prev

next

of 37

View

51Download

0

Embed Size (px)

DESCRIPTION

Magnetism Alternating-Current Circuits. Alternating Current Generators. A coil of area A and N turns rotating with constant angular velocity in a uniform magnetic field produces a sinusoidal emf. Alternating current motor. - PowerPoint PPT Presentation

Transcript

Magnetism Alternating-Current Circuits

Alternating Current Generators Alternating current motorA coil of area A and N turns rotating with constant angular velocity in a uniform magnetic field produces a sinusoidal emf Instead of mechanically rotating, we can apply an ac potential difference generated by other ac generator to the coil. This produces an ac current in the coil, and the magnetic field exerts forces on the wires producing a torque that rotates the coil.

The magnetic field. Magnetic forces on moving charges. Magnetic forces on a current elementTorques on current loops and magnets

The Magnetic FieldMagnetsThe Earth is a natural magnet with magnetic poles near the north and south geographic poles.

The Magnetic FieldMagnetsDoes an isolated magnetic pole exist?The SI units of magnetic field is the tesla [T]Earth magnetic field is about 10-4 TPowerful laboratories produce fields of 1 -2 T as a maximum1 Gauss [G] = 10-4 Tesla [T]

The Magnetic Field

The Magnetic Field. Magnetic force on a moving chargeA proton is moving in a region of crossed fields E = 2x105 N/C and B = 3000 G, as shown in the figure. (a) What is the speed of the proton if it is not deflected. (b) If the electric field is disconnected, draw the path of the proton

The Magnetic Field. Magnetic force on a current elementIn the case of a straight segment of length L

The Magnetic Field. Torques on Current loops and MagnetsA circular loop of radius 2 cm has 10 turns of wire and carries a current of 3 A. The axis of the loop makes an angle of 30 with a magnetic field of 8000 G. Find the magnitude of the torque on the loop. BA current-carrying loop experiences no net force in a uniform magnetic field, but it does experience a torque that tends to twist the loop

Sources of Magnetic Field The Magnetic Field of Moving Charges The Magnetic Field of Currents. The Biot-Savart LawThe Magnetic Field Due to a Current loop

Sources of Magnetic FieldMoving Point Charges are the source of Magnetic Field

A solenoid is a wire tightly wounded into a helix of closely space turns . A solenoid is used to produce a strong, uniform magnetic field in the region surrounded by the loopsFor a long solenoidFind the magnetic field at the center of a solenoid of 600 turns, length 20 cm; radius 1.4 cm that carries a current of 4 ASources of Magnetic FieldA solenoidIn this figure, the length is ten times longer than the radiusn = N/L; N number of turns; L : length of solenoid

Sources of Magnetic Field: Solenoid and magnetsLeft: Magnetic field lines of a solenoid; right Magnetic field lines of a bar magnet

Magnetic Induction Magnetic Flux Induced EMF and Faradays LawLenzs Law

MAGNETIC INDUCTIONIn 1830, Michel Faraday in England and Joseph Henry in the USA independently discovered that in a changing magnetic field, a changing magnetic flux through a surface bounded by a stationary loop of wire induces a current in the wire: emf induced and induced current. This process is known as induction. In a static magnetic field, a changing magnetic flux through a surface bounded by a moving loop of wire induces an emf in the wire: motional emfMagnetic flux through a surface bounded by a loop of wire. The SI unit for magnetic flux is weber [Wb] 1Wb= 1 Tm2Find the magnetic flux through a 40 cm long solenoid with a 2.5 cm radius and 600 turns carrying a current of 7.5 A.

The induced emf is in such direction as to oppose, or tend to oppose, the change that produces it. Lenzs LawMAGNETIC INDUCTION

The coil with many turns of wire gives a large flux for a given current in the circuit. Thus, when the current changes, there is a large emf induced in the coil opposing the change. This self-induced emf is called a back emfMAGNETIC INDUCTION

Eddy Currents Heat produced by eddy currents constitute a power loss in a transformer. But eddy currents have some practical applications: damping mechanical oscillations, magnetic braking system

Inductance Self-inductanceThe SI unit of inductance is the henry [H]1 H = 1 Wb/A= 1 T.m2.A-1Find the self-inductance of a solenoid of length 10 cm, area 5 cm2, and 100 turns

Magnetic Energy

Alternating Current Generators Alternating current motorA coil of area A and N turns rotating with constant angular velocity in a uniform magnetic field produces a sinusoidal emf Instead of mechanically rotating, we can apply an ac potential difference generated by other ac generator to the coil. This produces an ac current in the coil, and the magnetic field exerts forces on the wires producing a torque that rotaes the coil.

