Motional EMF xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx v B E - F E = -eE F B = -evB eE = evB E = vB V ind = LE = LvB

xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx v L d V t  i = LdB  f = L(d+v  t)B |V ind | =  /  t = Lv  tB/  t = LvB

Motional emf As the negative charges accumulate at the base, a net positive charge exists at the upper end of the conductor As the negative charges accumulate at the base, a net positive charge exists at the upper end of the conductor As a result of this charge separation, an electric field is produced in the conductor As a result of this charge separation, an electric field is produced in the conductor Charges build up at the ends of the conductor until the downward magnetic force is balanced by the upward electric force Charges build up at the ends of the conductor until the downward magnetic force is balanced by the upward electric force There is a potential difference between the upper and lower ends of the conductor There is a potential difference between the upper and lower ends of the conductor

Motional emf, cont The potential difference between the ends of the conductor can be found by The potential difference between the ends of the conductor can be found by V = B v LV = B v L The upper end is at a higher potential than the lower endThe upper end is at a higher potential than the lower end A potential difference is maintained across the conductor as long as there is motion through the field A potential difference is maintained across the conductor as long as there is motion through the field If the motion is reversed, the polarity of the potential difference is also reversedIf the motion is reversed, the polarity of the potential difference is also reversed

Motional emf in a Circuit Assume the moving bar has zero resistance Assume the moving bar has zero resistance As the bar is pulled to the right with velocity v under the influence of an applied force, F, the free charges experience a magnetic force along the length of the bar As the bar is pulled to the right with velocity v under the influence of an applied force, F, the free charges experience a magnetic force along the length of the bar This force sets up an induced current because the charges are free to move in the closed path This force sets up an induced current because the charges are free to move in the closed path

Motional emf in a Circuit, cont The changing magnetic flux through the loop and the corresponding induced emf in the bar result from the change in area of the loop The changing magnetic flux through the loop and the corresponding induced emf in the bar result from the change in area of the loop The induced, motional emf, acts like a battery in the circuit The induced, motional emf, acts like a battery in the circuit

Lenz’ Law Revisited – Moving Bar Example As the bar moves to the right, the magnetic flux through the circuit increases with time because the area of the loop increases As the bar moves to the right, the magnetic flux through the circuit increases with time because the area of the loop increases The induced current must in a direction such that it opposes the change in the external magnetic flux The induced current must in a direction such that it opposes the change in the external magnetic flux

Lenz’ Law, Bar Example, cont The flux due to the external field in increasing into the page The flux due to the external field in increasing into the page The flux due to the induced current must be out of the page The flux due to the induced current must be out of the page Therefore the current must be counterclockwise when the bar moves to the right Therefore the current must be counterclockwise when the bar moves to the right

Lenz’ Law, Bar Example, final The bar is moving toward the left The bar is moving toward the left The magnetic flux through the loop is decreasing with time The magnetic flux through the loop is decreasing with time The induced current must be clockwise to to produce its own flux into the page The induced current must be clockwise to to produce its own flux into the page

Lenz’ Law, Moving Magnet Example A bar magnet is moved to the right toward a stationary loop of wire (a) A bar magnet is moved to the right toward a stationary loop of wire (a) As the magnet moves, the magnetic flux increases with time The induced current produces a flux to the left, so the current is in the direction shown (b) The induced current produces a flux to the left, so the current is in the direction shown (b)

Lenz’ Law, Final Note When applying Lenz’ Law, there are two magnetic fields to consider When applying Lenz’ Law, there are two magnetic fields to consider The external changing magnetic field that induces the current in the loopThe external changing magnetic field that induces the current in the loop The magnetic field produced by the current in the loopThe magnetic field produced by the current in the loop

Generators Alternating Current (AC) generator Alternating Current (AC) generator Converts mechanical energy to electrical energyConverts mechanical energy to electrical energy Consists of a wire loop rotated by some external meansConsists of a wire loop rotated by some external means There are a variety of sources that can supply the energy to rotate the loopThere are a variety of sources that can supply the energy to rotate the loop These may include falling water, heat by burning coal to produce steam These may include falling water, heat by burning coal to produce steam

AC Generators, cont Basic operation of the generator Basic operation of the generator As the loop rotates, the magnetic flux through it changes with timeAs the loop rotates, the magnetic flux through it changes with time This induces an emf and a current in the external circuitThis induces an emf and a current in the external circuit The ends of the loop are connected to slip rings that rotate with the loopThe ends of the loop are connected to slip rings that rotate with the loop Connections to the external circuit are made by stationary brushed in contact with the slip ringsConnections to the external circuit are made by stationary brushed in contact with the slip rings

AC Generators, final The emf generated by the rotating loop can be found by The emf generated by the rotating loop can be found by V =2 B ℓ v  =2 B ℓ v sin θ If the loop rotates with a constant angular speed, ω, and N turns If the loop rotates with a constant angular speed, ω, and N turns V = N B A ω cos ω t V = V max when loop is parallel to the field V = V max when loop is parallel to the field V = 0 when when the loop is perpendicular to the field V = 0 when when the loop is perpendicular to the field

AC Generator

Angular velocity,  Amount of angle (radian) turned in a second  t = total angle of turn during time t 2  f =  period T = 1/f = 2  t = 0:  = 0 t1t1 t = t 1 :  = A B sin(t 1 ) V ind = - /t = - ABsin(t 1 )/t 1 V ind = - /t = - ABcos(t) AC generation

Hot Neutral GND

170 V -170 V When we say 120 V, it means rms value!! P  v 2 or i 2 v rms = 0.707v a

Power Transmission City of Gainesville has 120,000 population. On average approximately 200 W/person of electric power is required. Let’s assume that GRU transmit power with 120 V. How much current Should be carried in power line? P t = 120,000 x 200 W = 24,000,000 W = 24 MW P = IV, I = P/V = 24,000,000/120 = 200,000 A However, if we deliver power with 500,000 V, I = 24,000,000/500,000 = 48 A Now Joule heating due to wire resistance (R) is reduced By (48/200,000) 2 = 5.8 x 10 -8

Transformer Iron Core AC V NpNp NsNs V p /V s = N p /N s /t V p = -N p /t V s = -N s /t