EE301 Final Exam Review Final Exam Review 1) Determine the total resistance (π½π½π»π» ) seen by the source and the currents (π°π°ππ ), (π°π°ππ ), and (π°π°ππ ) in the DC circuit below. 10 β¦ ππππ π½π½ π π = 10 + οΏ½ πΌπ = π°π°ππ + - π°π°ππ ππ 15 β¦ 12 β¦ −1 1 1 + οΏ½ = ππππ. ππ β¦ 12 15 + 5 πΌ1 = πππ 30 = = ππ. ππππππ π½π½ π π 17.5 π ππ = οΏ½ π°π°ππ πΌ2 = −1 1 1 + οΏ½ = ππ. ππ β¦ 12 15 + 5 5β¦ π ππ 7.5 (1.714) = ππ. ππππππ π½π½ (πΌπ ) = π 12 12 π ππ 7.5 (1.714) = ππ. ππππππ π½π½ (πΌπ ) = π 15+5 15 + 5 2) Find the power delivered by the source (π·π·ππ ) and the power absorbed by all of the resistors (π·π·ππππ ), (π·π·ππππ ), (π·π·ππππ ), and (π·π·ππ ). Does the power being delivered equal to the total power being absorbed? π·π·ππ = π·π·ππππ + π·π·ππππ + π·π·ππππ + π·π·ππ ππ = (πΌπ )(πππ ) = (1.714)(30) = ππππ. ππππ πΎπΎ π10 = (πΌπ )2 (π 10 ) = (1.714)2 (10) = ππππ. ππππ πΎπΎ π12 = (πΌ1 )2 (π 12 ) = (1.071)2 (12) = ππππ. ππππ πΎπΎ π15 = (πΌ2 )2 (π 15 ) = (0.643)2 (15) = ππ. ππππ πΎπΎ ππππ. ππππ πΎπΎ = 29.38 + 13.76 + 6.20 + 2.07 = ππππ. ππππ πΎπΎ Yes! Power delivered equals total power absorbed. π5 = (πΌ2 )2 (π 5 ) = (0.643)2 (5) = ππ. ππππ πΎπΎ 3) Use nodal analysis to find the voltage at the node (π½π½). Now use Ohm’s Law to find the voltage across the 12 β¦ resistor. Do these voltages equal each other? ππ − 30 ππ ππ + + =0 10 12 15 + 5 ππ οΏ½ 30 1 1 1 + + οΏ½= 10 10 12 20 ππ[0.233] = 3 ππ = 3 = 12.876 ππ 0.233 ππ12 = (πΌ1 )(π 12 ) = (1.071)(12) = 12.85 ππ Yes! This demonstrates there are many ways to solve a circuit. 4) Determine the total impedance (πππ»π» ) seen by the source and the currents (π°π°ππ ), (π°π°ππ ), and (π°π°ππ ) in the AC circuit below. 8β¦ ππππβ‘ππππππ π½π½ ππ = 8 + οΏ½ + π°π°ππ 14 β¦ π°π°ππ - 12 β¦ -j10 β¦ πππ 25β‘15π = = ππ. ππππβ‘ππππ. ππππππ π½π½ ππ 20.65β‘−7.34π πππ = οΏ½ πΌ1 = πΌ2 = 6β¦ j18 β¦ −1 −1 1 1 1 1 + + οΏ½ =8+οΏ½ οΏ½ 12 − π10 14 + 6 + π18 15.62β‘−39.81π 26.91β‘41.99π ππ = 8 + [0.064β‘39.81π + 0.037β‘−41.99π ]−1 = 8 + πΌπ = π°π°ππ 1 0.0784β‘11.94 π = ππππ. ππππβ‘−ππ. ππππππ β¦ −1 1 1 + οΏ½ = 12.76β‘−11.94π 12 − π10 14 + 6 + π18 πππ 12.76β‘−11.94π (πΌπ ) = (1.21β‘22.34π ) = ππ. ππππππβ‘ππππ. ππππππ π½π½ π1 12 − π10 πππ 12.76β‘−11.94π (πΌπ ) = (1.21β‘22.34π ) = ππ. ππππππβ‘−ππππ. ππππππ π½π½ π2 14 + 6 + π18 οΏ½οΏ½οΏ½οΏ½βπ»π» ) and the Real/Reactive power of the 5) Find the complex power delivered by the source (πΊπΊ elements (π·π·ππ ), (π·π·ππππ ), (πΈ−ππππππ ), (π·π·ππππ ), (π·π·ππ ) and (πΈππππππ ). Does the source complex power equal to the total Real and Reactive power of the elements? ∗ οΏ½οΏ½οΏ½οΏ½β οΏ½οΏ½οΏ½βπ οΏ½οΏ½πΌοΏ½οΏ½βπ οΏ½ = (25β‘15π )(1.21β‘−22.34π ) ππ = οΏ½ππ οΏ½οΏ½οΏ½οΏ½βπ = ππππ. ππππβ‘−ππ. ππππππ π½π½π½π½ π π8 = (πΌπ )2 (π 8 ) = (1.21)2 (8) = ππππ. ππππ πΎπΎ π12 = (πΌ1 )2 (π 12 ) = (0.988)2 (12) = ππππ. ππππ πΎπΎ π−π10 = (πΌ1 )2 (ππ ) = (0.988)2 (10) = −ππ. ππππ π½π½π½π½π½π½ Remember that an asterisk (*) is the symbol for the complex conjugate. πΌ 2 = (πΌ)(πΌ ∗ ) = (πΌβ‘π)(πΌβ‘ − π) = πΌ 2 β‘π − π = πΌ 2 β‘0π = πΌ 2 π14 = (πΌ2 )2 (π 14 ) = (0.574)2 (14) = ππ. ππππ πΎπΎ π6 = (πΌ2 )2 (π 6 ) = (0.574)2 (6) = ππ. ππππ πΎπΎ ππ18 = (πΌ2 )2 (ππΏ ) = (0.574)2 (10) = ππ. ππππ π½π½π½π½π½π½ οΏ½οΏ½οΏ½οΏ½β πΊπΊπ»π» = (π·π·ππ + π·π·ππππ + π·π·ππππ + π·π·ππ ) + ππ(πΈ−ππππππ + πΈππππππ ) οΏ½οΏ½οΏ½οΏ½β π π = (11.71 + 11.71 + 4.61 + 1.98) + π(−9.76 + 5.93) οΏ½οΏ½οΏ½οΏ½β ππ = (30.01) + π(−3.83) = ππππ. ππππβ‘−ππ. ππππππ π½π½π½π½ 6) What is the difference between Apparent Power and Complex Power? Complex Power has a magnitude and angle while Apparent Power is just the magnitude of the Complex Power. 7) Find the power factor (ππππ ) for the given Complex Power. Make sure to include if it is Leading or Lagging. a. πβ = 322β‘30.25π πππ΄ πΉπ = ππ. ππππππ π³π³π³π³πππππππ b. πβ = 259 − π324 πππ΄ tan π = πππππ ππ‘π π = π΄πππππππ‘ π −324 π = tan−1 οΏ½ οΏ½ = −51.36π 259 πΉπ = ππ. ππππππ π³π³πππ³π³π³π³πππππ πΉπ = cos π = cos(30.25) = 0.864 **Since the Complex Power Angle is Positive the Load is Inductive and using the acronym π¬π¬π³π³π°π° current Lags voltage, therefore it is a Lagging Power Factor. πβ = πβ‘−51.36π πΉπ = cos(−51.36) = 0.624 **Since the Complex Power Angle is Negative the Load is Capacitive (π°π°πͺπͺπ¬π¬) so current Leads voltage. ππππππ πΎπΎ π½π½ πΊπΊ −ππππππ π½π½π½π½π½π½ 8) An AC circuit operates at a frequency of ππ. ππππππ ππ»π»π and its impedance is ππ = ππππ + ππππππππ β¦. Is the impedance Inductive or Capacitive? What is the Inductive/Capacitive component value? **Since the imaginary component is positive then the impedance is Inductive. ππΏ = ππΏ πΏ= ππΏ 130 = = ππ. ππ ππ»π» π 2π(6.465π₯103 ) 9) An AC circuit operates at a frequency of ππππππ. ππππ ππ³π³π³π³/ππ and its impedance is ππ = ππππ − ππππππππ β¦. Is the impedance Inductive or Capacitive? What is the Inductive/Capacitive component value? **Since the imaginary component is negative then the impedance is Capacitive. ππ = πΆ= 1 ππΆ 1 1 = = ππππ ππππ π(ππ ) (383.14)(145) 10) The following circuit is operating at a frequency of π = ππππππ ππ³π³π³π³/ππ. π°π°ππ + ππππππ πΎπΎ ππππππβ‘ππππππ π½π½ ππππππ π½π½π½π½π½π½ - a. Draw the Power Triangle for the Load and label the Apparent, Real, and Reactive Power. Also include the Complex Power angle. οΏ½πβοΏ½ = οΏ½1602 + 4002 = 430.81 πππ΄ 400 π = tan−1 οΏ½ οΏ½ = 68.2π 160 b. Find the source current (π°π°ππ ). ∗ οΏ½οΏ½οΏ½οΏ½βπ οΏ½ οΏ½οΏ½οΏ½οΏ½β πβ = οΏ½ππ πΌπ οΏ½ ∗ οΏ½πΌοΏ½οΏ½βπ οΏ½ = 430.81β‘68.2π 220β‘40π ππππ. ππππ ππππππ π½π½π½π½π½π½ ππππππ πΎπΎ πΌπ = ππ. ππππβ‘−ππππ. ππππ π½π½ = 1.96β‘28.2π π΄ c. Typically we like to reduce the source current. This can be accomplished by connecting a Capacitor in parallel to an Inductive Load. The Capacitor component value (πͺπͺ) is determined by choosing a Capacitance Reactive Power (πΈππ ) equal to the Inductance Reactive Power (πΈπ³π³ ). Find the Capacitor component value so all of the Reactive Power at the Load is cancelled. In other words, what component value will correct the power factor to unity? |ππΏ | = |ππ | = 400 πππ΄π ππ 2 ππ = => ππ ππ = 1 => ππΆ (220)2 ππ = = 121 β¦ 400 πΆ= 1 = ππππ. ππππ ππππ (500)(121) d. Find the source current (π°π°ππ ) when a Capacitor is connected in parallel with the Load. Assume the Capacitance Reactive Power is −ππππππ π½π½π½π½π½π½. + π°π°ππ π°π°ππ ππππππ πΎπΎ ππππππβ‘ππππππ π½π½ πΌ1 = 1.96β‘−28.2π π΄ (πΌ2 = −ππππππ π½π½π½π½π½π½ ππππππ π½π½π½π½π½π½ - )∗ π°π°ππ οΏ½πβ οΏ½οΏ½οΏ½β πππ = 400β‘−900 220β‘40π πΌ2 = 1.82β‘130π π΄ πΌπ = πΌ1 + πΌ2 π = 1.82β‘−130 π΄ πΌπ = (1.96β‘−28.2π ) + (1.82β‘130π ) πΌπ = ππ. ππππππβ‘ππππ. ππππππ π½π½ 11) Find the Primary (π°π°ππ ) and Secondary (π°π°ππ ) currents for the circuit shown below. ππππ β¦ ππππβ‘ππππ π½π½ + π°π°ππ ππππππ β¦ ππππβ‘ππππ π½π½ + - π°π°ππ π°π°ππ - −ππππ β¦ ππβ¦ **Reflecting everything to the Primary side. ππππ β¦ 4:6 ππππππ β¦ ππ−ππππ ππππ π= ππ 4 2 = = ππ 6 3 2 2 π−π8 = π2 (ππ ) = οΏ½ οΏ½ (−π8) = −π3.56 β¦ 3 2 2 π6 = οΏ½ οΏ½ (6) = 2.67 β¦ 3 πΌπ = πππ 60β‘0π = = ππ. ππππβ‘−ππππ. ππππππ π½π½ ππ 10 + π15 − π3.56 + 2.67 2 πΌπ = ποΏ½πΌπ οΏ½ = (3.51β‘−42.08π ) = ππ. ππππβ‘−ππππ. ππππππ π½π½ 3 12) Refer to the circuit in problem 11. What component values do we need if we treat the secondary side as the Load and can replace the Load impedances (πππ³π³πππ³π³π³π³ ) with components that will achieve Maximum Power Transfer? ππΏπππ = (πππ» )∗ 10 − π15 = = ππππ. ππ − ππππππ. ππππ β¦ π2 2 2 οΏ½ οΏ½ 3 13) Find the Thevenin Equivalent (π½π½π»π»π»π») and (πππ»π»π»π» ) for the circuit below. 