Please help to solve 11-20 Step by step

Mathematics
Please help to solve 11-20 Step by step

ScanSolve AI Answer

Here are the solutions for questions 11-20.

Question 11: Step 1: Identify the given values and the formula for motional EMF. The speed of the train is v=10 m/sv = 10 \text{ m/s}. The magnetic flux density is B=10 μT=10×10−6 TB = 10 \text{ μT} = 10 \times 10^{-6} \text{ T}. The length of the axle is L=1.0 mL = 1.0 \text{ m}. The magnetic field is perpendicular to the velocity and the axle, so sin⁡θ=1\sin\theta = 1. The formula for motional EMF is E=BLvsin⁡θ\mathcal{E} = B L v \sin\theta.

Step 2: Substitute the values into the formula and calculate the EMF. E=(10×10−6 T)×(1.0 m)×(10 m/s)×1\mathcal{E} = (10 \times 10^{-6} \text{ T}) \times (1.0 \text{ m}) \times (10 \text{ m/s}) \times 1 E=100×10−6 V\mathcal{E} = 100 \times 10^{-6} \text{ V} E=1.0×10−4 V\mathcal{E} = 1.0 \times 10^{-4} \text{ V} The induced emf is *1.0×10−4 V*\boxed{\text{*}1.0 \times 10^{-4} \text{ V*}}.

Question 12: Step 1: Identify the given values and the formula for induced EMF by Faraday's Law. Number of turns N=5N = 5. Initial magnetic flux Φ1=1.0 mWb=1.0×10−3 Wb\Phi_1 = 1.0 \text{ mWb} = 1.0 \times 10^{-3} \text{ Wb}. Final magnetic flux Φ2=2.0 mWb=2.0×10−3 Wb\Phi_2 = 2.0 \text{ mWb} = 2.0 \times 10^{-3} \text{ Wb}. Time interval Δt=1.0 s\Delta t = 1.0 \text{ s}. The magnitude of the induced EMF is given by ∣E∣=N∣ΔΦ∣∣Δt∣|\mathcal{E}| = N \frac{|\Delta\Phi|}{|\Delta t|}.

Step 2: Calculate the change in magnetic flux. ΔΦ=Φ2−Φ1=(2.0×10−3 Wb)−(1.0×10−3 Wb)=1.0×10−3 Wb\Delta\Phi = \Phi_2 - \Phi_1 = (2.0 \times 10^{-3} \text{ Wb}) - (1.0 \times 10^{-3} \text{ Wb}) = 1.0 \times 10^{-3} \text{ Wb}

Step 3: Substitute the values into the EMF formula and calculate. ∣E∣=5×1.0×10−3 Wb1.0 s|\mathcal{E}| = 5 \times \frac{1.0 \times 10^{-3} \text{ Wb}}{1.0 \text{ s}} ∣E∣=5.0×10−3 V|\mathcal{E}| = 5.0 \times 10^{-3} \text{ V} The magnitude of the induced emf is *5.0×10−3 V*\boxed{\text{*}5.0 \times 10^{-3} \text{ V*}}.

Question 13: Step 1: Identify the given values and the formula for motional EMF. Wing span L=10 mL = 10 \text{ m}. Speed of the aircraft v=100 m/sv = 100 \text{ m/s}. Vertical component of Earth's magnetic field B=10 μT=10×10−6 TB = 10 \text{ μT} = 10 \times 10^{-6} \text{ T}. The wing span is perpendicular to both the velocity and the vertical magnetic field, so sin⁡θ=1\sin\theta = 1. The formula for motional EMF is E=BLvsin⁡θ\mathcal{E} = B L v \sin\theta.

Step 2: Substitute the values into the formula and calculate the EMF. E=(10×10−6 T)×(10 m)×(100 m/s)×1\mathcal{E} = (10 \times 10^{-6} \text{ T}) \times (10 \text{ m}) \times (100 \text{ m/s}) \times 1 E=10000×10−6 V\mathcal{E} = 10000 \times 10^{-6} \text{ V} E=1.0×10−2 V\mathcal{E} = 1.0 \times 10^{-2} \text{ V} The induced emf is *1.0×10−2 V*\boxed{\text{*}1.0 \times 10^{-2} \text{ V*}}.

