6.7 Electromagnetic Induction - Lenz Law Flashcards Preview

A-Level Physics EDEXCEL Year 2 > 6.7 Electromagnetic Induction - Lenz Law > Flashcards

Flashcards in 6.7 Electromagnetic Induction - Lenz Law Deck (20)
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1
Q

What is Lenz Law?

A

‘the induced emf is always in such a direction as to oppose the change in flux that caused it’

2
Q

What is Lenz Law example of ?

A

Conservation of energy and Newton’s Third Law.

3
Q

How is Lenz Law an example of conservation of energy?

A

As when there is a change in flux linkage energy si transferred to induce emf. (work is done on charge carriers)

4
Q

How is Lenz Law an example of Newton’s Third Law?

A

As every action will try to be opposed by the creation of magnetic field in the wire.

5
Q

What is the equation for Lenz Law?

A

E = - nΦ / t

6
Q

What does the minus sign represent?

A

It shows the direction of emf and how the magnetic field created will try to exert a force to oppose change in magnetic flux / magnetic flux linkage.

7
Q

What is the induction rule, what does each finger represent?

A

the new right hand rule
THUMB = motion
FIRST FINGER = field
SECOND FINGER = direction of induced emf

8
Q

What would be direction of the current from this rule?

A

The same as direction of emf, second finger

9
Q

How do we use this rule for? What do we use it for?

A

We use this rule to work out direction of induced emf, then we can use fleming’s left hand rule to work out direction of resistance to motion.

10
Q

What is this resistance to motion created by?

A

Magnetic field of the emf induced wire, it is either magnetic attraction or repulsion.

11
Q

What would happen when a north pole of a bar magnet is approaching a coil of wire?

A

There would be and emf and therefore current induced. This creates a magnetic field around the coil in such a way that the closest side of coil to magnet will act as a north pole to oppose the motion.

12
Q

What would happen when withdrawing the magnet?

A

The current would backtrack and so the bar magnet will be attracted to the coil, as the coil of wire will be acting as a south pole.

13
Q

Using the practical from the book, for capturing induced emf what set up would we use?

A

A coil connected in series to a data logger that has a resistor between its poles.

14
Q

What do we do in this activity?

A

We drop a bar magnet through a coil and use the data logger to capture the pd across a time frame.

15
Q

What would an emf over time graph look like?

A

Start at 0, then increase until reaching peak, then drop in a straight line peak on the negative y-axis and increase to 0.

16
Q

In what case would the 2 peaks (in the negative and positive direction ) equal?

A

As long as the bar magnet is dropped through the centre of the coil.

17
Q

Why does the emf become negative?

A

When magnet starts to exit the coil , this happens as current backtracks changing the magnetic flux / magnetic flux linkage.

18
Q

What would be the conclusion of the peaks not being equal?

A

The bar magnet wasn’t dropped centrally.
or
The magent accelerates as it falls, making speed grater with distance covered so that time is less.

19
Q

Why wouldn’t the magnet normally fall at 9.8ms^-1?

A

As induced emf and therefore current in the coil produce a magnetic field of its own, after emf has been induced by the change in magnetic flux/ magnetic flux linkage. This magnetic field will act in a way to repel the action of the magent pushing it out of the coil initially and later trying to keep it in, according to Lenz Law. These produce an upward force stopping magnet from falling at 9.8ms^-1.

20
Q

What would happen to the emf time graph if the number of coils was increased?

A

emf would have double at each stage as magnetic flux/magnetic flux linkage is greater.

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