220 β¦ j30 β¦ 100 β¦ πππ³π³π³π³π³π³π³π³ -j50 β¦ ππβ‘ππππππ π¨π¨ -j20 β¦ j30 β¦ 220 β¦ First remove the Load. Next turn off the source (Current Source = Open) and find the Thevenin Impedance from the Load perspective. Note the 220β¦ and the –j20β¦ are not included because they do not provide a complete path. 100 β¦ -j50 β¦ πππ»π»π»π» -j20 β¦ πππ» = 100 + π30 − π50 = ππππππ − ππππππ β¦ j30 β¦ 220 β¦ Now turn on the source and find the Thevenin Voltage at the open terminals where the Load was. Note the j30β¦ and 100β¦ are on an open branch so no current travels through them and no voltage drop occurs. ππβ‘ππππππ π¨π¨ 100 β¦ + π½π½π»π»π»π» - -j50 β¦ -j20 β¦ ππππ» = (πΌπ )(π−π50 ) = (5β‘46π )(50β‘−90π ) = ππππππβ‘−ππππππ π½π½ a. Determine the Load (πππ³π³πππ³π³π³π³ ) that will achieve Maximum Power Transfer and draw the Thevenin Circuit with the Load. ππΏπππ = (πππ» )∗ = 100 + π20 β¦ ππππππβ‘−ππππππ π½π½ ππππππ β¦ + - −ππππππ β¦ ππππππ β¦ ππππππ β¦ 14) Find the time constants for the circuit below if: 50 β¦ 120 V + - 1 ππ 2 12 β¦ πͺπͺ = ππππππ. ππππππππ 20 β¦ + π½π½ππ - 30 β¦ 1 kβ¦ a. The switch is in the (ππ) position for a long time and then moves to position (ππ) until steady-state is reached. Is the Capacitor Charging or Discharging? 50 β¦ π ππ = (50)(30) = 18.75 β¦ 50 + 30 ππ→1 = (π ππ )(πΆ) = Charging + 30 β¦ (18.75)(373.33π₯10−6 ) = ππ πππ - b. The switch is in the (1) position for a long time and then moves to position (2) until steady-state is reached. Is the Capacitor Charging or Discharging? 2 (32)(373.33π₯10−6 ) 12 β¦ = ππππ. ππππ πππ + πΉπΉππππ - 15) In the Linear Motor below (π½π½ππ = 5.5 πππ), (π· = 8π), (π½π½π½π½ = 12 β¦), and (π³π³ = 3π). At (π‘ = 0) the switch is closed. Assume the sliding bar is initially at rest and there is no mechanical friction. πΉπΉπ¨π¨ π½π½ππ + - π°π°ππ + π¬π¬ππππππ π³π³ - a. Find the initial current and Force just after the switch is closed. **Initial πΈπππ = 0 because there is no motion. πΎπππΏ: − πππ + (πΌπ )(π π΄ ) + πΈπππ = 0 πΌπ = πππ 5.5π₯103 = = ππππππ. ππππ π½π½ π π΄ 12 πΉπΉππππ Discharging π ππ = 12 + 20 = 32 β¦ π1→2 = (π ππ )(πΆ) = 1 πΉ = πΌπΏπ½ = (458.33)(3)(8) πΉ = ππππ ππ°π° 20 β¦ b. Find the velocity of the bar and Force when (π°π°ππ = 50 π΄). ** πΈπππ = π’π½πΏ πΎπππΏ: − πππ + (πΌπ )(π π΄ ) + π’π½πΏ = 0 π’= πππ − (πΌπ )(π π΄ ) (5.5π₯103 ) − (50)(12) = = ππππππ. ππππ π/ππ π½πΏ (8)(3) πΉ = πΌπΏπ½ = (50)(3)(8) = ππ. ππ ππ°π° c. When the bar begins to move why does the total current (π°π°ππ ) in the circuit decrease? The current decreases because the induced voltage (π¬π¬πππππ³π³ ) across the sliding bar will increase creating a current opposing the source current (π°π°ππ ). 