20 questions in 35 minutes, like Section I, marked with worked explanations.
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HSC Physics · Module 6 flashcards
101 cards. Work out each answer first, then open the card to check it and see the working.
Answer: induced currents in the copper produce fields that oppose the magnet's motion
The moving magnet changes the flux through the tube, inducing eddy currents. By Lenz's law these currents oppose the change that produced them, so they oppose the motion of the magnet.
Answer: zero
F = qvB sinθ. With θ = 0° there is no force; the particle continues in a straight line.
Answer: the plane of the coil is perpendicular to the field
Φ = BA cosθ where θ is between the field and the normal to the coil. Flux is greatest when the field passes straight through the coil face, i.e. the plane is perpendicular to the field.
Answer: reduce the current and so reduce I²R heating losses
For a given power P = VI, raising V lowers I. Power lost as heat is I²R, so lowering current cuts losses sharply.
Answer: 1.8 × 1014 m s-2
a = qE/m = 1.602 × 10-19 × 1000/9.109 × 10-31 = 1.8 × 1014 m s-2.
Answer: east
Right-hand rule: fingers along current (north), curl toward field (up), thumb gives force. North × up = east.
Answer: reverse the current in the coil every half turn so the torque keeps the same sense
Without reversal, the torque would flip direction every half turn and the coil would rock back and forth instead of rotating.
Answer: decreases because the back emf increases
The rotating coil cuts flux and induces a back emf that opposes the supply. Net voltage across the coil, and so current, falls as speed rises. Current is greatest at start-up or when stalled.
Answer: the rate of rotation of the coil
One rotation gives one full cycle of emf, so frequency equals the rotation frequency. Turns, field and area change the amplitude, not the frequency.
Answer: accelerates uniformly towards the negative plate, gaining kinetic energy qV
The field is uniform, so the force qE and acceleration are constant. Work done by the field over the full gap is qV.
Answer: inversely proportional to the separation
F/L = (μ0/2π)(I1I2/r). The 1/r dependence comes from the field of a long straight wire.
Answer: decreases
E = V/d. Larger d at fixed V gives a smaller field.
Answer: direction only
The magnetic force is always perpendicular to the velocity, so it does no work. Speed and kinetic energy are constant; only direction changes.
Answer: is independent of speed
T = 2πr/v and r = mv/qB, so T = 2πm/(qB). Faster particles move in bigger circles and take the same time.
Answer: 0.87 N
F = BIL sinθ = 0.050 × 10 × 2.0 × sin60° = 0.87 N.
Answer: doubles
ε = nBAω. The flux changes twice as fast, so the peak emf doubles (and the frequency doubles too).
Answer: 4.4 mm
t = 0.050/1.0 × 107 = 5.0 × 10-9 s. a = qE/m = 3.5 × 1014 m s-2. y = ½at² = 0.5 × 3.5 × 1014 × 2.5 × 10-17 = 4.4 × 10-3 m.
Answer: attract each other
Each wire lies in the other's field and the F = IL × B direction points towards the other wire for parallel currents.
Answer: straight, parallel and evenly spaced, from positive to negative
The field is uniform, so the lines are straight, equally spaced, and run from + to −.
Answer: 2 : 1
r = mv/(qB). The alpha has 4× the mass and 2× the charge, so r × 4/2 = 2.
Answer: the current is parallel to the field
F = BIL sinθ. sin0° = 0.
Answer: 1.0 cm
F/L = 2 × 10-7 I²/r, so r = 2 × 10-7 × 1/2.0 × 10-5 = 0.010 m.
Answer: zero (apart from a brief pulse when switched on or off)
A transformer needs a changing flux to induce an emf. Steady DC gives constant flux, so no continuous output.
Answer: a higher peak emf and a higher frequency
Faster rotation means the flux changes faster (bigger emf) and more cycles per second (higher frequency).
Answer: 2.5 × 104 N C-1
E = F/q = 4.0 × 10-15/1.602 × 10-19 = 2.5 × 104 N C-1.
Answer: 3.2 × 10-16 J
KE = qV = 1.602 × 10-19 × 2000 = 3.2 × 10-16 J.
Answer: 5.0 × 105 m s-1
qE = qvB gives v = E/B = 5.0 × 104/0.10 = 5.0 × 105 m s-1.
Answer: the plane of the loop is perpendicular to the field
When the plane is perpendicular to the field, the forces on opposite sides are in line with each other and produce no turning effect.
Answer: Lenz's law and the conservation of energy
The induced current opposes the motion. The work done against this opposing force is what provides the electrical energy — energy is conserved.
Answer: 6.4 × 10-17 J
W = qEd = 1.602 × 10-19 × 2.0 × 104 × 0.020 = 6.4 × 10-17 J.
Answer: a helix
The perpendicular component gives circular motion; the parallel component is unaffected. Combining them gives a helix along the field direction.
Answer: 4.0 × 10-4 N m-1
F/L = 2 × 10-7 × 100/0.050 = 4.0 × 10-4 N m-1.
Answer: higher voltage and lower current
Power is conserved: VpIp = VsIs. Stepping up V steps down I.
Answer: towards the bottom of the page
For a positive charge, v (right) × B (into page) gives a force towards the top. The electron is negative, so the force is towards the bottom of the page.
Answer: is greatest when the plane of the coil is parallel to the field and zero when perpendicular
τ = nIAB cosθ, θ being the angle between the coil plane and the field. The lever arm of the forces on the sides shrinks to zero when the coil is perpendicular to the field.
Answer: doubles
ε = nBAω. Emf is proportional to the number of turns.
Answer: 1.6 × 10-19 C (one electron)
qE = mg, so q = mg/E = 1.0 × 10-15 × 9.8/6.1 × 104 = 1.6 × 10-19 C.
