Series Circuits 2 February 2005 Series Circuits Objective • At the conclusion of this presentation the student will – – – – – – – – – – Identify a series circuit Apply Ohm’s law in series circuits Determine and identify ground in a circuit Determine total series resistance Determine the current in a series circuit Determine the total effect of voltage sources in series Apply Kirchhoff’s voltage law Use a series circuit as a voltage divider Determine power in a series circuit Apply the proper prefix for units of measurement 2 February 2005 Professor Andrew H. Andersen Series Circuits 2 1 Series Circuits 2 February 2005 Series Circuit Characteristics 1. The current is the same everywhere in the circuit. – 2. Each component has an individual Ohm's law Voltage Drop. – 3. 5. This means that I can calculate the voltage using Ohm's Law if I know the current through the component and the resistance. Kirchoff's Voltage Law (KVL) applies. – 4. This means that wherever I try to measure the current, I will obtain the same reading. This means that the sum of all the voltage sources is equal to the sum of all the voltage drops or – VS = V1 + V2 + V3 + . . . + VN The total resistance in the circuit is equal to the sum of the individual resistances. – RT = R1 + R2 + R3 + . . . + RN The sum of the power supplied by the source is equal to the sum of the power dissipated in the components. – PT = P1 + P2 + P3 + . . . + PN 2 February 2005 Series Circuits 3 Current in a Series Circuit • The current in a series circuit is the same through all points • The current through each resistor in a series circuit is the same as the current through all the other resistors that are in series with it • Current entering any point in a series circuit is the same as the current leaving that point 2 February 2005 Professor Andrew H. Andersen Series Circuits 4 2 Series Circuits 2 February 2005 Current in a Series Circuit Current in a series circuit is the same everywhere 2 February 2005 Series Circuits 5 Measuring Current in a Series Circuit In a series circuit the location of the ammeter does not matter 2 February 2005 Professor Andrew H. Andersen Series Circuits 6 3 Series Circuits 2 February 2005 Series Resistance Formula • Regardless of the number of individual resistors connected in series, the total resistance of a series circuit is the sum of each of the individual values RT = R1 + R2 + R3 + . . . + RN • The total resistance will always be larger than the largest individual resistor 2 February 2005 Series Circuits 7 Total Series Resistance • The total resistance of a series circuit is equal to the sum of the resistances of each individual series resistor 2 February 2005 Professor Andrew H. Andersen Series Circuits 8 4 Series Circuits 2 February 2005 Resistors in Series • A series circuit provides only one path for current between two points so that the current is the same through each series resistor 2 February 2005 Series Circuits 9 Series Connected Resistance RAB = R1 + R2 RAB = R1 + R2 + R3 RAB = R1 + R2 + R3 + R4 2 February 2005 Professor Andrew H. Andersen Series Circuits 10 5 Series Circuits 2 February 2005 Total Series Resistance RT is not dependent on component order 2 February 2005 Series Circuits 11 Determining the Resistance on a Printed Circuit Board Trace the path from one end to the other and draw it on paper as you go 2 February 2005 Professor Andrew H. Andersen Series Circuits 12 6 Series Circuits 2 February 2005 Resistors on a Protoboard 2 February 2005 Series Circuits 13 Find R4 RT = R1 + R2 + R3 + R4 R4 = RT - R1 - R2 - R3 2 February 2005 Professor Andrew H. Andersen Series Circuits 14 7 Series Circuits 2 February 2005 Find R4 R4 = RT - R1 - R2 - R3 R4 = 146kΩ – 10kΩ – 33kΩ – 47kΩ 56kΩ 2 February 2005 Series Circuits 