Experiment No 1 Title: Transmission ratio of the Transformer Board Experimental Purpose: Determine the transmission ratio of the transformer built-in in the Transformer Board. Necessary Equipment: Transformer board Connecting wires Voltmeter Experimental Setup: Experimental Procedure: First of all, I observed all the safety precautions. Then, I set up the circuit as shown in fig. After that, I measured voltages U1 and U2 and recorded them. I repeated the measurements for circuit (b). I then calculated the transmission ratio once from the measured values, and once from the number of windings. Table: Circuit 𝑼𝟏 /𝑽 𝑼𝟐 /V Transmission ratio determined from voltages Transmission ratio determined from of No. of windings a) 231.8V 266.1V 0.87 1.78 b) 231.7V 133.0V 1.74 1.74 Evaluation: Q.1 What do you ascertain when you compare the transmission ratio calculated from the voltages with the transmission ratio calculated from the number of windings? Answer: After observing the turn ratio from both of the methods, it can easily be concluded that both of their values are almost same, rather the values obtained from voltage ratio was more precise. Q.2 Why is the transmission ratio not exactly “1” in a transformer with equal primary and Secondary voltage? Answer: The turn ratio can possible to be “1” only and only if it is an ideal transformer but in real life it doesn’t exist so that’s why it can’t be exactly “1”. Experiment No 2 Title: Current and voltage ratios on load of transformer. Experimental Purpose: Measure the load current IL and the secondary voltage U2 on different types of loads (resistive load, inductive load and capacitive load). Necessary Equipment: Transformer board Connecting wires Voltmeter Experimental Experimental Setup: Primary Side: Primary side remains same in all circuit connections. i.e., no load, resistive load, capacitive load, inductive load etc. Its connections are as follows: Secondary Side: Experimental Procedure: First of all, I observed all the safety precautions. Then, I set up the circuit as shown in fig. After that, I measured voltages IL and U2 and recorded them. I repeated the measurements for Resistive Load Capacitive load Inductive load I recorded all the values in the observation. Table: Load 𝑼𝟐 /V 𝑰𝑳 /mA (a) 266.0V 66.1 mA (b) 246.8V 71.6 mA (c) 255.7V 88.8 mA (d) 267.0V 71.8 mA Graph: 266.8 U/V 261.8 256.8 251.8 246.8 66.1 71.1 76.1 81.1 86.1 I / mA Evaluation: Q.1 How does the transformer behave on different loads? Answer: If primary voltage is kept the same then for different types of loads, the value of current varied. Such that; the value of current was 0 for no-load, for resistive load it was same as the utilization of the load, for inductive it increased w.r.t resistive load and for capacitive load it was a bit lower than that of resistive load. Experiment No 3 Title: No load characteristics of transformer. Experimental Purpose: Record the no-load characteristic I0 = f (U0) of the transformer in the Transformer Board. A regulating transformer (0...230 V AC) is required as a voltage source in this experiment. Necessary Equipment: Transformer board Connecting wires Voltmeter Ammeter Experimental Setup: Experimental Procedure: First of all, I observed all the safety precautions. Then, I set up the circuit as shown in fig. After that, I measured voltages and current. Measure the no load current Io. Enter the values in the table. Transfer the values from the table to the grid provided in figure. Draw the no-load characteristics. I recorded all the values in the table. Table: 𝑼𝒐 /V 0 25 50 75 100 140 160 180 200 𝑰𝑜 /mA 0 0.04 0.09 0.13 0.19 0.28 0.35 0.41 0.48 Graph: 0.48 0.42 I 0 / mA 0.36 0.3 0.24 0.18 0.12 0.06 0 0 20 40 60 80 100 120 140 160 180 200 U0 / V Evaluation: Q.1 Why is the current characteristics not a straight line? Answer: It does not obey homogeneity and additive properties. A circuit is linear if and only if its input and output can be related by a straight line passing through the origin otherwise, it is a nonlinear system. Experiment No 4 Title: No load losses of transformer. Experimental Purpose: Determine the iron losses using the no-load experiment. The iron losses can be determined directly because the resistive losses of the winding are negligibly small in noload. A power meter or Watt meter (e. g. hps type 8705) is required to measure the active power P0. Necessary Equipment: Trainer board Connecting wires Voltmeter Ammeter Power meter Experimental Setup: Experimental Procedure: First of all, I observed all the safety precautions. Then, I set up the circuit as shown in fig. After that, I measured the iron losses using the no-load experiment. The iron losses