fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
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AC CIRCUITS<br />
For a sinusoidal voltage or current <strong>of</strong> frequency f (Hz) and<br />
period T (seconds),<br />
f = 1/T = ω/(2π), where<br />
ω = the angular frequency in radians/s.<br />
Average Value<br />
For a periodic waveform (either voltage or current) with<br />
period T,<br />
X ave = 1<br />
T<br />
( T ) x(<br />
t)<br />
∫<br />
0<br />
dt<br />
The average value <strong>of</strong> a full-wave rectified sinusoid is<br />
Xave = (2Xmax)/π<br />
and half this for half-wave rectification, where<br />
Xmax = the peak amplitude <strong>of</strong> the waveform.<br />
Effective or RMS Values<br />
For a periodic waveform with period T, the rms or effective<br />
value is<br />
12<br />
⎡ T<br />
2 ⎤<br />
Xeff = Xrms = ⎢( 1 T) ∫ x ( t) dt⎥<br />
⎣ 0 ⎦<br />
For a sinusoidal waveform and full-wave rectified sine<br />
wave,<br />
X = X = X 2<br />
eff<br />
rms max<br />
For a half-wave rectified sine wave,<br />
Xeff = Xrms = Xmax/2<br />
For a periodic signal,<br />
∞<br />
2 2<br />
rms dc n<br />
n= 1<br />
X = X + ∑ X where<br />
Xdc is the dc component <strong>of</strong> x(t)<br />
Xn is the rms value <strong>of</strong> the n th harmonic<br />
Sine-Cosine Relations<br />
cos (ωt) = sin (ωt + π/2) = – sin (ωt – π/2)<br />
sin (ωt) = cos (ωt – π/2) = – cos (ωt + π/2)<br />
Phasor Transforms <strong>of</strong> Sinusoids<br />
Ρ [Vmax cos (ωt + φ)] = Vrms ∠ φ = V<br />
Ρ [Imax cos (ωt + θ)] = Irms ∠ θ = I<br />
For a circuit element, the impedance is defined as the ratio<br />
<strong>of</strong> phasor voltage to phasor current.<br />
Z = V I<br />
For a Resistor, ZR = R<br />
1<br />
For a Capacitor, ZC = = jXC<br />
jωC 169<br />
ELECTRICAL AND COMPUTER ENGINEERING (continued)<br />
For an Inductor,<br />
ZL = jωL = jXL, where<br />
XC and XL are the capacitive and inductive reactances<br />
respectively defined as<br />
1<br />
X C = − and X L = ωL<br />
ωC<br />
Impedances in series combine additively while those in<br />
parallel combine according to the reciprocal rule just as in<br />
the case <strong>of</strong> resistors.<br />
ALGEBRA OF COMPLEX NUMBERS<br />
Complex numbers may be designated in rectangular form or<br />
polar form. In rectangular form, a complex number is<br />
written in terms <strong>of</strong> its real and imaginary components.<br />
z = a + jb, where<br />
a = the real component,<br />
b = the imaginary component, and<br />
j = − 1<br />
In polar form<br />
z = c ∠ θ, where<br />
c =<br />
2<br />
2<br />
a + b ,<br />
θ = tan –1 (b/a),<br />
a = c cos θ, and<br />
b = c sin θ.<br />
Complex numbers are added and subtracted in rectangular<br />
form. If<br />
z1 = a1 + jb1 = c1 (cos θ1 + jsin θ1)<br />
= c1 ∠ θ1 and<br />
z2 = a2 + jb2 = c2 (cos θ2 + jsin θ2)<br />
= c2 ∠ θ2, then<br />
z1 + z2 = (a1 + a2) + j (b1 + b2) and<br />
z1 – z2 = (a1 – a2) + j (b1 – b2)<br />
While complex numbers can be multiplied or divided in<br />
rectangular form, it is more convenient to perform these<br />
operations in polar form.<br />
z1 × z2 = (c1 × c2) ∠ θ1 + θ2<br />
= (c1 /c2) ∠ θ1 – θ2<br />
z1/z2<br />
The complex conjugate <strong>of</strong> a complex number z1 = (a1 + jb1)<br />
is defined as z1* = (a1 – jb1). The product <strong>of</strong> a complex<br />
number and its complex conjugate is z1z1* = a1 2 + b1 2 .