16) Match the following definitions. ___ I Personnel Safety A. Converts Electrical Energy into Mechanical Energy. ___ D Faraday’s Law B. Converts Mechanical Energy into Electrical Energy. ___ G Bus C. Magnetic field created by a current carrying wire interacts with an existing magnetic field to exert a developed force on the wire. ___ E Commutator H Equipment Reliability ___ ___ A Motor D. Movement of a conductor in a magnetic field that will induce a voltage. E. A segmented device commonly found in DC motors that are used with brushes to reverse the direction of the applied current on the rotor. F. A device commonly found in AC generators that are used with brushes to pass a DC current to create an electromagnet on the rotor. ___ J Circuit Breakers ___ F Slip Ring ___ C Lorentz Force Law ___ B Generator G. A heavy gauge conductor that connects multiple circuits or loads to a common voltage supply. H. The main reason an ungrounded system is used on Navy Ships. I. A critical downside of using an ungrounded system on Navy Ships. J. A device designed to trip when overcurrent or high currents are reached. 17) A DC Motor was tested under two operating speeds. Find the armature resistance (π½π½π³π³ ), motor constant (π²π π ), and the Mechanical Torque Loss (π»π»π³π³ππππππ). Test 1: Applied (ππππ π½π½π«π«πͺπͺ ) and measured (π°π°π³π³ = ππ. ππ π½π½) at (ππππππππ ππππ) with no load Test 2: Applied (ππππ π½π½π«π«πͺπͺ ) and measured (π°π°π³π³ = ππππ π½π½) at (ππππππππ ππππ) with a load πΉπΉππ π½π½π«π«π«π« + - π°π°ππ Applying KVL to the circuit to the right we get: π¬π¬ππ −πππ·πΆ + (πΌπ )(π π ) + πΈπ = 0 + - πΈπ = (πΎπ£ )π −πππ·πΆ + (πΌπ )(π π ) + (πΎπ£ )π = 0 π·π·πΆπΆπΆπΆπΆπΆ π·π·π π π π π π π·π·π°π°π°π° π·π·π΄π΄π΄π΄π΄π΄π΄π΄ π³π³π³π³π³π³π³π³ π·π·π¬π¬π¬π¬π¬π¬π¬π¬ π³π³π³π³π³π³π³π³ Test 1: −87 + (7.5)π π + (πΎπ£ )(200.01) = 0 Test 2: −87 + (68)π π + (πΎπ£ )(180.12) = 0 68 Multiply the Test 1 Equation by οΏ½− οΏ½ and add 7.5 the two equation together to solve for π²π π . + π ππ 1910 π1 = 2π οΏ½ οΏ½ = 2π οΏ½ οΏ½ = 200.01 πππ/π 60 60 π ππ 1720 π2 = 2π οΏ½ οΏ½ = 2π οΏ½ οΏ½ = 180.12 πππ/π 60 60 788.8 − (68)π π + (πΎπ£ )(−1813.42) = 0 −87 + (68)π π + (πΎπ£ )(180.12) =0 701.8 + (0)π