can be determined directly. Experiment No 5 Title: Short circuit experiment Experimental Purpose: The copper losses of a transformer can be determined with the shortcircuit experiment. To do this the secondary winding is short-circuited and the voltage on the primary winding increased from 0 V until the rated current flows on the secondary side. Due to the very low voltage on the primary winding the iron losses can be neglected. Necessary Equipment: Transformer board Connecting wires Voltmeter Ammeter Power meter Experimental Setup: Experimental Procedure: First of all, I observed all the safety precautions. Then, I set up the circuit as shown in fig. After that, I measured the copper losses using the short-circuit experiment. Experiment No 6 (A) Title: Down transformation of voltages on no load. Experimental Purpose: Set up an auto-transformer with the TRANSFORMER BOARD and examine the voltage ratios on no-load. Theory: The auto-transformer is a special version of a transformer. It differs from the normal twowinding trans- former in that it only has one common winding with one tap. The winding is divided into two parts, the parallel and the series winding. With an auto-transformer the voltages can be transformed up or down depending on the wiring. With the auto-transformer the voltages can be transformed down. To transform up the in- put voltage U1 must be applied at the parallel winding and the output voltage U2 to the series winding. As a result, the output voltage U2 is higher than the input voltage U1. Since the input winding is connected conductively with the output winding (common winding), there is no electrical isolation from the feeding mains. Autotransformers may therefore not be used for generating safety extra-low voltages. The advantage of the auto-transformer is in the saving on winding copper and core iron. Smaller autotransformers are often designed as regulating transformers with a toroidal core. The efficiency of auto-transformers is up to 99.8 % providing the voltages at the output and input do not differ by more than 10 %. The total possible power emission of an auto-transformer is known as the throughline power SD. It is transferred partly by the current line of the input winding and the magnetic flow of the iron core. The more the transmission ratio ü approaches the value „1“, the smaller the power transmitted with induction at constant through line power (SD = U2 x I2). This power is known as construction power SB. The size of an auto- transformer depends on this. Experimental Setup: Experimental Procedure: Set up the circuit shown in figure. Measure the input voltage U1 and the output voltage U2 of the auto-transformer. Then calculate the output voltage U2 with the number of windings N1= 1978 and N2 = 1462. Result: In this experiment I Set up an auto-transformer with the Transformer Board and examine the voltage ratios on load. By performing experiment, I got following measurements, U1 = Input voltage = 220 V U2 = Output Voltage = 95V By calculation I get, U2calculated =U1measured.N2/ (N1+N2) =220. 1462/ (1978+1462) = 93.5 Evaluation: Q.1 What do you ascertain when you compare the transmission ratio calculated from the voltages with the transmission ratio calculated from the number of windings? Answer: Measured and calculated value of the output voltage U2 match very well. The transformer basic equation can therefore be used for the auto-transformer as well. A transformer turns ratio is the division of the number of turns in the primary winding by the number of turns in the secondary winding by the equation T_R=\frac{N_P} {N_S} This ratio should also equal the voltage of the primary winding divided by the voltage of the secondary winding, as given by Vp/Vs. Q.2 Why is the transmission ratio not exactly „1“in a transformer with equal primary and secondary voltage? Answer: Yes, ratio of turns is the same as ratio of voltages of windings for an ideal transformer. Real transformers do not have perfect coupling-they have leakage inductance which appears as a series inductance in each winding that does not couple to other winding inductances. This reduces the voltage a little from a secondary winding. (B) Title: Down transformation of voltages on load. Experimental Purpose: Set up an auto-transformer with the Transformer Board and examine the voltage ratios on load Experimental Setup: Experimental Procedure: Switch the board on and measure the mains voltage U1. Then switch the board back off. Set up the circuit shown in figure. Measure the output voltage U2 of the auto-transformer. Result: By this experiment I concluded that, the calculated and measured values of U2 is approximately samehe