In terms ofXwe can writex(t)as:
x(t)=Im(Xejωt)
wherein lies the usefulness of phasors – the frequency behaviour of x(t) is sepa-
rated out.
Phasors representing sinusoids of the same frequency can be added and subtracted
by complex algebra. Thus, if the phasorsX 1 =A 1 ejφ^1 ,X 2 =A 2 ejφ^2 represent signals
x 1 (t)=A 1 sin(ωt+φ 1 ),x 2 (t)=A 2 sin(ωt+φ 2 )respectively then the phasorX 1 +X 2
represents the signalx 1 (t)+x 2 (t)and the phasorX 1 −X 2 represents the signalx 1 (t)−
x 2 (t).
- Sketch and write down the phasors corresponding to the sinusoids 2 sin(ωt+π/ 4 ),
sin(ωt+ 4 π/ 3 ),3cos(ωt+π/ 3 ),4sin(ωt−π/ 6 )– write these in Cartesian forma+
jb. - Sketch and write down the phasors corresponding to the sinusoids:
(i) 3 sin(ωt+π/ 6 ) (ii) 2 sin(ωt+π/ 2 )
(iii) sin(ωt−π/ 4 ) (iv) 3 cos(ωt−π/3)
Express the phasors ina+jbform.
Answers:
(i) 3ejπ/^6 ,
3
√
3
2
+j
3
2
(ii) 2ejπ/^2 ,2j
(iii) e−jπ/^4 ,
1
√
2
−j
1
√
2
(iv) 3ejπ/^6 ,
3
√
3
2
+j
3
2
- Find the sinusoidal functions (assume frequencyω) corresponding to the following
phasors ina+jbform
(i) 3+ 3 j (ii) − 4 + 2
√
3 j (iii) − 4 − 3 j (iv) 3− 5. 2 j
Answers:
(i) 3
√
2sin(ωt+π/ 4 ) (ii) 2
√
7sin(ωt+ 2. 43 )
(iii) 5 sin(ωt+ 3. 79 ) (iv) 6 sin(ωt− 1. 05 )
NB. All angles in radians.
- Express 2 cosωtand
√
2cos(ωt+π/ 4 )in phasor form and hence determine the ampli-
tude and phase of
2cosωt+
√
2cos(ωt+π/ 4 )