Series Circuits: Difference between revisions
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:The best way to visualize a series circuit is to draw a schematic, which is a simplified representation of the circuit in real life. | :The best way to visualize a series circuit is to draw a schematic, which is a simplified representation of the circuit in real life. | ||
:Resistors are usually represented in a schematic with [[File:Resistor Symbol.png|100px]] | :Resistors are usually represented in a schematic with [[File:Resistor Symbol.png|100px]] | ||
:<math>R_\text{total} = R_1 + R_2 + | :In series, individual resistances can be added up throughought and the sum is equal to the entire resistance across the whole circuit. | ||
:<math>R_\text{total} = R_1 + R_2 + R_n</math> | |||
:Batteries are represented in a schematic by [[File:Schematic-symbols-battery.png|75px]] | :Batteries are represented in a schematic by [[File:Schematic-symbols-battery.png|75px]] |
Revision as of 21:07, 9 April 2017
claimed by Cameron Whiteman spring 2017
Main Idea
- A series circuit is the most simple type of electrical circuit in which components are placed in succession of one another. A circuit in series only has one loop that can be drawn throughout.
- The electrical connection is not branched in any way and any disruption of the circuit causes the entire circuit to lose current. One can visualize this circuit as simply a closed loop. simple
- circuits often contain multiple components of differing resistances and functions which can be solved for using the loop rule. These components include: resistors, switches, capacitors, inductors, and of course, batteries.
The loop Rule
- When attempting to solve a series circuit, the simple rule to follow is the Loop rule. This is derived from Kirchoff's laws as well as Ohm's law and allows for electric potential, current, or resistance(s) to be solved
- for. To begin, draw a loop beginning from the positive terminal of the battery and traveling in a mathematical loop on a path to the negative terminal. More difficult circuits may have multiple loops and
- require more calculation, however, in the end this rule should always be true. The sum of the current at each resistor multiplied by its resistance must be equal to the electric potential of the battery. In other words, sum
- of the current going into the circuit must be equal to sum of the current leaving.
A Mathematical Model
- Kirchhoff's Current and Voltage Laws apply in a series circuit.
- Through Kirchhoff's Current Law, we know that the sum of all current going in must equal the sum of all current going out.
- [math]\displaystyle{ \sum{I}_{in} - \sum{I}_{out} = 0 }[/math]
- Since there are no nodes for the current to split up, the current throughout a series circuit will always be the same through each component.
- Through Kirchhoff's Voltage Law, the sum of all voltage in a closed system must be zero.
- [math]\displaystyle{ \sum{V}_{Battery} - \sum{V}_{Components} = 0 }[/math]
- Through Kirchhoff's Current Law, we know that the sum of all current going in must equal the sum of all current going out.
- Ohm's Law is extremely useful in finding the voltages, resistances, and current throughout the series circuit.
- Ohm's Law gives us the following formula:
- [math]\displaystyle{ V=IR }[/math]; it can be rearranged to yield [math]\displaystyle{ I=\frac{V}{R} }[/math] and [math]\displaystyle{ R = \frac{V}{I} }[/math]
- Ohm's Law gives us the following formula:
- Total Resistance in a series circuit is the sum of all resistances. It can be used to find the overall current in the circuit, which can then be used to find individual resistances.
- Total resistance is described by:
- [math]\displaystyle{ R_T=\sum_{n=1}^N {R}_{Series}=R_1+R_2+R_3+...R_N }[/math]
- Total resistance is described by:
- When solving circuits, the voltage across each component can be used in relation with Kirchhoff's Voltage Law in order to find unknown values.
- The voltage across an inductor is related by the following equation:
- [math]\displaystyle{ \Delta V_{inductor} = L\frac{dI}{dt} }[/math]
- The voltage across a capacitor can be determined using the following formula:
- [math]\displaystyle{ \Delta V_{capacitor} = \frac{Q}{C} }[/math]
- The voltage across a battery is found through the following equation:
- [math]\displaystyle{ \Delta V_{battery} = Ɛ_{mf} }[/math]
- The voltage across an inductor is related by the following equation:
A Computational Model
- The best way to visualize a series circuit is to draw a schematic, which is a simplified representation of the circuit in real life.
- Resistors are usually represented in a schematic with
- In series, individual resistances can be added up throughought and the sum is equal to the entire resistance across the whole circuit.
- [math]\displaystyle{ R_\text{total} = R_1 + R_2 + R_n }[/math]
- Batteries are represented in a schematic by
- Switches can be open or closed. An open switch is represented by
- Inductors are represented in a schematic by
- Capacitors are represented by
Examples
For these examples, find the values specified.
