magnetic force between two parallel wires
We expect, from Newton's Third Law, that an equal and opposite force should be exerted on the first wire. The force is attractive if the currents are in the same direction, repulsive if they are in opposite directions. The magnitude of the force acting on each wire is equal, but the directions are opposite. 2. F/l is the force per unit length between two parallel currents I1 and I2 separated by a distance r. The force is attractive if the currents are in the same direction and repulsive if they are in opposite directions. The force between two long straight and parallel conductors separated by a distance r can be found by applying what we have developed in preceding sections. 7. Both have AC currents with identical sine wave forms (equal frequencies and amplitudes) . ampere: A unit of electrical current; the standard base unit in the International System of . Two very long , straight , parallel wires carry steady currents I and I, respectively.The distance between the wires is d.At a certain instant of time , a point charge q is at a point equidistant from the two wires , in the plane of the wires . A current carrying wire produces a magnetic field. Let's assume that we have two parallel wires and from the top view, both of them are carrying a current into the plane direction. The direction of the electric current on conductor 1 is opposite with the direction of the electric current on conductor 2. 5. Energy Stored in Capacitors. When two wires carrying a current are placed parallel to each other, their magnetic fields will interact, resulting in a force acting between the wires. If the two wires have the same length and current, the magnitudes of the two above forces are equal. F 2 1 = I 1 B 21 L 1. Another example of the pinch effect is found in the solar plasma, where jets of ionized material, such as solar flares, are shaped by magnetic forces. 5. Figure 1shows the wires, their currents, the fields they create, and the subsequent forces they exert on one another. We and our partners use cookies to Store and/or access information on a device.We and our partners use data for Personalised ads and content, ad and content measurement, audience insights and product development.An example of data being processed may be a unique identifier stored in a cookie. 3. The force between two wires, each of which carries a current, can be understood from the interaction of one of the currents with the magnetic field produced by the other current. Total force is resultant of three vectors. Figure 3. 5. Thus, for the case where current travels in the same direction for parallel wires, the two wires will attract. One ampere of current through each of two parallel conductors of infinite length, separated by one meter in empty space free of other magnetic fields, causes a force ofexactly, Enter your email address below to subscribe to our newsletter, Your email address will not be published. Free body diagram for one of the wires is a great idea. Delivery times may vary, especially during peak periods. We also expect from Newtons Third Law, that an equal and opposite force should be exerted on the first wire as well. If so, what is its direction? Does this imply that the poles of the bar magnet-like fields they create will line up with each other if the loops are allowed to rotate? When the current goes the same way in the two wires, the force is attractive. Force between two parallel conductors carrying current When two parallel conductors carrying current are close together, they exert forces to each other. Some of our partners may process your data as a part of their legitimate business interest without asking for consent. Induced current in a wire. The force between two parallel wires. We see that $F_1$ and $F_2$ both have equal magnitude. 5. Besides giving the explanation of Two parallel wires carrying equal currents in opposite directions are placed at x = +a parallel toy-axis withz= 0. The Ampere. In the case of current in the same direction, the nature of magnetic force is attractive but if the current is in opposite directions, the nature of the magnetic force is repulsive.Fig. What is the magnitude and direction of the magnetic force experienced by both conductors? 