Calculate current that to produce a magnetic field.Use the best hand ascendancy 2 to recognize the direction of current or the direction of magnetic ar loops.

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How much existing is essential to produce a far-reaching magnetic field, perhaps as strong as the earth’s field? Surveyors will certainly tell you that overhead electric power lines produce magnetic fields that interfere through their compass readings. Indeed, as soon as Oersted discovered in 1820 that a existing in a wire influenced a compass needle, he to be not taking care of extremely large currents. Just how does the shape of wires carrying current impact the shape of the magnetic field created? We provided earlier the a current loop developed a magnetic field comparable to that of a bar magnet, but what around a straight wire or a toroid (doughnut)? exactly how is the direction of a current-created field related to the direction that the current? Answers to these concerns are discover in this section, together with a short discussion that the legislation governing the fields produced by currents.

Magnetic fields have both direction and also magnitude. As provided before, one means to discover the direction that a magnetic field is v compasses, as shown for a lengthy straight current-carrying wire in number 1. Hall probes deserve to determine the magnitude of the field. The field roughly a long straight cable is discovered to be in one loops. The ideal hand ascendancy 2 (RHR-2) increase from this exploration and is valid for any current segment—point the ignorance in the direction the the current, and the fingers curly in the direction of the magnetic field loops developed by it.

Figure 1. (a) Compasses put near a lengthy straight current-carrying wire indicate that field lines kind circular loops centered on the wire. (b) ideal hand ascendancy 2 claims that, if the right hand thumb points in the direction that the current, the fingers curl in the direction that the field. This ascendancy is continuous with the field mapped because that the lengthy straight wire and is precious for any kind of current segment.

The magnetic ar strength (magnitude) produced by a lengthy straight current-carrying wire is found by experiment come be

B=\\frac\\mu_0I2\\pi r\\left(\\textlong directly wire\\right)\\\\,

where I is the current, r is the shortest street to the wire, and the constant \\mu _0=4\\pi \\times 10^-7\\textT\\cdot\\text m/A\\\\ is the permeability of free space. (μ0 is one of the simple constants in nature. We will certainly see later that μ0 is concerned the speed of light.) because the cable is an extremely long, the magnitude of the field depends just on distance from the wire r, not on position along the wire.

Find the current in a long straight wire the would develop a magnetic field twice the strength of the earth’s at a street of 5.0 centimeter from the wire.


The Earth’s field is about 5.0 × 10−5 T, and so below B because of the wire is taken to be 1.0 × 10−4 T. The equation B=\\frac\\mu_0I2\\pi r\\\\ can be offered to uncover I, because all other quantities space known.


Solving for I and entering recognized values gives

\\beginarraylllI& =& \\frac2\\pi rB\\mu _0=\\frac2\\pi\\left(5.0\\times 10^-2\\text m\\right)\\left(1.0\\times 10^-4\\text T\\right)4\\pi \\times 10^-7\\text T\\cdot\\textm/A\\\\ & =& 25\\text A\\endarray\\\\


So a moderately huge current produce a significant magnetic ar at a street of 5.0 centimeter from a long straight wire. Keep in mind that the price is declared to just two digits, since the Earth’s ar is specified to just two number in this example.

The magnetic field of a lengthy straight wire has more implications 보다 you might at first suspect. Each segment of present produces a magnetic field like that of a lengthy straight wire, and also the complete field of any type of shape present is the vector amount of the fields as result of each segment. The officially statement that the direction and also magnitude the the field as result of each segment is dubbed the Biot-Savart law. Integral calculus is required to amount the field for one arbitrary form current. This results in a much more complete law, referred to as Ampere’s law, i beg your pardon relates magnetic field and current in a basic way. Ampere’s law consequently is a part of Maxwell’s equations, which offer a finish theory of every electromagnetic phenomena. Considerations of how Maxwell’s equations show up to various observers brought about the contemporary theory that relativity, and the realization the electric and magnetic fields are various manifestations the the very same thing. Many of this is beyond the border of this text in both mathematical level, inquiry calculus, and also in the amount of an are that deserve to be specialized to it. But for the interested student, and specifically for those who proceed in physics, engineering, or similar pursuits, delving right into these matters additional will expose descriptions of nature that are elegant and also profound. In this text, us shall save the general attributes in mind, such as RHR-2 and also the rules because that magnetic ar lines listed in Magnetic Fields and also Magnetic field Lines, if concentrating top top the fields created in particular important situations.

