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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 .

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