Question 14: Step 1: Identify the given values and the formula for induced EMF by Faraday's Law. Number of turns N=100N = 100. Initial magnetic flux Φ1=2 mWb=2×10−3 Wb\Phi_1 = 2 \text{ mWb} = 2 \times 10^{-3} \text{ Wb}. Final magnetic flux Φ2=0 Wb\Phi_2 = 0 \text{ Wb}. Time interval Δt=1.0 s\Delta t = 1.0 \text{ s}. The magnitude of the average induced EMF is given by ∣E∣=N∣ΔΦ∣∣Δt∣|\mathcal{E}| = N \frac{|\Delta\Phi|}{|\Delta t|}.

Step 2: Calculate the change in magnetic flux. ΔΦ=Φ2−Φ1=0 Wb−(2×10−3 Wb)=−2×10−3 Wb\Delta\Phi = \Phi_2 - \Phi_1 = 0 \text{ Wb} - (2 \times 10^{-3} \text{ Wb}) = -2 \times 10^{-3} \text{ Wb}

Step 3: Substitute the values into the EMF formula and calculate. ∣E∣=100×∣−2×10−3 Wb∣1.0 s|\mathcal{E}| = 100 \times \frac{|-2 \times 10^{-3} \text{ Wb}|}{1.0 \text{ s}} ∣E∣=100×(2×10−3 V)|\mathcal{E}| = 100 \times (2 \times 10^{-3} \text{ V}) ∣E∣=0.2 V|\mathcal{E}| = 0.2 \text{ V} The average induced emf is *0.2 V*\boxed{\text{*}0.2 \text{ V*}}.

Question 15: Step 1: Compare the given equation with the general form of alternating EMF. The given equation for emf is E=20sin⁡(100πt)\mathcal{E} = 20 \sin (100 \pi t). The general form for alternating emf is E=E0sin⁡(ωt)\mathcal{E} = \mathcal{E}_0 \sin(\omega t), where E0\mathcal{E}_0 is the peak emf and ω\omega is the angular frequency.

Step 2: Identify the peak value from the equation. By comparing the two equations, the peak value E0\mathcal{E}_0 is the coefficient of the sine function. E0=20 V\mathcal{E}_0 = 20 \text{ V} The peak value E0\mathcal{E}_0 is *20 V*\boxed{\text{*}20 \text{ V*}}.

Question 16: Step 1: Identify the given RMS voltage and the relationship between RMS and peak voltage. The RMS voltage of the main supply is Vrms=230 VV_{rms} = 230 \text{ V}. The relationship between RMS voltage (VrmsV_{rms}) and peak voltage (VpeakV_{peak}) for an AC supply is Vrms=Vpeak2V_{rms} = \frac{V_{peak}}{\sqrt{2}}.

Step 2: Rearrange the formula to solve for peak voltage and substitute the value. Vpeak=Vrms×2V_{peak} = V_{rms} \times \sqrt{2} Vpeak=230 V×2V_{peak} = 230 \text{ V} \times \sqrt{2} Vpeak≈230 V×1.414V_{peak} \approx 230 \text{ V} \times 1.414 Vpeak≈325.22 VV_{peak} \approx 325.22 \text{ V} The peak voltage is *325 V*\boxed{\text{*}325 \text{ V*}}.

Question 17: Step 1: Identify the given current equation and resistance, and the formulas for mean power. The alternating current is I=3sin⁡(50t)I = 3 \sin (50t). From this, the peak current is Ipeak=3 AI_{peak} = 3 \text{ A}. The resistive load is R=10 ΩR = 10 \text{ Ω}. The mean power dissipated in a resistive load is Pmean=Irms2RP_{mean} = I_{rms}^2 R.