transformer basic equation can therefore be used for the auto-transformer as well. From this experiment I got following observations, Main voltage = U1 = 218V Output Voltage = U2 = 92.3V Evaluation: Q.1 How does the transformer behave on different loads? Answer: A control transformer is designed to provide rated output voltage at full VA. As the load decreases, the output voltage will go up. Conversely, increases in load will result in lower output voltages. Q.2 How does the transformer behave on different loads? Answer: A control transformer is designed to provide rated output voltage at full VA. As the load decreases, the output voltage will go up. Conversely, increases in load will result in lower output voltages. Experiment No 7 (A) Title: Up transformation of voltages no-load Experimental Purpose: Set up an auto-transformer with the Transformer Board and examine the voltage ratios on no-load. Necessary Equipment: Transformer board Connecting wires Voltmeter Experimental Setup: Experimental Procedure: Set up the circuit shown in figure. Measure the input voltage U1 and the output voltage U2 of the auto-transformer. Then calculate the output voltage U2 with the numbers of windings N1 = 1978 and N2 = 1462. Result: By this experiment I concluded that the calculated and measured values of U2 is approximately same. Real transformers don not have perfect couplinghe transformer basic equation can therefore be used for the auto-transformer as well. From this experiment I got following observations, Main voltage = U1 = 223V Output Voltage = U2 = 394V Calculated value from numbers of turns U2calculated =U1measured. (N1+N2)/N1 =220. (1978+1462)/1978 = 387.8V Evaluation: What do you determine when you compare the measured and calculated value of the output voltage U2? Answer: The output voltage equals the input voltage scaled by a ratio of resistors: the bottom resistor divided by the sum of the resistors. Measurements is the actual figure of the given thing. Whereas calculation is made by using the measured figures and putting that into formula. The actual (measured) resistance will vary from the nominal value due to subtle mechanical and chemical differences that occur during manufacturing. (B) Title: Up transformation of voltages on load Experimental Purpose: Set up an auto-transformer with the TRANSFORMER BOARD and examine the voltage ratios on load. Necessary Equipment: Transformer board Connecting wires Voltmeter Ammeter Experimental Setup: Experimental Procedure: Switch the board on and measure the mains voltage U1. Then switch the board back off. Set up the circuit shown in figure. Due to the expected high output voltage U2 two lamps must be connected in series as a load. Measure the output voltage U2 of the auto- transformer. Result: In this experiment I set up an auto-transformer with the transformer Board and examine the voltage ratios on load. From this experiment I got following observations, Main voltage = U1 = 210V Output Voltage = U2 = 360V Evaluation: Question 1: How strongly does the output voltage drop under load in comparison with noload? What are the reasons for the drop? Answer: Under no load conditions, there is no current flowing through the circuit, but there exist terminal voltages, which are equal to the rated voltage of the device. Voltage drops occur when loads are increased because an increase in current occurs, which depletes source capacity. The term "voltage drop" isn't a one-size-fits-all term, and unfortunately a lot of dickheads use the term interchangeably without the proper accommodating clarification. There are two common ways to view "voltage drop". 1- measuring potential difference across individual loads. 2- measuring potential difference across the source. Experiment No 8 Title: Commissioning of the three-phase induction motor Experimental Purpose: Operate the three-phase induction motor with squirrel-cage rotor on no load Necessary Equipment: Three-phase Induction Motor (Type 2707) Brake Unit (Type 2719) Control Unit (Type 2730) Universal Power Supply (Type 2740) Experimental Setup: Experimental Procedure: 1. I pushed the experimental machine onto the Brake Unit and couple it to the braking machine. 2. I set up the experiment as shown in Fig. 3. I connected the motor to the 400 V mains in delta circuit and switch on the Control Unit. 4. Then I switched on the Universal Power Supply: speed, torque and direction of rotation are displayed. 