DC Circuits
- Electromotive force is the energy converted into electrical energy when 1 C of charge passes through the power source
P.D. and E.M.F.
Internal Resistance
- Internal resistance is the resistance to current flow within the power source; it reduced p.d. when delivering current
- V = Ir – E
- Voltage across the resistor: V = IR
- Voltage lost to internal resistance: V = Ir
- Thus e.m.f.: E = IR + Ir
- E = I(R + r)
Kirchhoff’s First Law
- Sum of currents into a junction is equal to the sum of currents out of the junction
- Kirchhoff’s first law is another statement of the law of conservation of charge
Kirchhoff’s Second Law
- Sum of e.m.fs in a closed circuit is equal to the sum of the potential differences
- Kirchhoff’s second law is another statement of the law of conservation of energy
Applying Kirchhoff’s Laws
- Calculate the current in each of the resistors
- Using Kirchhoff’s first law:
- I3 = I1 + I2
- Using Kirchhoff’s second law on loop ABEF:
- 3 = 30I3 + 10I1
- Using Kirchhoff’s second law on loop CBED:
- 2 = 30I3
- Using Kirchhoff’s second on loop ACDF:
- 3 – 2 = 10I1
- Solve the simultaneous equations:
- I1 = 0.1
- I2 = -0.033
- I3 = 0.067
- Using Kirchhoff’s first law:
Deriving Effective Resistance in Series
- From Kirchhoff’s second law:
- E = ∑IR
- IR = IR1 + IR2
- Current is constant, therefore:
- R = R1 + R2
Deriving Effective Resistance in Parallel
- From Kirchhoff’s first law:
- I = ∑I
- I = I1 + I2
- V/R = V/R1 + V/R2
- Voltage is constant, therefore;
- 1/R = 1/R1 + 1/R2
Properties of Magnets
- A potential divider divides the voltage into smaller parts
- Vout/Vin = R2/RTotal
- Usage of a thermistor at R1:
- Resistance decreases with increasing temperature
- It can be used in potential divider circuits to monitor and control temperatures
- Usage of an LDR at R1:
- Resistance decreases with increasing light intensity
- It can be used in potential divider circuits to monitor light intensity
Potentiometers
- A potentiometer is a continuously variable potential divider used to compare potential differences
- Potential difference along the wire is proportional to the length of the wire
- It can be used to determine the unknown e.m.f. of a cell
- This can be done by moving the sliding contact along the wire until it finds the null point that the galvanometer shows a zero reading; the potentiometer is balanced
- For example:
- E1 is 10 V, distance XY is equal to 1 m. The potentiometer is balanced at point T which is 0.4 m from X. Calculate E2
-
- E1/E2 = L1/L2
- 10/E2 = 1/0.4
- E2 = 4 V
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- E1 is 10 V, distance XY is equal to 1 m. The potentiometer is balanced at point T which is 0.4 m from X. Calculate E2