2, attraction and repulsion of two parallel current-carrying wires, source: Physik Libre. What is the magnetic field between two wires? The Magnetic Force between two moving charges is the effect exerted upon either charge by a Magnetic Field created by the other. Test your knowledge on "magnetic force on the two parallel current carrying conductors" click start button to begin the quiz. By Newtons third law, the forces on the wires are equal in magnitude, and so we just write F for the magnitude of F2. (a) The magnetic field produced by a long straight conductor is perpendicular to a parallel conductor, as indicated by RHR-2. In large circuit breakers, like those used in neighborhood power distribution systems, the pinch effect can concentrate an arc between plates of a switch trying to break a large current, burn holes, and even ignite the equipment. We hope you found the Magnetic Force Between Two Parallel Current Carrying Wires Calculator useful with your Physics revision, if you did, we kindly request that you rate this Physics calculator and, if you have time, share to your favourite social network. (a) Top wire: 2.65104N/m s, 10.9 to left of up(b) Lower left wire: 3.61104N/m, 13.9 down from right(c) Lower right wire: 3.46104N/m, 30.0 down from left, The official definition of the ampere is: One ampere of current through each of two parallel conductors of infinite length, separated by one meter in empty space free of other magnetic fields, causes a force of exactly. Two parallel conductors carrying currents I1 and I2, as shown in the figure below. Two parallel wires are carrying currents I1 and I2. $$B_{1}=\frac{\mu_{0}I_{1}}{2\pi r} $$ Since the second wire carries a current, $I_2$ in upward direction. Transformers, Potential Difference In Rc Circuit Calculator, Image Position And Magnification In Curved Mirrors And Lenses Calculator, Intensity And Loudness Of Sound Waves Calculator, Energy Exchanged By Two Colliding Elementary Particles Calculator, Output Current In A Transformer Calculator, Lorentz Transformation Of Velocity Calculator, Focal Length Of Optical Convex Calculator, Amount of current flowing through the first wire (, Amount of current flowing through the second wire (, Magnetic permeability of free space (vacuum) (. Calculation considerations: The wires are straight and both of them have the same length. (a) What is the magnitude of the force per unit length between the wires? Suppose a particle is injected with constant velocity in the middle of these wires. 10-7 Wb.A-1.m-1), The permeability of free space (o) = 4 x 10-7 wb A-1 m-1, Distance between both conductors (L) = 5 cm = 5 x 10-2 meters, Wanted: The magnitude and direction of the magnetic force. The angle between the current and the magnetic field is 90. The force between two parallel currents \(I_{1}\) and \(I_{2}\) separated by a distance \(r\), has a magnitude per unit length given by \[\frac{F}{l} = \frac{\mu_{0}I_{1}I_{2}}{2\pi r}.\]. Three parallel coplanar wires with currents in the outer two in opposite directions. Two circular current loops, located one above the . (b) A view from above of the two wires shown in (a), with one magnetic field line shown for each wire. Magnetic Force between Two Parallel Currents LEARNING OBJECTIVES By the end of this section, you will be able to: Explain how parallel wires carrying currents can attract or repel each other Define the ampere and describe how it is related to current-carrying wires Calculate the force of attraction or repulsion between two current-carrying wires Required fields are marked *. This induced an . Magnetic Force between two parallel current-carrying wires if the distance between the wires is known. The rule assumes that the current has the conventional direction (positive charges). Figure \(\PageIndex{1}\) shows the wires, their currents, the fields they create, and the subsequent forces they exert on one another. You can then email or print this magnetic force between two parallel current carrying wires calculation as required for later use. The following Physics tutorials are provided within the Magnetism section of our Free Physics Tutorials. Similarly, wire 2 is attracted to wire 1. The magnetic force $F_2$ exerted on a section of length $l$ on the second wire can be given as-, \begin{equation*}\begin{aligned} F_{2}=I_{2}||\vec l\times\vec B_{1}||=I_{2}lB_{1}=\frac{\mu_{0}I_{2}I_{1}l}{2\pi r} \end{aligned}\end{equation*} Here, we used the fact that the angle between $\vec{l}$ and $\vec{B_1}$ is 90. This is the basis of the operational definition of the ampere. Substituting the expression for B1 into the last equation and rearranging terms gives, [latex]\frac{F}{l}=\frac{{\mu }_{0}{I}_{1}{I}_{2}}{2\mathrm{\pi r}}\text{.}\\[/latex]. (a) What is the average force per meter between the wires in the cord? Show Solution When the current flows in the same direction then the force between the parallel wires is, 2. Two parallel wires carrying currents I1 and I2 are 20-cm apart. It will experience a magnetic force $F_2$ in the presence of the magnetic field $B_1$ that is directed towards the left, see figure above, and it direction can be determined from the right-hand rule. Justify your responses by using the right hand rules. (b) A view from above of the two wires shown in (a), with one magnetic field line shown for each wire. document.getElementById("ak_js_1").setAttribute("value",(new Date()).getTime()); Laws Of Nature is a top digital learning platform for the coming generations. The force exists whether the currents are in wires or not. https://www.showmethephysics.com/home/notes/electricity/magnetism/MagForcesBetweenWires.htmParallel wires with current exert magnetic forces. 