Answer: the force is always perpendicular to the velocity
Work = F·s. A force perpendicular to the displacement transfers no energy, so the particle's speed is unchanged.
Answer: the back emf induced in the rotating coil opposes the supply voltage
The rotating coil is also a generator. Its induced emf opposes the supply, reducing the net voltage driving current.
Answer: one weber per square metre
Φ = BA, so B = Φ/A has units Wb m-2.
Answer: eddy currents induced in the disc that oppose its motion
Flux through each part of the disc changes as it spins, inducing eddy currents. By Lenz's law their effect opposes the rotation.
Answer: 5.9 × 106 m s-1
½mv² = qV, v = √(2qV/m) = √(2 × 1.602 × 10-19 × 100/9.109 × 10-31) = 5.9 × 106 m s-1.
Answer: the right-hand grip rule (thumb along current, fingers curl with field)
Point the right thumb along the conventional current; the curled fingers show the direction of the circular field lines.
Answer: 1.7 × 10-3 m
r = mv/(qB) = 9.109 × 10-31 × 3.0 × 106/(1.602 × 10-19 × 0.010) = 1.7 × 10-3 m.
Answer: 2.4 × 10-4 N m-1, repulsive
F/L = 2 × 10-7 × 24/0.020 = 2.4 × 10-4 N m-1. Opposite currents repel.
Answer: eddy current losses
Insulated thin sheets interrupt the paths of the circulating currents the changing flux would otherwise drive through a solid core.
Answer: a split-ring commutator instead of slip rings
Slip rings pass the alternating emf out unchanged. A split ring reverses the connection each half turn, so the output stays one polarity.
Answer: velocity parallel to the plates is constant and it accelerates towards one plate
The force is along the field only, so the perpendicular velocity component is unchanged while the parallel component grows uniformly — projectile-like motion.
Answer: 0.10 m
r = mv/(qB) = 6.64 × 10-27 × 1.0 × 106/(3.2 × 10-19 × 0.20) = 0.10 m.
Answer: to the right
F = IL × B. (into page) × (up) = to the right by the right-hand rule.
Answer: the commutator reverses the coil current every half turn
Reversing the current as the coil passes the vertical keeps the torque in the same rotational sense.
Answer: points out of the coil, opposing the increase
The induced effect always opposes the change in flux that caused it.
Answer: 2.0 × 104 N C-1
E = F/q = 0.040/2.0 × 10-6 = 2.0 × 104 N C-1.
Answer: 0.25 T
B = F/(qv) = 2.0 × 10-14/(1.6 × 10-19 × 5.0 × 105) = 0.25 T.
Answer: 8.0 × 10-3 N m-1
F/L = 2 × 10-7 × 400/0.010 = 8.0 × 10-3 N m-1.
Answer: the flux through the coil is maximum
Emf depends on the rate of change of flux. When flux is at its maximum (coil perpendicular to field) it is momentarily not changing.
Answer: zero
Moving along an equipotential (perpendicular to the field) involves no component of force along the displacement.
Answer: the same force and a much larger acceleration
F = qE is equal in magnitude (same |q|). a = F/m, and the electron's mass is about 1/1836 of the proton's, so it accelerates far more.
Answer: is larger
Faraday's law: emf is proportional to the rate of change of flux. Faster motion means faster flux change.
Answer: step up voltage at the power station and step down near consumers
High voltage for transmission minimises I²R losses; it is stepped down for safe domestic use.
Answer: upward towards the negative plate
A positive charge is attracted to the negative plate.
Answer: 0.60 N m
τ = nIAB = 200 × 0.50 × 0.020 × 0.30 = 0.60 N m.
Answer: clockwise, producing a field into the page inside the loop
Flux into the page is decreasing. Lenz's law: the induced current replaces it with a field into the page, which requires a clockwise current.
Answer: 50 Hz
The secondary emf follows the rate of change of the primary flux, so the frequency is unchanged. Only voltage and current change.
Answer: 1.9 × 107 m s-1
v = √(2qV/m) = √(2 × 1.602 × 10-16/9.109 × 10-31) = 1.9 × 107 m s-1.
Answer: 0°
F = BIL sinθ; sin0° = sin180° = 0. Current parallel or antiparallel to the field gives no force.
Answer: the conservation of energy
If induced currents aided the change instead of opposing it, a small push would create ever-growing motion and current — energy from nothing.
Answer: 1.6 × 10-16 J
V = Ed = 1.0 × 105 × 0.010 = 1000 V. KE = qV = 1.6 × 10-16 J.
Answer: perpendicular to both the current and the field
F = IL × B is perpendicular to the plane containing L and B.
Answer: 8.4 cm
r = mv/(qB) = 1.67 × 10-27 × 4.0 × 106/(1.6 × 10-19 × 0.50) = 0.084 m.
Answer: 4.8 × 10-5 N
F/L = 2 × 10-7 × 12/0.10 = 2.4 × 10-5 N m-1. F = 2.4 × 10-5 × 2.0 = 4.8 × 10-5 N.
Answer: 950 W
0.95 × 1000 = 950 W; the other 50 W becomes heat.
Answer: west
Field direction is defined by the force on a positive charge. A negative charge feels the opposite direction.
Answer: decreases
The field does positive work on it; potential energy converts to kinetic energy.
Answer: is unchanged
r = mv/(qB). Doubling both v and B leaves r the same.
Answer: parallel to the field
When parallel, the forces on the two sides act at the full width of the coil, giving the largest lever arm.
Answer: falls more slowly through the connected coil
An emf is induced in both, but only the closed coil carries a current and so only it exerts an opposing force (Lenz's law).
20 questions in 35 minutes, like Section I, marked with worked explanations.
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317 cards across Modules 5–8.
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