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22.7: Magnetic Force on a Current-Carrying Conductor

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  • Because charges ordinarily cannot escape a conductor, the magnetic force on charges moving in a conductor is transmitted to the conductor itself.

    Figure \(\PageIndex{1}\): The magnetic field exerts a force on a current-carrying wire in a direction given by the right hand rule 1 (the same direction as that on the individual moving charges). This force can easily be large enough to move the wire, since typical currents consist of very large numbers of moving charges.

    We can derive an expression for the magnetic force on a current by taking a sum of the magnetic forces on individual charges. (The forces add because they are in the same direction.) The force on an individual charge moving at the drift velocity \(v_{d}\) is given by \(F = qv_{d}B\sin \theta \). Taking \(B\) to be uniform over a length of wire \(l\) and zero elsewhere, the total magnetic force on the wire is then \(F = \left(qv_{d}B \sin \theta \right) \left(N\right)\), where \(N\) is the number of charge carriers in the section of wire of length \(l\). Now, \(N = nV\), where \(n\) is the number of charge carriers per unit volume and \(V\) is the volume of wire in the field. Noting that \(V = Al\), where \(A\) is the cross-sectional area of the wire, then the force on the wire is \(F = \left(qv_{d}B\sin\theta\right))\left(nAl\right)\). Gathering terms,

    \[F = \left(nqAv_{d}\right)lB\sin\theta . \label{22.8.1}\]

    Because \(nqAv_{d} = I\) (see Current),

    \[F = \pi B \sin \theta \label{22.8.1b}\]

    is the equation for magnetic force on a length \(l\) of wire carrying a current \(I\) in a uniform magnetic field \(B\), as shown in Figure \(\PageIndex{2}\). If we divide both sides of this expression by \(l\), we find that the magnetic force per unit length of wire in a uniform field is \(\frac{}{} = IB \sin \theta \). The direction of this force is given by RHR-1, with the thumb in the direction of the current \(I\). Then, with the fingers in the direction of \(B\), a perpendicular to the palm points in the direction of \(F\), as in Figure 2.

    Figure \(\PageIndex{2}\): The force on a current-carrying wire in a magnetic field is \(F = \pi B \sin \theta \). Its direction is given by RHR-1.

    Example \(\PageIndex{1}\): Calculating Magnetic Force on a Current-Carrying Wire: A Strong Magnetic Field

    Calculate the force on the wire shown in Figure \(\PageIndex{1}\), given \(B = 1.50 T\), \(l = 5.00 cm\), and \(I = 20.0 A\).


    The force can be found with the given information by using \(F = \pi B \sin\theta\) and noting that the angle \(\theta\) between \(I\) and \(B\) is \(90^{\circ}\), so that \(sin \theta = 1\).


    Entering the given values into \(F = \pi B \sin \theta\) yields

    \[F = \pi B \sin \theta = \left(20.0 A\right) \left(0.0500 m\right) \left(1.50 T\right) \left(1\right). \nonumber\]

    The units for tesla are \(1 T = \frac{N}{A \cdot m}\); thus,

    \[F = 1.50 \,N. \nonumber\]


    This large magnetic field creates a significant force on a small length of wire.

    Magnetic force on current-carrying conductors is used to convert electric energy to work. (Motors are a prime example—they employ loops of wire and are considered in the next section.) Magnetohydrodynamics (MHD) is the technical name given to a clever application where magnetic force pumps fluids without moving mechanical parts (Figure \(\PageIndex{3}\)).

    Figure \(\PageIndex{3}\): Magnetohydrodynamics. The magnetic force on the current passed through this fluid can be used as a nonmechanical pump.

    A strong magnetic field is applied across a tube and a current is passed through the fluid at right angles to the field, resulting in a force on the fluid parallel to the tube axis as shown. The absence of moving parts makes this attractive for moving a hot, chemically active substance, such as the liquid sodium employed in some nuclear reactors. Experimental artificial hearts are testing with this technique for pumping blood, perhaps circumventing the adverse effects of mechanical pumps. (Cell membranes, however, are affected by the large fields needed in MHD, delaying its practical application in humans.) MHD propulsion for nuclear submarines has been proposed, because it could be considerably quieter than conventional propeller drives. The deterrent value of nuclear submarines is based on their ability to hide and survive a first or second nuclear strike. As we slowly disassemble our nuclear weapons arsenals, the submarine branch will be the last to be decommissioned because of this ability (Figure \(\PageIndex{4}\)). Existing MHD drives are heavy and inefficient—much development work is needed.

    Figure \(\PageIndex{4}\):An MHD propulsion system in a nuclear submarine could produce significantly less turbulence than propellers and allow it to run more silently. The development of a silent drive submarine was dramatized in the book and the film The Hunt for Red October.


    • The magnetic force on current-carrying conductors is given by \[F = \pi B \sin \theta, \nonumber\] where \(\) is the current, \(l\) is the length of a straight conductor in a uniform magnetic field \(B\), and \(\theta\) is the angle between \(I\) and \(B\). The force follows RHR-1 with the thumb in the direction of \(I\).


    Paul Peter Urone (Professor Emeritus at California State University, Sacramento) and Roger Hinrichs (State University of New York, College at Oswego) with Contributing Authors: Kim Dirks (University of Auckland) and Manjula Sharma (University of Sydney). This work is licensed by OpenStax University Physics under a Creative Commons Attribution License (by 4.0).