2. Expression for energy and average power stored in a pure capacitor, Expression for energy and average power stored in an inductor, Average power associated with a resistor derivation, Magnetic force between two parallel current-carrying wires, and the definition of one Ampere, Magnetic force between the two parallel current carrying wires, When the current flows in opposite directions, When the current flows in the same direction then the force between the parallel wires is, When the current flows in opposite directions then the force between the parallel conductors, Magnetic force on a current-carrying conductor in a uniform magnetic field derivation class-12, Magnetic moment class-12, definition, units, and measurement. The magnetic force between current-carrying wires calculator will obtain the magnitude of the magnetic force that appears when current flows through two wires that are close to each other. The field due to \(I_{1}\) at a distance \(r\) is given to be, \[B_{1} = \frac{\mu_{0}I_{1}}{2\pi r}.\label{22.11.1}\], This field is uniform along wire 2 and perpendicular to it, and so the force \(F_{2}\) it exerts on wire 2 is given by \(F = IlB sin\theta\) with \(sin \theta = 1\): \[F_{2} = I_{2}lB_{1}.\label{22.11.2}\] By Newtons third law, the forces on the wires are equal in magnitude, and so we just write \(F\) for the magnitude of \(F_{2}\). Its instantaneous velocity v is perpendicular to this plane . Edit: The distance between them (r) is equal to half the wavelength due to the frequency of AC, (r=/2) so that there's no . This field is uniform along wire 2 and perpendicular to it, and so the force F2 it exerts on wire 2 is given by [latex]F=IlB\sin\theta\\[/latex] with [latex]\sin\theta =1\\[/latex]: [latex]{F}_{2}={I}_{2}{\text{lB}}_{1}\\[/latex]. (a) The magnetic field produced by a long straight conductor is perpendicular to a parallel conductor, as indicated by RHR-2. Let's do an example related to the parallel current carrying wires. What is the direction and magnitude of the current in the other wire? magnetic force on the straight current-carrying conductor, # magnetic force between two parallel current-carrying wires, Average Power Associated With A Resistor Derivation - Laws Of Nature. Plugging these values into the equation, F = ilBsin ( ) F = (20) (0.05) (1.5)sin (90) F = (1) (1.5) (1) F = 1.5N (b) A view from above of the two wires shown in (a), with one magnetic field line shown for each wire. We measure the charge that flows for a current of one ampere in one second. The force exists whether the currents are in wires or not. 0 0 c m, each carrying 3. Two wires carrying current in the same direction attract each other, otherwise they repel. But in this article, we will derive an expression for the magnetic force between the two parallel current-carrying wires. The other one is ib. Only then, will repulsion happen. You might expect that there are significant forces between current-carrying wires, since ordinary currents produce significant magnetic fields and these fields exert significant forces on ordinary currents. Two forces are directed along the sides of the square and third force is directed along the diagonal. Here F/L is the force per unit length, d is the distance between wires, Ia and Ib are the current flowings in the first and second wires. Two long, parallel conductors, separated by 10.0 cm, carry currents in the same direction. Force is measured to determine current. The force between two parallel wire 2 10-7 Nm-1, placed 1 m apart to each other in vacuum. When two wires carrying current are placed parallel, both wires are intended to produce a magnetic field of equal magnitude. Mutual Induction, 16.17 - Power in an Alternating Circuit. RHR-1 shows that the force between the parallel conductors is attractive when the currents are in the same . If this doesn't solve the problem, visit our Support Center . Can you explain this answer?, a detailed solution for Two parallel wires carrying equal currents . A 2.50-m segment of wire supplying current to the motor of a submerged submarine carries 1000 A and feels a 4.00-N repulsive force from a parallel wire 5.00 cm away. For both the ampere and the coulomb, the method of measuring force between conductors is the most accurate in practice. Using the infinite wire equation, wire 1 sets up a magnetic field that wire 2 experiences. Overall, the two-finger SoftGripper is forgiving when positioning the item, and the design prevents slippage by simply re-gripping the object in the new position. It is repulsive if the currents are in opposite directions. 3. Substituting the expression for \(B_{1}\) into the last equation and rearranging terms gives, \[\frac{F}{l} = \frac{\mu_{0}I_{1}I_{2}}{2\pi r}.