Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb...

11
Definition of Potential Definition of Potential Difference Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving 2 C of charge across a p.d. of 10 V. W = ? V = 10 V Q = 2C W = Q x V W = 2 x 10 = 20 J

Transcript of Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb...

Page 1: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Definition of Potential DifferenceDefinition of Potential Difference

p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge.

Example

Calculate the work done in moving 2 C of charge across a p.d. of 10 V.

W = ? V = 10 V Q = 2C

W = Q x V

W = 2 x 10 = 20 J

Page 2: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance Internal Resistance

Terminal potential difference ( Vt.p.d. ) is the p.d. across the load

Vtpd

Page 3: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance 2Internal Resistance 2

Resistance of power supply itselfResistance of power supply itself Work is done to push charges through Work is done to push charges through

power supply hence ‘Lost Volts’ power supply hence ‘Lost Volts’ Electromotive Force (E.M.F. ) Maximum Electromotive Force (E.M.F. ) Maximum energy to push unit charge around circuitenergy to push unit charge around circuit

Terminal potential difference , work to push Terminal potential difference , work to push unit charge through external circuit ( load )unit charge through external circuit ( load )

Page 4: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance 3Internal Resistance 3

Apply the principle of conservation of energy

Electromotive force = terminal p.d. + lost volts

E.M.F ( E ) = Vtpd + Vlost

But Vlost = I x r I = current flowing and

r = internal resistance

Therefore E = Vtpd + Ir

Page 5: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance 4Internal Resistance 4

E = V E = V t.p.dt.p.d. + V . + V lostlost

V V t.p.d.t.p.d. = E - V = E - V lost lost VV t.p.d t.p.d = E – (I x r)= E – (I x r)

V t.p.d

I

E.M.F

open circuit p.d. NO lost volts

- slope = r

Short circuit current E = V lost

0

VV t.p.d t.p.d = -r x I + E

y = mx + c

Page 6: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance 5Internal Resistance 5

EMF is measured by connecting a voltmeter across the battery when there is NO load. No load means NO current and hence NO lost volts.

Short Circuit Current is the maximum current the battery can deliver. From the graph, Vtpd = 0V when current is maximum. Hence E = Vlost.

This is a theoretical value.

Page 7: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

ExampleA cell of e.m.f. 1.5V and internal resistance 0.75 Ω is connected as shown in the following circuit.

(a) Calculate the value of the reading on the voltmeter.

(b) What is the value of the “lost volts” in this circuit?

(a) Ve.m.f. = I(R+r)

1.5 = I (3 + 0.75)

I = 1.5/3.75 = 0.4 A

Vt.p.d. = IR = 0.4 x 3 = 1.2 V

(b)Lost volts = Ir = 0.4 x 0.75 = 0.3 V

OR Lost volts = Ve.m.f - Vt.p.d. = 1.5 – 1.2 =

0.3 V

1.5V

3 Ω

V

0.75 Ω

Or use voltage divider equation

Total resistance

Page 8: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance 7Internal Resistance 7

Example

Calculate :

a)The short circuit current of the cell and

b) The quantity of heat energy dissipated in the battery when connected as shown.

E = 6.0 V r= 1.0 Ω

4.0 Ω

a)

a) When short circuit current flows Vtpd = 0V

Therefore E = Vl = I r

I = E / r = 6.0 / 1.0 = 6.0 A

Page 9: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Internal Resistance 7aInternal Resistance 7a

b) Energy per second ( power ) can be calculated by various ways :

P = I2 r

P = 1.22 x 1.0

P = 1.44 A

I = E / Rtotal

I = E / ( R = r )

I = 6.0 / ( 4.0+1.0 )

I = 1.2 AThis is one more significant figure than data. We are allowed to quote ‘2’extra sig figs

Page 10: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Power SuppliesThe ideal voltage source maintains a constant output voltage no matter what load is connected to it . This ideal source would have ZERO internal resistance.

In the real world power supplies have internal resistance and as soon as a load is connected then the terminal potential difference decreases. It is important to carefully match the internal resistance of the power supply with the resistance of the load:

R = 5Ω

Internal resistance, r, Load, R.

If r > R then the ‘lost volts ‘ will be bigger than the terminal potential difference and lots of heat is generated inside supply

Page 11: Definition of Potential Difference p.d. of 1 Volt when 1 joule of work is required to move 1 coulomb of charge. Example Calculate the work done in moving.

Amplifiers need to be matched carefully to loudspeakers of certain impedance if max power is to be transferred to the speakers. The internal resistance of the amplifier should equal that of the speakers for max power transfer.