5. I watched the direction-of-rotation display and no-load speed of motor. Note: The motor should turn to the right. Exchange the mains leads if necessary. Switch off the Universal Power Supply First. Observation & Calculations: Direction of rotation: Right. No load speed N0 = 1470 rpm Experiment No 9 Title: Operation of a three-phase induction motor in star and delta circuit Experimental Purpose: Operate the three-phase induction motor first in star and then in delta circuit. Determine the torque characteristics Necessary Equipment: Three-phase Induction Motor (Type 2707) Brake Unit (Type 2719) Control Unit (Type 2730) Universal Power Supply (Type 2740) Experimental Setup: In star In Delta Experimental Procedure: I set up the experiment as shown in Fig I start up the system in star circuit. The motor should turn to the right. I recorded the characteristic points asked for in Table I switched off the Universal Power Supply first and then the Control Unit. Then I set up the experiment as shown in Fig I switch on the Control Unit. Start the braking machine and switch on the Universal Power Supply. I recorded the characteristic points asked for in Table To finish the experiment first switch off the Universal Power Supply and then the Control Unit. I draw the torque characteristics in graphs respectively. Table: For Star: Characteristics Points Speed (n) rpm Torque (M) Nm No load speed 1470 0.25 Rated speed 1440 0.58 1st sub value 1410 0.88 Pull out torque 1370 1.23 2nd sub value 1340 1.48 3rd sub value 1270 1.82 Min speed 120 1.91 Graph: 1470 1425 n rpm 1380 1335 1290 1245 1200 0.25 0.58 0.91 M Nm 1.24 1.57 1.9 For Delta: Characteristics Points No load speed Speed (n) rpm Torque (M) Nm 1480 0.23 Rated speed 1440 1.62 1st sub value 1390 2.99 Pull out torque 1350 3.74 2 sub value 1290 4.57 3rd sub value 1250 5.09 Min speed 510 5.75 nd Graph: 1470 1310 n rpm 1150 990 830 670 510 0.23 1.33 2.43 3.53 4.63 5.73 M Nm Evaluation: Q.1 How does the torque behave in star and delta circuit? Answer: Higher current means higher torque, and lower current means lower torque. Delta connected motor will draw more line current, so the torque it produces will also be higher compared to the Star connection of the same motor. During starting the motor windings are connected in star configuration and this reduces the voltage across each winding. This also reduces the torque by a factor of three. Q.2 When is the star/delta-startup circuit used? Describe the function of the circuit. Answer: This is the reduced voltage starting method. Voltage reduction during star-delta starting is achieved by physically reconfiguring the motor windings as illustrated in the figure below. During starting the motor windings are connected in star configuration and this reduces the voltage across each winding 3. This also reduces the torque by a factor of three. Q.3 The rating plate of a three-phase induction motor carries the specification A/Y 230/400V. How does this motor behave in delta circuit on the 400V three phase mains. Answer: When we use 400v the ampere will be the 1.732 times more than the 400v ampere. There will be a drop in efficiency as well as Break away starting torque will be less. The mean operating temperature will increase by 3 to 5deg. This is done by star and delta winding connection. Experiment No 10 Title: Efficiency, current and power factor of a three-phase induction motor Experimental Purpose: Objective is to determine the characteristics for efficiency, current and power factor of a three-phase induction motor with squirrel-cage rotor. Necessary Equipment: Three-phase Induction Motor (Type 2707) Brake Unit (Type 2719) Control Unit (Type 2730) Universal Power Supply (Type 2740) Power Factor Meter (10 A) 2 Multimeters Experimental Setup: Experimental Procedure: I set the experiment as shown in Fig Note: The motor should be operated in delta circuit and turn to the right. I recorded the characteristic points and wrote them in Table I measured the current I, the voltage U and the power factor cosΦ. Then I switched off the Universal Power Supply first and then the Control Unit. I draw the characteristics for efficiency, current in graph Calculation: N (rpm) M (Nm) POut (kW) U (V) I (A) cos Ф PIn (kW) %ɳ no-loadspeed 1480 0 0 392.7 0.92 0.5 0.312 0 ratedspeed 1470 0.88 0.135 393.3 6.02 0.5 2.04 6.6 1st sub-value 1400 2.76 0.404 393.8 6.10 0.5 2.08 19.4 pull-outtorque 1370 3.31 0.474 394 6.22 0.5 2.122 22.3 2nd sub-value 1270 4.52 0.60 392.5 6.49 0.5 2.20 27.7 3rd sub-value 510 6.09 0.325 393.4 6.44 0.5 2.50 18.8 min. speed 240 5.44 0.136 392 7.56 0.5 2.566 5.3 Characteristic points at Graph: 7.52 6.42 I/A 5.32 4.22 3.12 2.02 0.92 240 440 640 840 1040 1240 1440 1040 1240 1440 n / rpm 27 22.5 n% 18 13.5 9 4.5 0 240 440 640 840 n / rpm Evaluation: Q.1 What do you learn from the characteristics? Answer: In this experiment when the load is increased on motor, the current is increased.