400×0.5 =994w At full load, let IL=Line current=Ia+If

Power i/p=Power o/p +total loosses Vt×IL =20,000+994+Ia^2×ra+Vb×Ia 400(Ia+0.5)=20,000+994+Ia^2+2×Ia Ia=56.22A Armature ohmic losses=56.22^2×0.5=1580.34w Brush drop losses=56.22×2=112.44w. Total losses=994+1580.34+112.44=2686.78w. Power i/p=20,000+2686.78=22686..78w. ή(motor at full load) =(20.000/22686.78)×100=88.157%

ADVANTAGES Low power is required for testing even large m/c, since only no load losses are to be supplied from the main. It is convenient and economical. The efficiency can be calculated at any load because constant losses are known.

DISADVANTAGES As the test is on no load, it doesn’t indicate whether the commutation on full load is satisfactory and whether the temperature rise would be within specified limit. THIS TEST CAN’T BE APPLIED FOR A SERIES MOTOR because speed of series motor is very high at no load ,it is not possible to run series motor on no load. Note:-In comparison to other the armature cu losses is so small that it may be neglected & constant loss may be take equal to no load i/p

Regenerative/Hopkinson’s method. In this method ,two identical d.c m/c are coupled ,both mechanically & electrically and are tested simultaneously. One of the m/c made to run as a MOTOR and it derives the other m/c as GENERATOR .

For this test m/c 1 is as a dc shunt motor by a starter & brought upto rated speed with switch S open .Bothe the m/c run at same speed ,because these are MECHANICALLY coupled .

To perform the test following procedure is adopted M/c 1(motor) is started through starter & its field rheostat is adjusted so that it runs at normal speed. The m/c 1(Motor) will drive m/c 2(Generator).The switch S is initially kept open. The excitation of m/c 2 is gradually increased ( by decreasing the field circuit resistance).till the volt metre 1 reads ZERO.Then switch S is closed.

M/c 2 is now floating neither taking any current from the supply nor delivering any current .Any desired load can be put on the set by adjusting the shunt field regulators.The m/c with lower excitation will act as a MOTOR and other m/c will act as a GENERATOR. Let V=supply voltage I2=Armature current of m/c 2(Generator) I1= Armature current of m/c 1(motor) . If2=Field current of m/c 2(Generator). If1=Field current of m/c 1(Motor). Ra=Armature resistance of each m/c

Motor i/p power =V(I+I2)=V×I1 Generator o/p power=V×I2. ............(1) If both the m/c have same efficiency ή,then o/p of motor =ή×i/p =ήV(I+I2)= V×I1 =Generator i/p . o/p of Generator =ή×i/p . =ή×ήV×I1=ή^2V(I1)............(2) From equ (1) & (2). ή^2V(I1)=V×I2. sqrt{(I2/(I1)}

EFFICIENCY Armature circuit loss in Generator =I2^2×ra . Armature circuit loss in Motor=I1^2×ra . Power drawn from supply= V×I. No load rotational loss in two m/c=W0= V×I-ra(I1^2+I2^2) . No load rotational loss for each m/c=W0/2 . Generator o/p= I2^2×ra. Generator loss=Wg=(W0/2)+V×If2+ I2^2×ra. ή(g)=[1-(Wg)/(V×I2+Wg)]

Motor i/p=V(I1+If1) Total motor losses Wm=(W0/2)+ V×If1 +I1^2×ra . ή( Motor)=[1-(Wm)/V(I1+If2)]

ADVANTAGE Total power taken from the supply is very low. Therefore this method is very economical. The temperature rise and the commutation condition can be checked under rated load condition. Large m/c can be tested at rated load without consuming much power from the supply. Efficiency at different load can be determine.

DISADVANTAGES The main disadvantage of this method is the necessity two practically identical m/c to be available

THANK YOU....