Alternating Current Generators A coil of area A and N turns rotating with constant angular velocity in a uniform magnetic field produces a sinusoidal emf

Alternating Current Circuits: Alternating current in a ResistorInductors in Alternating Currents Capacitors in Alternating Currents

Potential drop across the resistor, VR Current in the resistor I Power dissipated in the resistor, P Average power dissipated in the resistor PaverageAlternating currents in a Resistor

Root-Mean-Square Values

Inductors in Alternating Current CircuitsThe potential drop across the inductor led the current 90 (out of phase)Instantaneous power delivered by the emf to the inductor is not zeroThe average power delivered by the emf to the inductor is zero.INDUCTIVE REACTANCE

Inductors in Alternating Current CircuitsInstantaneous power delivered by the emf to the inductor is not zeroThe average power delivered by the emf to the inductor is zero.INDUCTIVE REACTANCEThe potential drop across a 40-mH inductor is sinusoidal with a peak potential drop of 120 V. Find the inductive reactance and the peak current when the frequency is (a) 60 Hz, and (b) 2000 Hz

Capacitors in Alternating Current CircuitsThe potential drop lags the current by 90Power delivered by the emf in the capacitor: Instantaneous and averageCAPACITIVE REACTANCE

Driven RLC CircuitsSeries RLC circuit

The Kirchhoffs rules govern the behavior of potential drops and current across the circuit. When any closed-loop is traversed, the algebraic sum of the changes of potential must equal zero (loops rule)At any junction (branch point) in a circuit where the current can be divided, the sum of the currents into the junction must equal the sum of the currents out of the junction (junction rule)

Series RLC circuits

Power delivered to the series RLC circuitPower factor: cos

Series RLC circuitsA series RLC circuit with L = 2 H, C =2 F and R=20 is driven by an ideal generator with a peak emf of 100 V and a frequency of 60 Hz, find (a) the current peak (b) the phase (c) the power factor, (d) the average power delivered; (e) the peak potential drop across each element

Phasors Potential drop across a resistor can be represented by a vector VR, which is called a phasor. Then, the potential drop across the resistor IR, is the x component of vector VR, Potential drop across a series RLC circuit

In the circuit shown in the figure, the ac generator produces an rms voltage of 115 V when operated at 60 Hz. (a) What is the rms current in the circuit (b) What is the power delivered by the ac generator (c) What is the rms voltage across: points AB; points BC; points CD; points AC; points BD?.A certain electrical device draws 10 A rms and has an average power of 720 W when connected to a 120-V rms 60-Hz power line. (a ) What is the impedance of the device? (b) What series combination of resistance and reactance is this device equivalent to? (c) If the current leads the emf, is the reactance inductive or capacitive?

The Transformer Because of the iron core, there is a large magnetic flux through each coil, even when the magnetizing current Im in the primary circuit is very small . The primary circuit consists of an ac generator and a pure inductance (we consider a negligible resistance for the coil). Then the average power dissipated in the primary coil is zero. Why?: The magnetizing current in the primary coil and the voltage drop across the primary coil are out of phase by 90Secondary coil open circuit The potential drop across the primary coil isIf there is no flux leakage out of the iron core, the flux through each turn is the same for both coils, and thenA transformer is a device to raise or lower the voltage in a circuit without an appreciable loss of power. Power losses arise from Joule heating in the small resistances in both coils, or in currents loops (eddy currents) within the iron core. An ideal transformer is that in which these losses do not occur, 100% efficiency. Actual transformers reach 90-95% efficiency

The Transformer However, the potential drop in the primary is determined by the generator emf According to this, the total flux in the iron core must be the same as when there is no load in the secondary. The primary coil thus draws an additional current I1 to maintain the original flux turn. The flux through each turn produced by this additional current is proportional to N1I1. Since this flux equals turn, the additional current I1 in the primary is related to the current I2 in the secondary byThese curents are 180 out of phase and produce counteracting fluxes. Since I2 is in phase with V2, the additional current I1 is in phase with the poten