Step 2: Calculate the RMS current from the peak current. The relationship between RMS current (IrmsI_{rms}) and peak current (IpeakI_{peak}) is Irms=Ipeak2I_{rms} = \frac{I_{peak}}{\sqrt{2}}. Irms=3 A2I_{rms} = \frac{3 \text{ A}}{\sqrt{2}}

Step 3: Substitute the RMS current and resistance into the mean power formula. Pmean=(32)2×10 ΩP_{mean} = \left(\frac{3}{\sqrt{2}}\right)^2 \times 10 \text{ Ω} Pmean=92×10 WP_{mean} = \frac{9}{2} \times 10 \text{ W} Pmean=4.5×10 WP_{mean} = 4.5 \times 10 \text{ W} Pmean=45 WP_{mean} = 45 \text{ W} The mean power dissipated is *45 W*\boxed{\text{*}45 \text{ W*}}.

Question 18: Step 1: Identify the given power and RMS voltage, and the formulas for power and peak current. Power of the heater P=4.0 kW=4000 WP = 4.0 \text{ kW} = 4000 \text{ W}. RMS voltage of the supply Vrms=240 VV_{rms} = 240 \text{ V}. The power in an AC circuit is P=VrmsIrmsP = V_{rms} I_{rms}. The relationship between RMS current and peak current is Ipeak=Irms2I_{peak} = I_{rms} \sqrt{2}.

Step 2: Calculate the RMS current. Irms=PVrmsI_{rms} = \frac{P}{V_{rms}} Irms=4000 W240 VI_{rms} = \frac{4000 \text{ W}}{240 \text{ V}} Irms=40024 A=503 A≈16.67 AI_{rms} = \frac{400}{24} \text{ A} = \frac{50}{3} \text{ A} \approx 16.67 \text{ A}

Step 3: Calculate the peak current. Ipeak=Irms2I_{peak} = I_{rms} \sqrt{2} Ipeak=503 A×2I_{peak} = \frac{50}{3} \text{ A} \times \sqrt{2} Ipeak≈16.67 A×1.414I_{peak} \approx 16.67 \text{ A} \times 1.414 Ipeak≈23.57 AI_{peak} \approx 23.57 \text{ A} The peak current drawn is *23.6 A*\boxed{\text{*}23.6 \text{ A*}}.

Question 19: Step 1: Identify the given voltages and secondary turns, and the transformer turns ratio formula. Primary voltage Vp=220 VV_p = 220 \text{ V}. Secondary voltage Vs=7.5 VV_s = 7.5 \text{ V}. Number of turns on the secondary coil Ns=140N_s = 140 turns. For an ideal transformer, the ratio of voltages is equal to the ratio of turns: VpVs=NpNs\frac{V_p}{V_s} = \frac{N_p}{N_s}.

Step 2: Rearrange the formula to solve for the number of turns on the primary coil (NpN_p) and substitute the values. Np=Ns×VpVsN_p = N_s \times \frac{V_p}{V_s} Np=140 turns×220 V7.5 VN_p = 140 \text{ turns} \times \frac{220 \text{ V}}{7.5 \text{ V}} Np=140×29.333...N_p = 140 \times 29.333... Np≈4106.67N_p \approx 4106.67 Since the number of turns must be an integer, we round to the nearest whole number. The number of turns on the primary coil is *4107 turns*\boxed{\text{*}4107 \text{ turns*}}.

Question 20: Step 1: Identify the given voltages and secondary current, and the power conservation formula for an ideal transformer. Primary voltage Vp=240 VV_p = 240 \text{ V}. Secondary voltage Vs=15 VV_s = 15 \text{ V}. Secondary current Is=2.0 AI_s = 2.0 \text{ A}. For an ideal transformer, the power in the primary coil equals the power in the secondary coil: Pp=PsP_p = P_s. This can be written as VpIp=VsIsV_p I_p = V_s I_s.

Step 2: Rearrange the formula to solve for the primary current (IpI_p) and substitute the values. Ip=VsIsVpI_p = \frac{V_s I_s}{V_p} Ip=(15 V)×(2.0 A)240 VI_p = \frac{(15 \text{ V}) \times (2.0 \text{ A})}{240 \text{ V}} Ip=30 W240 VI_p = \frac{30 \text{ W}}{240 \text{ V}} Ip=18 AI_p = \frac{1}{8} \text{ A} Ip=0.125 AI_p = 0.125 \text{ A} The current drawn from the primary coil is *0.125 A*\boxed{\text{*}0.125 \text{ A*}}.

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