Electric Potential Difference: Difference between revisions
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Claimed and Written by Daniel Kurniawan for PHYS2212 | Claimed and Written by Daniel Kurniawan for PHYS2212 | ||
[[File:Voltages.jpg|right|300px|thumb|The figure above shows a voltmeter measuring the potential difference in the battery]] | [[File:Voltages.jpg|right|300px|thumb|The figure above shows a voltmeter measuring the potential difference in the battery]] | ||
[https://en.wikipedia.org/wiki/Voltage Electric Potential Difference], also known as voltage, is the difference in [https://en.wikipedia.org/wiki/Electric_potential electric potential energy] between two points per unit of electric charge. The voltage between two points is equal to the work done per unit of charge against | [https://en.wikipedia.org/wiki/Voltage Electric Potential Difference], also known as voltage, is the difference in [https://en.wikipedia.org/wiki/Electric_potential electric potential energy] between two points per unit of electric charge. The voltage between two points is equal to the work done per unit of charge against an unchanging electric field to move the charge between two points and is measured in volts. | ||
Voltage can be caused by static [https://en.wikipedia.org/wiki/Electric_field electric fields], by [https://en.wikipedia.org/wiki/Electric_current electric current] through a [https://en.wikipedia.org/wiki/Magnetic_field magnetic field], by time-varying magnetic fields, or some combination of these three. One can use a [https://en.wikipedia.org/wiki/Voltmeter voltmeter] to measure the potential difference between two points in a circuit. A voltage may represent either a source of energy (electromotive force), or lost, used, or stored energy (potential drop). | Voltage can be caused by static [https://en.wikipedia.org/wiki/Electric_field electric fields], by [https://en.wikipedia.org/wiki/Electric_current electric current] through a [https://en.wikipedia.org/wiki/Magnetic_field magnetic field], by time-varying magnetic fields, or some combination of these three. One can use a [https://en.wikipedia.org/wiki/Voltmeter voltmeter] to measure the potential difference between two points in a circuit. A voltage may represent either a source of energy (electromotive force), or lost, used, or stored energy (potential drop). | ||
== | ==The Main Idea== | ||
Say you have two points "A" and "B" in space. The potential difference is defined as the difference in electric potential between those two points. Electric potential is electric potential energy per unit charge, measured in [https://en.wikipedia.org/wiki/Joule joules] per [https://en.wikipedia.org/wiki/Coulomb coulomb] (J/C), otherwise known as volts. | |||
'''Circuits''' | |||
Potential difference is typically used in describing the voltage dropped across some sort of electrical device, such as a [https://en.wikipedia.org/wiki/Resistor resistor]. The voltage drop across the device is the difference between measurements at each terminal of the device with respect to a common reference point. The voltage drop is the difference between the two readings. Two points in an electric circuit that are connected by an ideal conductor without resistance and not within a changing magnetic field have a voltage of zero. Any two points with the same potential may be connected by a conductor and no current will flow between them. | |||
'''Potential Difference in a Series Circuit''' | |||
[[File: Seriess.jpg]] | |||
In a [https://en.wikipedia.org/wiki/Series_and_parallel_circuits series circuit], the potential difference supplied by the battery is divided up between the components. If the components all have the same resistance they will have equal amounts of potential difference across them. If the resistances are not equal, they may have different amounts of potential difference (See [https://en.wikipedia.org/wiki/Ohm%27s_law Ohm's Law]) across them but when added up they must always equal the potential difference supplied by the battery. | |||
'''Potential Difference in a Parallel Circuit''' | |||
[[File: Parallel.jpg]] | |||
In a [https://en.wikipedia.org/wiki/Series_and_parallel_circuits parallel circuit],the potential difference supplied by the battery is the same potential difference as that across each of the components in the circuit. If three resistors are placed in parallel branches and powered by a 12-volt battery, then the voltage drop across each one of the three resistors is 12 volts. A charge flowing through the circuit would only encounter one of these three resistors and thus encounter a single voltage drop of 12 volts. | |||
=== | ===A Mathematical Model=== | ||
<math>\Delta V_{BA} = V(x_B) - V(x_A) = - \int_{r_0}^{x_B} \vec{E} \cdot d\vec{l} - \left( - \int_{r_0}^{x_A} \vec{E} \cdot d\vec{l} \right) | <math>\Delta V_{BA} = V(x_B) - V(x_A) = - \int_{r_0}^{x_B} \vec{E} \cdot d\vec{l} - \left( - \int_{r_0}^{x_A} \vec{E} \cdot d\vec{l} \right) | ||
= \int_{x_B}^{r_0} \vec{E} \cdot d\vec{l} + \int_{r_0}^{x_A} \vec{E} \cdot d\vec{l} = \int_{x_B}^{x_A} \vec{E} \cdot d\vec{l}</math> | = \int_{x_B}^{r_0} \vec{E} \cdot d\vec{l} + \int_{r_0}^{x_A} \vec{E} \cdot d\vec{l} = \int_{x_B}^{x_A} \vec{E} \cdot d\vec{l}</math> | ||