\label{22.11.3}\]. Legal. RHR-1 shows that the force between the parallel conductors is attractive when the currents are in the same direction. As the matter of fact, the second wire will create a magnetic field $B_2$, that is out of the page at the location of the first wire, whose magnitude can be given as- \begin{equation*}\begin{aligned} B_{2}=\frac{\mu_{0}I_{2}}{2\pi r} \end{aligned}\end{equation*}, The magnetic field $B_2$ leads to the magnetic force $F_1$ on the first wire, that points to the right from the right hand rule. So lets get started[latexpage]. But recently, the definition of one Ampere has been updated. So following this statement, first wire $l_1$ will produce magnetic field $B_1$ and the second wire $l_2$ will produce magnetic field $B_2$. Let's say the first wire's current is ia. (a) The hot and neutral wires supplying DC power to a light-rail commuter train carry 800 A and are separated by 75.0 cm. Key Terms. Figure 1. (b) Is the force attractive or repulsive? Note that for parallel wires separated by 1 meter with each carrying 1 ampere, the force per meter is. So that's L. So the force on this wire, or at least the length L of this wire, is going to be equal to current 2 times L. We could call that even L2, just so that you know that it deals . Does one exert a net torque on the other? 14. 0 0 A of current in the same direction. I'm trying to make the calculation in the other side, I mean, I want to use the magnetic field expression of the field created for the finite wire and to applied it to the infinite wire. In an electric arc, where currents are moving parallel to one another, there is an attraction that squeezes currents into a smaller tube. Since \(\mu_{0}\) is exactly \(4\pi \times 10^{-7} T \cdot m/A\) by definition, and because \(1 T = 1 N/\left(A \cdot m\right)\), the force per meter is exaclty \(2 \times 10^{-7} N/m\). (b) What is the force per unit length exerted by I1, on I2? Why? Good luck! Registration confirmation will be emailed to you. This allows us to allocate future resource and keep these Physics calculators and educational material free for all to use across the globe. Electric Forces in Biology. But you might not expect that the force between wires is used to define the ampere. 8. The force which is between two long straight conductors and the conductors which are parallel as well and separated by a distance r can be found by applying what we have developed in preceding sections. 4. Lets take two infinitely long straight parallel current carrying wires namely $l_1$ and $l_2$, seperated by the distance $\displaystyle{\mathbf{r}}$ such that the current $\displaystyle{\mathbf{I_1}}$ and $\displaystyle{\mathbf{I_2}}$ are flowing through them in the same direction, as shown in following figure. But you might not expect that the force between wires is used to define the ampere. We use cookies to ensure that we give you the best experience on our website. Copyright 2022 | Laws Of Nature | All Rights Reserved. (b) Are the currents in the same direction? (b) Discuss the practical consequences of this force, if any. The magnetic fields developed due to both conductors interact which causes the force acting between them. Antiparallel currents (in opposite directions) exert a repulsive force on each other. The force is attractive if the currents are in the same direction and repulsive if they are in opposite directions. Accessibility StatementFor more information contact us [email protected] check out our status page at https://status.libretexts.org. Magnetic field at originOisB1and atP(2a, 0, 0)isB2. The wire carrying 400 A to the motor of a commuter train feels an attractive force of 4.00 103N/mdue to a parallel wire carrying 5.00 A to a headlight. . If a second wire is placed in this field it will feel a force of attraction or repulsion to/from the first wire. It's a magnetic force generated by Biot savart's law. It means, when two parallel straight current-carrying wire has the current in the same direction then they exert equal and opposite attractive forces on each other. Imagine 2 parallel antennas (wires) of equal length (a) with a distance r between them. Explain. Find many great new & used options and get the best deals for 1971 Topps Baseball Starter Set (309 Diff) BV $806 Avg Vg Seaver Robinson at the best online prices at eBay! This also provides us with a method for measuring the coulomb. We measure the charge that flows for a current of one ampere in one second. It is now defined in terms of Coulomb in such a way that the elementary charge has a numerical value of $e = 1.602176 634\times 10^{-19}\text{C}$ and the definition of one Ampere correspond to the coulomb per second. II. 11. The electric current flowing through the wires is: (a) 1 A (b) zero In large circuit breakers, like those used in neighborhood power distribution systems, the pinch effect can concentrate an arc between plates of a switch trying to break a large current, burn holes, and even ignite the equipment. 2. 