f(t)=sinωt ,
For full wave-
L[sinωt]=1−e−ω2πi1∫02πe−stsinωtdt
=1−e−ω2πi1(s2+ω2e−st[−ssinωt−ωcosωt])0ωπ
=1−e−ω2πi1(s2+ω2e−ωsπω+ω)
=(1−e−ωπi)(s2+ω2)ω
For half wave-
L[sinωt]=1−e−ω2πi1∫0πe−stsinωtdt
=1−e−ω2πi1(s2+ω2e−st[−ssinωt−ωcosωt])02ωπ
=1−e−ωπi1(s2+ω2e−2ωsπω+ω)
=(1−e−ωπi)(s2+ω2)2ω
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