As | As seen above, the potential difference from one point to another in space is calculated as the path integral of the electric field and the time rate of change of magnetic field along that path (alternate way - multiply electric field times the distance covered across the two points). The voltage between point A to point B is equal to the work which would have to be done, per unit charge, against or by the electric field to move the charge from A to B. The voltage between the two ends of a path is the total energy required to move a small electric charge along that path, divided by the magnitude of the charge. Both an unchanging electric field and a dynamic electromagnetic field must be included in determining the voltage between two points. Check out this [https://www.youtube.com/watch?v=Ircup9aIJzU YouTube Video] that shows how to calculate potential, potential difference, and voltage in a system. | ||
Potential difference is defined in such a way that negatively charged objects are pulled towards higher voltages, while positively charged objects are | Potential difference is defined in such a way that negatively charged objects are pulled towards higher voltages, while positively charged objects are attracted towards lower voltages. This means that the [https://en.wikipedia.org/wiki/Electric_current#Current conventional current] in a system always flows from higher voltage to lower voltage. Current can flow from lower voltage to higher voltage, but only when there is some source of energy present to push it against the opposing electric field. For example, inside a [https://en.wikipedia.org/wiki/Battery_(electricity) battery], chemical reactions provide the energy needed for ion current to flow from the negative to the positive terminal. | ||
== | ===A Computational Model=== | ||
[https://phet.colorado.edu/sims/html/john-travoltage/latest/john-travoltage_en.html John Travoltage] is a model for voltage using his body as the circuit. | |||
'''Kirchoff's Voltage Law''' | |||
One of [https://en.wikipedia.org/wiki/Kirchhoff%27s_circuit_laws Kirchoff's Circuit Laws] (more specifically the Voltage Law) can be used to calculate the various voltages within a circuit. For example, the voltage between points A and C is the sum of the voltage between A and B and the voltage between B and C. The various voltages can be calculated using [https://www.physics.uoguelph.ca/tutorials/ohm/Q.ohm.KVL.html Kirchoff's Voltage Law], which states that the directed sum of the electrical potential differences around any closed network is zero. Essentially, the sum of the potential differences in any closed loop is equivalent to the sum of the potential drops in that loop. | |||
<math>\sum_{k=1}^n V_k = 0</math> | |||
==Examples== | |||
===Simple=== | |||
[[File: 9.png]] | |||
'''Question''' | |||
What are the equations for voltage based on the loop rule for loop 1 and loop 2? | |||
In the figure above, the total voltage around loop 1 should sum to zero, as does the total voltage in loop 2. Also, the loop which consists of the outer part of the circuit (the path ABCD) should also sum to zero, as shown by Kirchoff's Voltage Law. | |||
'''Solution''' | |||
===Middling=== | |||
'''Question''' | |||
'''Solution''' | |||
===Difficult=== | |||
''' | '''Question''' | ||
'''Solution''' | |||
==See Also== | ==See Also== | ||
=== | ===Further Reading=== | ||
[https:// | *[https://en.wikipedia.org/wiki/Kirchhoff%27s_circuit_laws Kirchoff's Circuit Laws] <div></div> | ||
[ | *[https://en.wikipedia.org/wiki/Alternating_current Alternating Current]<div></div> | ||
*[https://en.wikipedia.org/wiki/Direct_current Direct Current]<div></div> | |||
*[https://en.wikipedia.org/wiki/Electric_potential Electric Potential]<div></div> | |||
*[https://en.wikipedia.org/wiki/Ohm%27s_law Ohm's Law] | |||
=== | ===External Links=== | ||
[https://www.youtube.com/watch?v=Ircup9aIJzU Calculating Potential, Potential Difference, and Voltage]<div></div> | *[https://www.physics.uoguelph.ca/tutorials/ohm/Q.ohm.KVL.html Kirchoff's Voltage Law]<div></div> | ||
[https://www.youtube.com/watch?v=HJrkw_YQzcc Potential Difference as a Path Integral] | *[http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference Electric Potential Difference] | ||
*[https://www.youtube.com/watch?v=Ircup9aIJzU Calculating Potential, Potential Difference, and Voltage]<div></div> | |||
*[https://www.youtube.com/watch?v=HJrkw_YQzcc Potential Difference as a Path Integral] | |||
==References== | ==References== | ||
[https://en.wikipedia.org/wiki/Voltage Voltage]<div></div> | *[https://en.wikipedia.org/wiki/Voltage Voltage]<div></div> | ||
[http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference Potential Difference]<div></div> | *[http://www.physicsclassroom.com/class/circuits/Lesson-1/Electric-Potential-Difference Potential Difference]<div></div> | ||
[http://www.schoolphysics.co.uk/ | *[http://www.schoolphysics.co.uk/age1619/Electricity%20and%20magnetism/Current%20electricity/text/Potential_and_potential_difference/index.html Potential and Potential Difference]<div></div> | ||
[http://www.physicsclassroom.com/class/circuits/Lesson-4/Parallel-Circuits Circuits] | *[http://www.physicsclassroom.com/class/circuits/Lesson-4/Parallel-Circuits Circuits] | ||
Latest revision as of 17:32, 14 October 2019
Claimed and Written by Daniel Kurniawan for PHYS2212
Electric Potential Difference, also known as voltage, is the difference in electric potential energy between two points per unit of electric charge. The voltage between two points is equal to the work done per unit of charge against an unchanging electric field to move the charge between two points and is measured in volts.