π + (πΎπ£ )(−1633.3) = 0 πΎπ£ = 701.8 = ππ. ππππππππ π½π½ − ππ 1633.3 Now substitute πΎπ£ into Test 1 Equation to solve for π½π½π³π³ . −87 + (7.5)π π + (0.4297)(200.01) = 0 π π = 87 − (0.4297)(200.01) = ππ. ππππππ β¦ 7.5 Since Test 1 is unloaded than we can set ππΏπππ = 0. ππππ£ = (πΎπ£ )(πΌπ ) = ππΏππ π + ππΏπππ ππΏππ π = (0.4297)(7.5) = ππ. ππππππ π°π° − π a. Find (π·π·π°π°π°π° ), (π·π·π¬π¬π¬π¬ππππ π³π³ππππππ), (π·π·π³π³πππ π ), (π·π·π΄π΄πππππ΄π΄ π³π³ππππππ ), (π·π·πΆπΆπΆπΆπ»π» ), and the efficiency (Ζ) of the Motor using the results from Test 2. Assume ππΏππ π is constant. ππΌπ = (πΌπ )(πππ·πΆ ) = (68)(87) = ππππππππ πΎπΎ ππΈπππ πΏππ π = (πΌπ )2 (π π ) = (68)2 (0.141) = ππππππ. ππππ πΎπΎ ππππ£ = (πΌπ )(πΎπ£ )(π) = (68)(0.4297)(180.12) = ππππππππ. ππππ πΎπΎ π΄ππ π ππππ£ = ππΌπ − ππΈπππ πΏππ π = 5916 − 651.99 = ππππππππ. ππππ πΎπΎ ππππβ πΏππ π = (ππΏππ π )(π) = (3.223)(180.12) = ππππππ. ππππ πΎπΎ ππππ = ππΌπ − ππΈπππ πΏππ π − ππππβ πΏππ π = 5916 − 651.99 − 580.53 = ππππππππ. ππππ πΎπΎ Ζ= ππππ 4683.68 (100) = (100) = ππππ. ππππ % ππΌπ 5916 18) In the balanced 3-phase circuit find the Phase Voltage (π¬π¬π½π½π°π° ), the Line Current (π°π°ππ ), and the Total Complex Power at the Load (πΊπΊπ»π» ). Assume positive sequence and π¬π¬π½π½π©π© = ππππππ. ππππβ‘ππππππ π½π½. π¨π¨ −ππππ β¦ ππππ β¦ π°π°ππ + π¬π¬π¨π¨ ππ ππππππ β¦ - ππππππ β¦ πͺπͺ ππππ β¦ π©π© π°π°ππ π°π°ππ −ππππ β¦ ππππ β¦ −ππππ β¦ ππππ β¦ ππππ β¦ ππ ππππππ β¦ ππππ β¦ ππ Typically the objective in 3-phase problems is to redraw the circuit as a Single Phase with reference to the neutral line. Phase π½π½ is commonly chosen as the phase to work with and this means we need to know the Line to Neutral Voltage (π¬π¬π½π½π°π° ) and make sure our Load is in the Y-formation. πΈπ΄π΅ = πΈπ΄π (√3 β‘30π ) πΈπ΄π = πΈπ΄π΅ √3 β‘30π = 346.41β‘30π √3 β‘30π = ππππππβ‘ππππ π½π½ Single Phase Circuit π¨π¨ −ππππ β¦ ππππ β¦ π°π°ππ + ππ π¬π¬π¨π¨π¨π¨ ππππ β¦ - π΅π΅ πΌπ = πΈπ΄π 200β‘0π = = 8β‘−16.26π π΄ ππ −π8 + 14 + 10 + π15 ππ ππππππ β¦ πΌπ = πΌπ (β‘−120π ) = 8β‘(−16.26π − 120π ) = ππβ‘ − ππππππ. ππππππ π½π½ οΏ½οΏ½οΏ½οΏ½β∅ = (πΌ)2 (π) = (8)2 (10 + π15) = 640 + π960 πππ΄ π οΏ½οΏ½οΏ½οΏ½β οΏ½οΏ½οΏ½οΏ½β∅ = 1920 + π2880 = ππππππππ. ππππβ‘ππππ. ππππππ π½π½π½π½ ππ = (3)π 19) In the balanced 3-phase circuit find the Phase Impedance (ππβ ) and the Phase Current (π°π°π³π³ππ ). Also οΏ½οΏ½οΏ½οΏ½βπ»π» οΏ½ Power delivered by the find the Total Real (π·π·π»π» ), Total Reactive (πΈπ»π» ), and Total Apparent οΏ½πΊπΊ οΏ½οΏ½οΏ½οΏ½β∅ = ππππππ − ππππππππ π½π½π½π½), Generator. The per-phase Complex Power at the Load is (πΊπΊ ππ ππ (π¬π¬π½π½π°π° = ππππβ‘ππππ π½π½), and (π°π°ππ = ππππβ‘ππππππ π½π½). Assume positive sequence. π¨π¨ + ππ β¦ π°π°ππ ππππππ β¦ ππ π¬π¬π¨π¨π¨π¨ - πͺπͺ π°π°ππ π©π© π°π°ππ ππ β¦ ππ β¦ ππππππ β¦ ππππππ β¦ ππ ππβ ππ Transform the (β − πΏπππ) to a (π − πΏπππ) so you can construct a Single Phase Circuit. ππ ππ ππ ππβ ππ = πβ 3 ππππ ππ ππ ππ Single Phase Circuit π¨π¨ ππ β¦ π°π°ππ + ππππππ β¦ ππππ π¬π¬π¨π¨π¨π¨ - ππ π΅π΅ Complex Power delivered by the Generator. πΌπ = πΌπ (β‘+120π ) πΌπ = πΌπ 12β‘130π = = 12β‘10π π΄ β‘1200 β‘120π π πΌπ = πΌππ (√3 β‘−30 ) πΌππ = πΌπ √3 β‘−30π = 12β‘10π √3 β‘−30π = ππ. ππππβ‘ππππππ π½π½ Single Phase Complex Power at the Load is οΏ½οΏ½οΏ½οΏ½β π∅ = 480 − π310 πππ΄ οΏ½οΏ½οΏ½οΏ½β∅ = π ππ = ππ (πΌπ )2 (ππ ) οΏ½οΏ½οΏ½οΏ½β π∅ 480 − π310 = = 3.33 − π2.15 β¦ 2 (πΌπ ) (12)2 πβ = (3)ππ = (3)(3.33 − π2.15) = ππππ − ππππ. ππππ β¦ οΏ½οΏ½οΏ½οΏ½β π∅ = (πΈπ΄π )(πΌπ )∗ οΏ½οΏ½οΏ½οΏ½β∅ = (80β‘20π )(12β‘−10π ) = 960β‘10π πππ΄ π οΏ½οΏ½οΏ½οΏ½β οΏ½οΏ½οΏ½οΏ½β∅ = 2880β‘10π πππ΄ ππ = (3)π οΏ½οΏ½οΏ½οΏ½β π π = 2836.25 + π500.11 πππ΄ ππ = ππππππππ. ππππ πΎπΎ ππ = ππππππ. ππππ π½π½π½π½π½π½ οΏ½οΏ½οΏ½οΏ½β οΏ½π π οΏ½ = ππππππππ π½π½π½π½ In previous 3-phase problems we have been only interested in the Line or Phase variables that the Generator (source) has produced to solve for the 3-phase system characteristics. In AC Generator problems we will step back to a more detail look of the internal parameters of the Generator. Remember a Generator converts Mechanical Energy from a prime mover (an axle) into Electrical Energy. An axle will rotate with an established constant magnetic field on the rotor that will induce a voltage (π¬π¬πππππ³π³ ) on the stator windings. Before the voltage potential reaches the outer terminals of the Generator (Line Voltages) the induced voltage will suffer internal losses due to resistance of the stator windings (π½π½πΊπΊ ) and mutual inductance of the stator winding (πΏπΏπΊπΊ ). The circuit diagram on the left is the Single Phase Circuit of the Generator. π°π°ππ + πΏπΏπΊπΊ πΉπΉπΊπΊ + + π·π·π°π°π°π° π·π·π¬π¬π¬π¬π¬π¬π¬π¬ π³π³π³π³π³π³π³π³ π°π°ππ π¬π¬π¨π¨π¨π¨ - - π΅π΅ π·π·π΄π΄π΄π΄π΄π΄π΄π΄ π³π³π³π³π³π³π³π³ π¨π¨ π¬π¬π¨π¨π¨π¨ π¬π¬ππππππ - π¨π¨ π΅π΅ π·π·πΆπΆπΆπΆπΆπΆ πͺπͺ Load π©π© π°π°ππ π°π°ππ 20) A 3-phase, Y-connected, 8-pole, 2.88 KV, 50 Hz synchronous generator is rated to deliver 4.5 MVA at a power factor of 0.8829 Lagging. The per-phase stator resistance is 0.09β¦ and the synchronous reactance is negligible. The AC Generator is operating at the rated Load with Mechanical Losses at 410 kW. To simplify the problem first list all the given variables. 