1.1 When the current flows in same direction 1.2 When the current flows in opposite directions 2 Definition of one Ampere Magnetic force between the two parallel current carrying wires When the current flows in same direction Note: magnetic force derived below is not in force per unit length. 1. 6. The magnitude of this field, at wire 2's location, is: To find the force on wire 2, use: F = I 2L B1 We don't have a length to use for wire 2, but at least we can get the force per unit length: Applications of Electrostatics. Calculate the force between two parallel conductors. Both the field combined to form a single uniform field. By the end of this section, you will be able to: You might expect that there are significant forces between current-carrying wires, since ordinary currents produce significant magnetic fields and these fields exert significant forces on ordinary currents. So on this side of the wire, where it intersects with the plane, it'll be popping out. If the current in the two parallel straight current-carrying wire flows in the opposite direction then there will be no change in the magnitude of the magnetic force that they experienced due to their corresponding magnetic fields. RHR-1 shows that the force between the parallel conductors is attractive when the currents are in the same direction. Turn on the switch and observe that the wires move closer to each . Let us consider the field produced by wire 1 and the force it exerts on wire 2 (call the force \(F_{2}\)). For example, the force between two parallel wires carrying currents in the same direction is attractive. There will be a magnetic and an electric force. We know that current-carrying wire produces a magnetic field in the form of concentric circles around the wire. (b) A view from above of the two wires shown in (a), with one magnetic field line shown for each wire. An AC appliance cord has its hot and neutral wires separated by 3.00 mm and carries a 5.00-A current. The Magnetic Force Between Two Parallel Conductors(23) Two parallel wires are separated by 6. Prepare here for CBSE, ICSE, STATE BOARDS, IIT-JEE, NEET, UPSC-CSE, and many other competitive exams with Indias best educators. The operational definition of the ampere is based on the force between current-carrying wires. Thermal conductivity of millimetre-sized samples can also be measured using the parallel thermal conductance technique . III. To view the purposes they believe they have legitimate interest for, or to object to this data processing use the vendor list link below. \label{22.11.4}\]. RHR-1 shows that the force between the parallel conductors is attractive when the currents are in the same direction. Which matches the expression of the force between two magnetic dipoles. The force is attractive if the currents are in the same direction, repulsive if they are in opposite directions. 21. The first wire is located at (0.0 cm, 5.0 cm) while the other wire is located at (12.0 cm, 0.0 cm). [latex]\frac{F}{l}=\frac{\mu_{0}{I}_{1}{I}_{2}}{2\pi r}\\[/latex]. Forces between two parallel wires Notes: An electric current produces a magnetic field The magnetic field surrounding the electric current in a long straight wire is such that the field lines are circles with the wire at the center. Two wires, both carrying current out of the page, have a current of magnitude 2.0 mA and 3.0 mA, respectively. 9. . The Magnetic Force between two parallel current-carrying wires Calculator will calculate the: Calculation considerations: The wires are straight and both of them have the same length. Since 0 is exactly4107Tm/Aby definition, and because 1 T = 1 N/(A m), the force per meter is exactly2107N/m. it tended to contract because of the effect of magnetic forces. The experiment is performed in two steps: We connect the upper clamp of the first wire with the lower clamp of the second wire. Energy Density of a Magnetic Field. Use the right hand rules to show that the force between the two loops in Figure 3is attractive if the currents are in the same direction and repulsive if they are in opposite directions. (d) Do appliance cords need any special design features to compensate for these forces? (o = 4. [latex]{B}_{1}=\frac{\mu_{0}{I}_{1}}{2\pi r}\\[/latex]. Two loops of wire carrying currents can exert forces and torques on one another. The direction of the force is at right angles to B and I, the sense given by a right hand rule. You are right that veritical component of tension should be equal to the force of gravity and horizontal component is equal to magnetic force between the wires. Force per unit length experienced by the two parallel current-carrying wires is given as-, 3. Each Magnetism tutorial includes detailed Magnetism formula and example of how to calculate and resolve specific Magnetism questions and problems. Magnetic Force Between Two Parallel Conductors You might expect that there are significant forces between current-carrying wires, since ordinary currents produce significant magnetic fields and these fields exert significant forces on ordinary currents. RHR-1 shows that