15 Ohm’s Law in Series Circuits • Current through one of the series resistors is the same as the current through each of the other resistors and is the total current • If you know the total voltage and the total resistance, you can determine the current by using: I= VT RT • If you know the voltage drop across one of the series resistors, you can determine the current by using any of the following: I= 2 February 2005 Professor Andrew H. Andersen VR1 VR2 VR3 VRN = = = R1 R2 R3 RN Series Circuits 16 8 Series Circuits 2 February 2005 Ohm’s Law in Series Circuits • If you know the total current, you can find the voltage drop across any of the series resistors by using: VR= I R • The polarity of a voltage drop across a resistor is positive at the end of the resistor that is closest to the positive terminal of the voltage source • The direction of current (electron flow) through a resistor is from the negative end of the resistor to the positive end 2 February 2005 Series Circuits 17 Ohm’s Law in Series Circuits • An open (an open switch or circuit failure) in a series circuit prevents all current from flowing (R = 0Ω) I = 0A • In an open series circuit, there is zero voltage drop across each series resistor • The supply voltage appears across the open points in the circuit 2 February 2005 Professor Andrew H. Andersen Series Circuits 18 9 Series Circuits 2 February 2005 Sources Connected Series Aiding 2 February 2005 Series Circuits 19 Sources Connected Series Opposing VT = VS1 – VS2 + VS3 2 February 2005 Professor Andrew H. Andersen Series Circuits 20 10 Series Circuits 2 February 2005 Kirchhoff’s Voltage Law • The algebraic sum of all voltages (both sources and drops) around a closed path is zero ΣV = 0 or VS – V1 – V2 – V3 - … - Vn = 0 2 February 2005 Series Circuits 21 Kirchhoff’s Voltage Law • The algebraic sum of all the voltage drops around a single closed loop in a circuit is equal to the total source voltage in that loop VS = V1 + V2 + V3 + … + Vn 2 February 2005 Professor Andrew H. Andersen Series Circuits 22 11 Series Circuits 2 February 2005 KVL ∑V SOURCES = ∑ VDROPS 10V = 5.5V + 4.5V 2 February 2005 Series Circuits 23 Voltage Divider I = I V1 VS = R1 R1 + R2 ⎛ R1 ⎞ V1 = VS ⎜ ⎟ ⎝ R1 + R2 ⎠ ⎛ R2 ⎞ V2 = VS ⎜ ⎟ ⎝ R1 + R2 ⎠ RT = R1 + R2 2 February 2005 Professor Andrew H. Andersen Series Circuits 24 12 Series Circuits 2 February 2005 Voltage Divider 2 February 2005 Series Circuits 25 Calculate V1 and V2 2 February 2005 Professor Andrew H. Andersen Series Circuits 26 13 Series Circuits 2 February 2005 Calculate V1 and V2 82Ω ⎛ ⎞ V1 = 10V ⎜ ⎟ ⎝ 82Ω + 68Ω ⎠ V1 = 5.47V 68Ω ⎛ ⎞ V2 = 10V ⎜ ⎟ ⎝ 82Ω + 68Ω ⎠ V2 = 4.53V 2 February 2005 Series Circuits 27 Use the Voltage Divider to Calculate V1, V2, and V3 2 February 2005 Professor Andrew H. Andersen Series Circuits 28 14 Series Circuits 2 February 2005 Use the Voltage Divider to Calculate V1, V2, and V3 ⎛ 100Ω ⎞ V1 = 100V ⎜ ⎟ ⎝ 1000Ω ⎠ V1 = 10V ⎛ 220Ω ⎞ V2 = 100V ⎜ ⎟ ⎝ 1000Ω ⎠ V2 = 22V ⎛ 680Ω ⎞ V3 = 100V ⎜ ⎟ ⎝ 1000Ω ⎠ V3 = 68V 2 February 2005 Series Circuits 29 Double Subscript Notation Node Referenced VAB VAC VBC VCD 2 February 2005 Professor Andrew H. Andersen Series Circuits 30 15 Series Circuits 2 February 2005 Double Subscript Notation Ground Referenced VA VB VC VD = 0V 2 February 2005 Series Circuits 31 Calculate the Voltage Drops 2 February 2005 Professor Andrew H. Andersen Series Circuits 32 16 Series Circuits 2 February 2005 Power in a Series Circuit • The total amount of power in a series resistive circuit is equal to the sum of the powers in each resistor in series PS = P1 + P2 + P3 + . . . + PN VS I = V1 I + V2 I + V3 I + . . . + VN I I2 RT = I2 R1 + I2 R2 + I2 R3 + . . . + I2 RN 2 February 2005 Professor Andrew H. Andersen Series Circuits 33 17