3 − πβππ π π π¦π‘ππ π ππ‘ππ πππ€ππ = 3 − πβππ π π΄πππππππ‘ πππ€ππ 8 − ππππ πππ€ππ ππππ‘ππ = πππππ ππ πΆππππππ₯ πππ€ππ π − πππππππ‘ππ π = 50 π»π§ π ππ‘ππ π£πππ‘πππ = πΏπππ π‘π πΏπππ π£πππ‘πππ = 2.88 πππ ππππβ πΏππ π = 410 ππ οΏ½οΏ½οΏ½οΏ½β οΏ½π π οΏ½ = 4.5 ππππ΄ π = cos−1(0.8829) = 28π *Lagging = positive angle π π = 0.09 β¦ ππ = 0 β¦ a. At what speed does the shaft rotate (ππππ)? ππππ = 120(π) 120(50) = = ππππππ ππππ πππππ 8 b. Find the Line Current (π°π°π³π³ ). Single Phase Circuit + - π°π°ππ πΏπΏπΊπΊ πΉπΉπΊπΊ + π¬π¬π¨π¨π¨π¨ π¬π¬ππππππ οΏ½οΏ½οΏ½οΏ½β πΊπΊ∅ Rated Single Phase Complex Power - π΅π΅ οΏ½οΏ½οΏ½οΏ½β ππ = 4.5β‘28π ππππ΄ οΏ½οΏ½οΏ½οΏ½β∅ = π π¨π¨ οΏ½οΏ½οΏ½οΏ½β ππ 4.5β‘28π ππππ΄ = = 1.5β‘28π ππππ΄ 3 3 π πππ πΈπ΄π΅ = 2.88β‘ππ΄π΅ πΈπ΄π = πΈπ΄π΅ √3 β‘30π οΏ½οΏ½οΏ½οΏ½β∅ = (πΈπ΄π )(πΌπ )∗ π (πΌπ )∗ = = π 2.88β‘ππ΄π΅ πππ √3 β‘30π = 1.663β‘0π πππ οΏ½οΏ½οΏ½οΏ½β π∅ 1.5β‘28π ππππ΄ = = 901.98β‘28π π΄ πΈπ΄π 1.663β‘0π πππ Note the given rated Line Voltage (π¬π¬π½π½π©π© ) does not include an angle so we can choose any angle. It is common for the ease of calculations to set (π¬π¬π½π½π°π° ) as the reference angle (π½π½π½π½π°π° = ππππ) or you can think of it as setting (π½π½π½π½π©π© = ππππππ ). πΌπ = ππππππ. ππππβ‘−ππππππ π½π½ c. Find (π·π·πΆπΆπΆπΆπ»π» ), (π·π·π¬π¬π¬π¬ππππ π³π³ππππππ), and (π·π·π°π°π°π° ) of the Generator. π·π·πΆπΆπΆπΆπ»π» is the real component of the rated Total Complex Power. ππππ = (4.5π₯106 ) cos(28π ) = ππ. ππππππ π΄π΄πΎπΎ π·π·π¬π¬π¬π¬ππππ π³π³ππππππ is caused only by the stator resistance. Remember the given π½π½πΊπΊ and the current we found (π°π°π³π³ ) is for single phase, so the π·π·π¬π¬π¬π¬ππππ π³π³ππππππ needs to be multiplied by 3. ππΈπππ πΏππ π = 3(πΌπ )2 (π π ) = 3(901.98)2 (0.09) = ππππππ. ππππ ππΎπΎ ππΌπ = ππππ + ππππβ πΏππ π + ππΈπππ πΏππ π = 3.973 + 0.41 + 0.21966 = ππ. ππππππ π΄π΄πΎπΎ d. What is the efficiency (Ζ) of the generator? Ζ= ππππ 3.973 ππ (100) = (100) = ππππ. ππππ% ππΌπ 4.603 ππ e. What is the prime mover torque? The prime mover will induce a synchronous Voltage which delivers the Power (π·π·π°π°π°π° ) into the Generator system. π = 2π οΏ½ π ππ 750 οΏ½ = 2π οΏ½ οΏ½ = 78.54 πππ/π 60 60 ππΌπ = (πππ )(π) πππ = ππΌπ 4.603π₯106 = = ππππ. ππππ ππ°π° − π π 78.54