Simple
Find the current in the circuit.
Middling
Find the voltage across the battery if the current in the circuit is 0.5 A
Difficult
The voltage across [math]\displaystyle{ R_1 }[/math] is 5 volts. The voltage across [math]\displaystyle{ R_2 }[/math] is 6 volts. What are the resistances of [math]\displaystyle{ R_1, R_2, }[/math] and [math]\displaystyle{ R_3 }[/math] if the current measured across [math]\displaystyle{ R_3 }[/math] is .65 A and the voltage of the battery is 16V?
Solutions to Examples
Simple
[math]\displaystyle{ I=0 }[/math] Since the circuit is open, there is no way for current to flow through the circuit.
Middling
- 1. Find Total Resistance
- [math]\displaystyle{ R_T=R_1+R_2+R_3=10+35+15=60 }[/math] Ohms
- 2. Use Ohm's Law (current is given already)
- [math]\displaystyle{ V=IR=0.5\bullet60=30 }[/math] Volts
Difficult
- 1. Note that current across a series circuit is the same.
- Current = 0.65 A
- 2. Sum of battery voltage is equal to the sum of all voltage across resistors.
- [math]\displaystyle{ \sum{V}_{Battery} = \sum{V}_{Components} }[/math]
- [math]\displaystyle{ 16 = 5 + 6 + V_3 }[/math]
- [math]\displaystyle{ V_3 = 5 }[/math]
- 3. Use the rearranged Ohm's Law to find the resistances.
- [math]\displaystyle{ R=\frac{V}{I} }[/math]
- [math]\displaystyle{ R_1=\frac{5}{.65}=7.69 }[/math] Ohms
- [math]\displaystyle{ R_2=\frac{6}{.65}=9.23 }[/math] Ohms
- [math]\displaystyle{ R_3=\frac{5}{.65}=7.69 }[/math] Ohms
Connectedness
- Series circuits are the most basic type of circuits.
- They are used in all electronics; even parallel circuits can be simplified into a series circuit!
- Some realistic applications include making lights, motors, and other electrical appliances work.
- The most commonly used example for a series circuit is in lighting. However, Series is generally not the
- ideal setup as the loss of one bulb causes the current to cease and loss of power to all bulbs. On a larger
- scale, the idea of series is used in everyday household appliances. The device, whether it be a lamp or toaster,
- is connected into the wall and a switch either flips on to connect the circuit, allowing current to flow or there is
- a disconnect in the system, causing the entire unit to fail.
- The most common usage of series circuits in physics appears when breaking down much more complex and detailed circuits
- that might even be in parallel. When doing this, Kirchoff's laws are utilized to break up the circuit into multiple individual loops
- that, at which point, can be treated as series circuits. This trick can be extremely useful for solving difficult circuits and allows even
- the most confusing problems to be broken down into the simplest form.
History
- Series circuits date as far back as when the first battery was invented.
- In the 1800's Alessandro Volta invented the first battery; it was originally used to produce hydrogen and oxygen from water.
- Around the 1880's, however, light bulbs were commercialized and used to illuminate cities- none of this could be done without the basic circuit.
- Electric circuits involve both direct current, DC, and alternating current, AC. Direct current, when all of the current only flows in one direction, was first used by Thomas Edison for his electric power transmission. Alternating current, ;when the current alternates directions, was first discovered by Nikola Tesla while he was looking for a way to allow power transmissions to go longer distances than with DC.
- Gustav Robert Kirchoff was the main contributor to understanding how circuits worked. He was born March 12, 1824 and died on October 17, 1887. As a renowned German physicist, he proposed what
- are now universally accepted laws surrounding the way that circuits work as student in 1845.
See also
- Ohm's Law
- Resistors and Conductivity
- Current
- Ammeters,Voltmeters,Ohmmeters
- Power in a circuit
- RL Circuit
- LC Circuit
Further reading
- Matter & Interactions, Vol. II: Electric and Magnetic Interactions, 4nd Edition by R. Chabay & B.Sherwood (John Wiley & Sons 2015)
External links
References
- "All About Circuits - Electrical Engineering & Electronics Community." All About Circuits - Electrical Engineering & Electronics Community. Web. 30 Nov. 2015.
- "Build Electronic Circuits - Electronics Explained in a Simple Way." Build Electronic Circuits. Web. 30 Nov. 2015.
- Matter & Interactions, Vol. II: Electric and Magnetic Interactions, 4nd Edition by R. Chabay & B.Sherwood (John Wiley & Sons 2015)
- Soclof, Sidney. HowStuffWorks. HowStuffWorks.com. Web. 30 Nov. 2015.