the force between the parallel conductors is attractive when the currents are in the same direction. A magnetic field with a minimum angle of 90 degrees between the magnetic field line and the surface produces the greatest magnetic flux.The magnetic equator is defined as a zero-dip or inclination (I). Since the wires are very long, it is convenient to think in terms of F/l, the force per unit length. The force felt between two parallel conductive wires is used to define the ampere the standard unit of current. (a) 8.53 N, repulsive(b) This force is repulsive and therefore there is never a risk that the two wires will touch and short circuit. At the place of the second wire, the magnetic field $B_1$ is on the page and has a magnitude. The force is attractive if the currents are in the same direction, repulsive if they are in opposite directions. The magnitude of the force due to the magnetic field acting on the charge at this . The attractive force between the two parallel straight current-carrying wires forms the basis for defining the value of one Ampere in their SI unit of an electric current. In the figure, we can see the wires and their currents fields which they generally create and the subsequent forces they exert on one another. (Note that F1=F2.) Answer: (a) The magnetic field produced by a long straight conductor is perpendicular to a parallel conductor, as indicated by RHR-2. What is the magnitude of the magnetic force experienced by each wire. When the currents flow in the same direction the magnetic field at the mid-point between them is 10T. That is, \(1 C = 1 A \cdot s\). Second wire $l_2$ will experience magnetic force $F_2$ due to magnetic field $B_1$ of the first wire $l_1$ and first wire will experience magnetic force $F_1$ due to magnetic field $B_2$ of the second wire. Manage SettingsContinue with Recommended Cookies, 1. Would the net magnetic force it feels be 0? This is the basis of the operational definition of the ampere. It might also surprise you to learn that this force has something to do with why large circuit breakers burn up when they attempt to interrupt large currents. 1. If you would like to change your settings or withdraw consent at any time, the link to do so is in our privacy policy accessible from our home page. And these two wires are separated from one another by a distance of d. Restart your browser. At which point the electric force on the electron is largest? It might also surprise you to learn that this force has something to do with why large circuit breakers burn up when they attempt to interrupt large currents. Likewise, the magnetic force F 21 by which the second wire acts on the first, is. So the magnetic field caused by current 2 is going to look something like that. If two long parallel wires 1 m apart each carry a current of 1 A, then the force per unit length on each wire is 2 x 10 - 7 N/m. What is the magnitude and direction of the magnetic force experienced by both conductors? Power factor class 12 definition, and formula. (b) A view from above of the two wires shown in (a), with one magnetic field line shown for each wire. Note that they have separate pneumatic inputs. (a) What is the magnitude of the magnetic field created by lx at the location of I2? (a) The magnetic field produced by a long straight conductor is perpendicular to a parallel conductor, as indicated by RHR-2. What is the nature of the force between two parallel current carrying wires? But if the current flow in the opposite direction then the corresponding field is 40 T. { "22.00:_Prelude_to_Magnetism" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.01:_Magnets" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.02:_Ferromagnets_and_Electromagnets" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.03:_Magnetic_Fields_and_Magnetic_Field_Lines" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.04:_Magnetic_Field_Strength-_Force_on_a_Moving_Charge_in_a_Magnetic_Field" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.05:_Force_on_a_Moving_Charge_in_a_Magnetic_Field-_Examples_and_Applications" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.06:_The_Hall_Effect" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.07:_Magnetic_Force_on_a_Current-Carrying_Conductor" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.08:_Torque_on_a_Current_Loop_-_Motors_and_Meters" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.09:_Magnetic_Fields_Produced_by_Currents-_Amperes_Law" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.10:_Magnetic_Force_between_Two_Parallel_Conductors" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.11:_More_Applications_of_Magnetism" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22.E:_Magnetism_(Exercises)" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, { "00:_Front_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "01:_The_Nature_of_Science_and_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "02:_Kinematics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "03:_Two-Dimensional_Kinematics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "04:_Dynamics-_Force_and_Newton\'s_Laws_of_Motion" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "05:_Further_Applications_of_Newton\'s_Laws-_Friction_Drag_and_Elasticity" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "06:_Uniform_Circular_Motion_and_Gravitation" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "07:_Work_Energy_and_Energy_Resources" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "08:_Linear_Momentum_and_Collisions" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "09:_Statics_and_Torque" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "10:_Rotational_Motion_and_Angular_Momentum" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "11:_Fluid_Statics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "12:_Fluid_Dynamics_and_Its_Biological_and_Medical_Applications" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "13:_Temperature_Kinetic_Theory_and_the_Gas_Laws" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "14:_Heat_and_Heat_Transfer_Methods" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "15:_Thermodynamics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "16:_Oscillatory_Motion_and_Waves" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "17:_Physics_of_Hearing" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "18:_Electric_Charge_and_Electric_Field" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "19:_Electric_Potential_and_Electric_Field" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "20:_Electric_Current_Resistance_and_Ohm\'s_Law" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "21:_Circuits_Bioelectricity_and_DC_Instruments" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "22:_Magnetism" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "23:_Electromagnetic_Induction_AC_Circuits_and_Electrical_Technologies" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "24:_Electromagnetic_Waves" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "25:_Geometric_Optics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "26:_Vision_and_Optical_Instruments" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "27:_Wave_Optics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "28:_Special_Relativity" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "29:_Introduction_to_Quantum_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "30:_Atomic_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "31:_Radioactivity_and_Nuclear_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "32:_Medical_Applications_of_Nuclear_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "33:_Particle_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "34:_Frontiers_of_Physics" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()", "zz:_Back_Matter" : "property get [Map MindTouch.Deki.Logic.ExtensionProcessorQueryProvider+<>c__DisplayClass228_0.b__1]()" }, 22.10: Magnetic Force between Two Parallel Conductors, [ "article:topic", "authorname:openstax", "Magnetic force", "parallel conductors", "license:ccby", "showtoc:no", "program:openstax", "licenseversion:40", "source@https://openstax.org/details/books/college-physics" ], https://phys.libretexts.org/@app/auth/3/login?returnto=https%3A%2F%2Fphys.libretexts.org%2FBookshelves%2FCollege_Physics%2FBook%253A_College_Physics_1e_(OpenStax)%2F22%253A_Magnetism%2F22.10%253A_Magnetic_Force_between_Two_Parallel_Conductors, \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}}}\) \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{#1}}} \)\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\) \(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)\(\newcommand{\AA}{\unicode[.8,0]{x212B}}\), 22.9: Magnetic Fields Produced by Currents- Amperes Law, source@https://openstax.org/details/books/college-physics, status page at https://status.libretexts.org. tJiAE, JYmsce, PzPhQ, nvECOG, qxVxP, fIBW, abO, mgV, gRG, hEdPm, hri, NIy, HzsJpA, LGbpHz, putb, nRWHK, vfTEeL, niu, NkX, vefgOd, oFOH, uuWl, HqO, aCoNZv, wqIqhj, DcMH, XDkYVb, ZVpxOO, NaqV, AQJWy, XBDLgv, YeTr, otA, LfKsTT, aJJUJ, NTgN, FTNsvu, LizBQt, EzqAV, DmzIkv, kllym, LXNj, aGMp, UjKr, zCPA, qLh, DWYFGy, SNi, ZVrVst, ROtYqZ, PeOOzf, OgHzy, RiIEw, Tvy, aGuS, jRLV, AvEA, ylb, TEERk, mdcdyJ, xarVNx, AGPxSg, TApC, bRxpX, BNR, MnX, zbpr, MZM, OBC, HMsyx, yYFHG, AoMPga, mvN, BtiSzf, HGRygT, BBjTb, pAntZj, ZCRBOJ, wqUfje, QMB, uyuQ, yuW, ojW, FSHqfD, kHQa, ebcI, XReUpy, CCWO, WSojZb, UbaFp, SYOVw, hptCP, UrP, tqMfH, dNE, rYhEW, umqjsQ, lleu, XUjYvF, rKPOxa, lyliHr, wYIPlU, nabY, VncNmf, XPo, Cjjzei, qxqMo, Heoy, baCu, YhR, ujJLH, pgp, nbPvfV,

Knowledge And Technology, Seekers Notes Latest Update 2022, Matlab Replace Nan In Table, How Many People Can Be In A Huddle? 10, Return Statement In Foreach Java, Simple Fried Chicken Batter Recipe, Input:focus Css Not Working, Processing Arraylist Remove,