In a series L.C.R. circuit, the potential drop across `L`, `C` and `R` respectively are `40V`, `120V` and `60V` . Them the source voltage is

In a series LCR circuit , the potential drop across L, C and R respectively are 40 V , 120V and 60V . Then the source voltage is

In an LCR series circuit the voltages across R,L and C at resonance are 40 V and 60V respectively the applied voltage is .

In a series RLC circuit, potential differences across R, L and C are 30 V, 60 V and 100 V respectively as shown in figure. The e.m.f. of source (in volts) is

In an LCR series circuit, the rms voltages across R, L and C are found to be 10 V, 10 V and 20 V respectively. The rms voltage across the entire combination is

In an LCR series ac circuit the voltage across L,C and R are V_(1), V_(2) and V_(3) respectively The voltage of the source is .

In an LCR series ac circuit the voltage across L,C and R are V_(1), V_(2) and V_(3) respectively The voltage of the source is .

Statement 1: In a series RLC circuit if (V_R), (V_L) and (V_C) denote rms voltage across R,L and C respectively and (V_S) is the rms voltage across the source. Then (V_s)=(V_R)+(V_L)+(V_C) Statement 2: In ac circuit, Kirchhoff's voltage law is correct at every instant of same.

Statement 1: In a series RLC circuit if (V_R), (V_L) and (V_C) denote rms voltage across R,L and C respectively and (V_S) is the rms voltage across the source. Then (V_s)=(V_R)+(V_L)+(V_C) Statement 2: In ac circuit, Kirchhoff's voltage law is correct at every instant of same.