Voltage can be caused by static electric fields, by electric current through a magnetic field, by time-varying magnetic fields, or some combination of these three. One can use a voltmeter to measure the potential difference between two points in a circuit. A voltage may represent either a source of energy (electromotive force), or lost, used, or stored energy (potential drop).
The Main Idea
Say you have two points "A" and "B" in space. The potential difference is defined as the difference in electric potential between those two points. Electric potential is electric potential energy per unit charge, measured in joules per coulomb (J/C), otherwise known as volts.
Circuits
Potential difference is typically used in describing the voltage dropped across some sort of electrical device, such as a resistor. The voltage drop across the device is the difference between measurements at each terminal of the device with respect to a common reference point. The voltage drop is the difference between the two readings. Two points in an electric circuit that are connected by an ideal conductor without resistance and not within a changing magnetic field have a voltage of zero. Any two points with the same potential may be connected by a conductor and no current will flow between them.
Potential Difference in a Series Circuit
In a series circuit, the potential difference supplied by the battery is divided up between the components. If the components all have the same resistance they will have equal amounts of potential difference across them. If the resistances are not equal, they may have different amounts of potential difference (See Ohm's Law) across them but when added up they must always equal the potential difference supplied by the battery.
Potential Difference in a Parallel Circuit
In a parallel circuit,the potential difference supplied by the battery is the same potential difference as that across each of the components in the circuit. If three resistors are placed in parallel branches and powered by a 12-volt battery, then the voltage drop across each one of the three resistors is 12 volts. A charge flowing through the circuit would only encounter one of these three resistors and thus encounter a single voltage drop of 12 volts.
A Mathematical Model
[math]\displaystyle{ \Delta V_{BA} = V(x_B) - V(x_A) = - \int_{r_0}^{x_B} \vec{E} \cdot d\vec{l} - \left( - \int_{r_0}^{x_A} \vec{E} \cdot d\vec{l} \right) = \int_{x_B}^{r_0} \vec{E} \cdot d\vec{l} + \int_{r_0}^{x_A} \vec{E} \cdot d\vec{l} = \int_{x_B}^{x_A} \vec{E} \cdot d\vec{l} }[/math]
As seen above, the potential difference from one point to another in space is calculated as the path integral of the electric field and the time rate of change of magnetic field along that path (alternate way - multiply electric field times the distance covered across the two points). The voltage between point A to point B is equal to the work which would have to be done, per unit charge, against or by the electric field to move the charge from A to B. The voltage between the two ends of a path is the total energy required to move a small electric charge along that path, divided by the magnitude of the charge. Both an unchanging electric field and a dynamic electromagnetic field must be included in determining the voltage between two points. Check out this YouTube Video that shows how to calculate potential, potential difference, and voltage in a system.
Potential difference is defined in such a way that negatively charged objects are pulled towards higher voltages, while positively charged objects are attracted towards lower voltages. This means that the conventional current in a system always flows from higher voltage to lower voltage. Current can flow from lower voltage to higher voltage, but only when there is some source of energy present to push it against the opposing electric field. For example, inside a battery, chemical reactions provide the energy needed for ion current to flow from the negative to the positive terminal.
A Computational Model
John Travoltage is a model for voltage using his body as the circuit.
Kirchoff's Voltage Law
One of Kirchoff's Circuit Laws (more specifically the Voltage Law) can be used to calculate the various voltages within a circuit. For example, the voltage between points A and C is the sum of the voltage between A and B and the voltage between B and C. The various voltages can be calculated using Kirchoff's Voltage Law, which states that the directed sum of the electrical potential differences around any closed network is zero. Essentially, the sum of the potential differences in any closed loop is equivalent to the sum of the potential drops in that loop.
[math]\displaystyle{ \sum_{k=1}^n V_k = 0 }[/math]
Examples
Simple
Question
What are the equations for voltage based on the loop rule for loop 1 and loop 2?
In the figure above, the total voltage around loop 1 should sum to zero, as does the total voltage in loop 2. Also, the loop which consists of the outer part of the circuit (the path ABCD) should also sum to zero, as shown by Kirchoff's Voltage Law.
Solution
Middling
Question
Solution
Difficult
Question
Solution
See Also
Further Reading
External Links
- Kirchoff's Voltage Law
- Electric Potential Difference
- Calculating Potential, Potential Difference, and Voltage
- Potential Difference as a Path Integral