Hearing all we do about Einstein, we sometimes acquire the impression that he invented relativity the end of nothing. On the contrary, one of Einstein’s motivations was to solve obstacles in discovering how different observers view magnetic and electric fields.

The magnetic ar near a current-carrying loop of wire is presented in number 2. Both the direction and also the size of the magnetic field developed by a current-carrying loop are complex. RHR-2 can be offered to provide the direction of the field near the loop, but mapping with compasses and also the rules around field lines provided in Magnetic Fields and Magnetic field Lines are essential for more detail. Over there is a straightforward formula because that the magnetic field strength at the center of a circular loop. That is

B=\\frac\\mu_0I2R\\left(\\textat center of loop\\right)\\\\,

where R is the radius the the loop. This equation is very comparable to that for a right wire, however it is precious only in ~ the center of a circular loop of wire. The similarity the the equations does indicate that similar field strength can be derived at the center of a loop. One means to get a larger ar is to have N loops; then, the field is 0I/(2R). Keep in mind that the larger the loop, the smaller the ar at that center, due to the fact that the existing is farther away.

Figure 2. (a) RHR-2 provides the direction of the magnetic field inside and also outside a current-carrying loop. (b) an ext detailed mapping through compasses or through a hall probe completes the picture. The field is similar to the of a bar magnet.

A solenoid is a lengthy coil of wire (with countless turns or loops, together opposed to a level loop). Since of that is shape, the field inside a solenoid deserve to be very uniform, and also also really strong. The field just exterior the coils is nearly zero. Figure 3 shows just how the ar looks and also how the direction is offered by RHR-2.

Figure 3. (a) since of that shape, the ar inside a solenoid of length l is substantial uniform in magnitude and also direction, as indicated by the straight and uniformly spaced field lines. The field outside the coils is nearly zero. (b) This cutaway shows the magnetic field generated through the current in the solenoid.

The magnetic field inside that a current-carrying solenoid is an extremely uniform in direction and magnitude. Only close to the ends does it begin to weaken and readjust direction. The field external has similar complexities to flat loops and bar magnets, yet the magnetic ar strength inside a solenoid is simply

B=\\mu _0nI\\left(\\textinside a solenoid\\right)\\\\,

where n is the variety of loops per unit length of the solenoid (N/l, v N being the number of loops and also l the length). Keep in mind that B is the field strength almost everywhere in the uniform region of the interior and also not simply at the center. Big uniform fields spread end a big volume are feasible with solenoids, as instance 2 implies.

What is the field inside a 2.00-m-long solenoid that has 2000 loops and carries a 1600-A current?


To uncover the ar strength inside a solenoid, we use B=\\mu _0nI\\\\. First, we keep in mind the number of loops every unit size is

n=\\fracNl=\\frac20002.00\\text m=1000\\text m^-1=10\\text cm^-1\\\\.

Solution Substituting recognized values gives

\\beginarraylllB & =& \\mu_0nI=\\left(4\\pi \\times 10^-7\\text T\\cdot\\textm/A\\right)\\left(1000\\text m^-1\\right)\\left(1600\\text A\\right)\\\\ & =& 2.01\\text T\\endarray\\\\


This is a large field stamin that might be created over a large-diameter solenoid, such as in clinical uses the magnetic resonance imaging (MRI). The very large current is one indication that the areas of this strength space not easily achieved, however. Such a big current v 1000 loops squeezed right into a meter’s size would produce significant heating. Higher currents deserve to be accomplished by utilizing superconducting wires, return this is expensive. Over there is an upper limit to the current, because the superconducting state is disrupted by very huge magnetic fields.

