Provided below are notes and various common formula used in designing electrical circuits.
Direction of currents
The terminology when representing the direction of the positive current flow is as follows
Electron drift which is the flow of electrons in an electrical circuit flows from negative to positive .
Electric batteries by convention are identified as shown in the figure below..
A simple dc circuit illustrates the various relationships and directions is shown below..
V = Voltage (Volts)
I = Current (Amperes)
R = Resistance (Ohms)
W = Power (Watts)
V = I.R = Sqrt (W . R) = W / I
I = V / R = Sqrt( W / R) = W / V
R = V / I = W / I2 = V2 / W
W = VI = V2 / R = I2 . R
General Form of Ohms law
R = ρ . L / A
L = Length (metres), A = Area (metre2 ), ρ = resistivity (Ω /metre)
Resistors in Series
R_total = R 1 + R 2 + R 3...
Voltage across Resistors in Series
V total = V R1 + V R2 + V R3..
Resistors in Parallel
R total = 1/ (1/R 1 + 1/R 2 +1/R 3...)
The Voltage across Resistors in Parallel is the Same = V
Alternating Current Supplies
v = V max. sin ω. t = V max .sin(2.π.f.t)
v = instantaneous voltage
V_max = maximum voltage,
t = time (seconds) from from point of zero rising voltage in sinusoidal variation., ω = angular velocity rads/sec, f = frequency (cycles /sec)
The average value of a sinusoidal alternating quantity is calculated at 0.637x maximum value
The Root Mean Square(RMS) value of a sinusoidal alternating quantity is calculated at 0.707 x maximum value.
The form factor of a wave is the RMS value / average Value = (for a sinusoidal wave) 1.1
The peak (crest) factor is the peak value / RMS value = 1.414
Kirchoffs First law.
The total current flowing towards a junction is equal to the total current flowing
away from that junction. i.e the algebraic sum of the currents flowing towards a junction is zero
Kirchoff's Second Law
In a closed circuit the algebraic sum of the products of the current and the
resistance of each part of the circuit is equal to the resultant e.m.f in the
As an example of Kirchoff's second law it is required to find the currents in each branch
in the circuit shown below
First it can be seen that I 3 = I 1 + I 2.......a)
In AFEB 2V - 3V = (I 1. 1 Ω) - I 2.2Ω)
Therefore .... -1 A = I 1 - 2.I 2.......(b)
IN BEDC 3V = (I 2.2 Ω) + (I 3.3 Ω )
Therefore.... 3A = 2.I 2 + 3 .I 3 ...... (c)
Substituting for I 3 in c) .. 2.I 2 + 3.I 1 + 3.I 2 = 3A Therefore 3.I 1 + 5.I 2 = 3A .....d)
- 3 times b).... -3.I 1 + 6.I 2 = 3A..
and adding the last two equations 11.I 2 = 6A. and therefore I 2 = (6/11) A....
(I 1 = 2.I 2 - 1) ...
so I 1 =(1/11) A
and I 3 = I 1 +I 1
so I 3 = (7/11) A
This theorem states that in any network containing more than one source , the current in, or the p.d across, any branch can be found
by considering each source separately and adding their effects: The omitted sources (of e.m.f) being
replaced by resistances equivalent to their internal resistances.
This theorem states that if a current is produced at point a in a network by a source
acting at point b then the the same current would be produced at b by the same value source
acting at point a
This theorem is used to determine the voltage / current flow across / through two
points say A and B in a complicated circuit which includes and number of sources
and loads. The theorem states
The current through a resistance R connected across any two points A and B of an active
network ( a network containing one or more sources of e.m.f. ) is obtained by dividing
the p.d. between A and B with R disconnected , by ( R + r ) where r is the resistance
of the network measure between A and B with R disconnected and the sources of e.m.f
replaced by their internal resistance.
Consider a general network containing voltage and current sources.
The network can be replaced by a single source of e.m.f (E) with and internal
E being the e.m.f. across A- B with the load disconnected and r
being the total resistance of the circuit measured across A-B with the
load disconnected and the e.m.f. sources replaced by their internal resistances.
As an example of this theorem it is necessary to find the p.d across A-B in the figure below.
First remove the resistance R and calculate V. As there is no current flow there
is no p.d. across R 2
The current through R 3 is E 1 / (R 1 + R 3)..
The p.d. across R 3 = ....V = is E 1. R 3 / ( R 1 + R 3)
The resistance of the network = r = R 2 + (R 1 .R 3) / (R 1 + R 3)
Thevenin's theorem states that the circuit above can be replaced by the simple circuit as shown below
The current flow I = V / (r +R)..The pd. across R = V.R/ (r+R)
Start Delta Conversions
The star delta conversion formula are useful if loads are connected in a star or
delta arrangement and it is more convenient to convert to the other arrangement
which may be more simpler to resolve for a particular problem....
The relationships are properties of the load impedances and are independent of the voltages and does not imply
three phase working....
Q = V . C therefore I = C dV/dt
Q = Charge (Coulomb)
V = Potential Difference (Volts)
C = Capacitance (Farad)
V = V / X c
X c = Capacitive Reactance (Ω )
X c = 1 / (2 π f C )
f = frequency (Herz)
Addition of Capacitors
Capacitors in Parallel
C total. V = Q total = Q 1+Q 2+Q 3...
C total. V = V.C 1+V.C 2+V.C 3...
C total = C 1+C 2+C 3...
Capacitors in Series
1/C total = 1/C 1 + 1/C 2 + 1/C 3...
C total = 1/ (1/C 1 + 1/C 2 + 1/C 3...)
V = L.dI/dt
L = Inductance (Henry)
I = V/ X L
X L = Inductive Reactance (Ω )
X L =2 π f L
f = frequency (Herz)
Inductances in Series
L total = L 1 + L 2 + L 3...
Inductances in Parallel
1 / L total = 1 / L 1 + 1 / L 2 + 1 / L 3 ...
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