There are exciting variations that the flat coil and solenoid. Because that example, the toroidal coil offered to confine the reactive corpuscle in tokamaks is lot like a solenoid bent into a circle. The ar inside a toroid is very solid but circular. Fee particles travel in circles, following the ar lines, and collide through one another, maybe inducing fusion. Yet the fee particles do not cross field lines and escape the toroid. A whole range of coil shapes are supplied to create all sorts of magnetic ar shapes. Adding ferromagnetic materials produces greater ar strengths and also can have actually a significant effect top top the form of the field. Ferromagnetic products tend to catch magnetic areas (the ar lines bend into the ferromagnetic material, leaving weaker fields external it) and also are offered as shields for devices that are adversely affected by magnetic fields, consisting of the earth’s magnetic field.

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Section Summary

The toughness of the magnetic field developed by existing in a long straight cable is offered by

where I is the current, r is the shortest distance to the wire, and the constant\\mu_0=4\\pi \\times 10^-7\\text T\\cdot\\text m/A\\\\ is the permeability of complimentary space.The direction that the magnetic field developed by a long straight cable is provided by right hand dominion 2 (RHR-2): Point the thumb of the ideal hand in the direction that current, and the fingers curly in the direction the the magnetic field loops created by it.The magnetic field produced by current following any path is the amount (or integral) that the fields due to segments along the course (magnitude and also direction as for a directly wire), causing a basic relationship in between current and also field well-known as Ampere’s law.The magnetic ar strength in ~ the center of a one loop is provided by
where R is the radius the the loop. This equation becomes B = μ0nI/(2R) for a flat coil of N loops. RHR-2 offers the direction that the field around the loop. A lengthy coil is referred to as a solenoid.The magnetic ar strength inside a solenoid is
where n is the number of loops every unit size of the solenoid. The ar inside is very uniform in magnitude and also direction.

See more: Integumentary System Labeling Worksheet, Integumentary System Labeling Diagram

1. Do a drawing and also use RHR-2 to uncover the direction the the magnetic field of a present loop in a motor (such as in number 1 indigenous Torque ~ above a current Loop). Then show that the direction the the torque on the loop is the very same as created by choose poles repelling and also unlike poles attracting.


right hand dominance 2 (RHR-2):a ascendancy to recognize the direction that the magnetic ar induced through a current-carrying wire: suggest the ignorance of the best hand in the direction of current, and also the fingers curl in the direction the the magnetic field loopsmagnetic field strength (magnitude) created by a lengthy straight current-carrying wire:defined as B=\\frac\\mu_0I2\\pi r\\\\, wherein is the current, r is the shortest street to the wire, and μ0 is the permeability of complimentary spacepermeability of complimentary space:the measure up of the ability of a material, in this case complimentary space, to support a magnetic field; the constant \\mu_0=4\\pi \\times 10^-7T\\cdot \\textm/A\\\\magnetic ar strength at the center of a one loop:defined as B=\\frac\\mu _0I2R\\\\ where R is the radius of the loopsolenoid:a thin wire wound into a coil the produces a magnetic ar when an electric existing is passed through itmagnetic ar strength within a solenoid:defined as B=\\mu _0\\textnI\\\\ wherein n is the number of loops every unit length of the solenoid n = N/l, through N gift the number of loops andthe length)Biot-Savart law:a physical regulation that explains the magnetic ar generated by an electric current in terms of a details equationAmpere’s law:the physical law that states that the magnetic field about an electric existing is proportional come the current; each segment of existing produces a magnetic field like the of a long straight wire, and the complete field of any type of shape existing is the vector amount of the fields due to each segmentMaxwell’s equations:a set of 4 equations that define electromagnetic phenomena