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forsale [732]
3 years ago
12

LC CIRCUIT: A 20.00-F capacitor is fully charged by a 100.00-V battery, then disconnected from the battery and connected in seri

es with a 0.280-mH inductor at t=0. Thus, the initial current 1-0. See circuit below after the charged capacitor is connected to the inductor. (a) What is the angular oscillation frequency o of the circuns (b) What is the maximum charge on the positive capacitor plate? (c) What is the energy stored in the capacitor at t - 0? (d) Using conservation of energy, find the current I when the charge reaches one-third the maximum charge. (e) Using conservation of energy, find the maximum current Imax 000000
Physics
1 answer:
klio [65]3 years ago
3 0

Answer:

(a) w=13.363\ rad/sec

(b) Q_m=2000\ coul

(c) E_{max}=100,000\ J

(d) I=25,197.63\ A

(e) I_{max}=26,726.12\ A

Explanation:

<u>LC Circuit</u>

The dynamics of an LC circuit is explained as the energy stored in the capacitor C in the form of an electrical field is transferred to the inductor L as a magnetic field. The energy stored in a capacitor is

\displaystyle E_c=\frac{CV^2}{2}

Where V is the potential between its plates where a charge Q is stored. The relation between them is

\displaystyle C=\frac{Q}{V}

The energy stored in an inductor of self-inductance L is

\displaystyle E_c=\frac{LI^2}{2}

Where I is the current flowing through the inductor. If we apply the principle of conservation of energy, the loss of electric energy in the capacitor will transform into magnetic energy in the inductor and vice-versa.

The angular frequency of oscillation of a LC circuit is

\displaystyle w=\sqrt{\frac{1}{LC}}

The question provides the following data

V_m=100\ V,\ C=20\ F,\ L=0.28\ mH=0.00028\ H

(a) The angular frequency is

\displaystyle w=\sqrt{\frac{1}{(0.00028)(20)}}

w=13.363\ rad/sec

(b) When the voltage is at maximum, the charge will also be maximum, its value can be computed solving for Q

\displaystyle C=\frac{Q_m}{V_m}

Q_m=V_mC=100(20)=2000

Q_m=2000\ coul

(c) At t=0, the voltage is at maximum, so the energy stored is

\displaystyle E_{max}=\frac{CV_m^2}{2}

\displaystyle E_{max}=\frac{20\ 100^2}{2}=100,000

E_{max}=100,000\ J

(d) If the charge reaches 1/3 of the initial value, it means 2/3 of the charge were transformed in magnetic energy. Let's call E_t to the transferred electric energy to magnetic energy, and E_1 to the remaining electric energy in the capacitor. Knowing Q_1=1/3Q_m

\displaystyle Q_1=\frac{2000}{3}=666.67\ coul

\displaystyle V_1=\frac{666.67}{20}=33.33\ V

\displaystyle E_1=\frac{(20)\ 33.33^2}{2}=11,111.11\ J

The energy transfered is

E_t=100,000-11,111.11=88,888.89\ J

We can compute the current solving for I in:

\displaystyle E_t=\frac{LI^2}{2}

\displaystyle I=\sqrt{\frac{2E_t}{L}}

Calculating I

\displaystyle I=\sqrt{\frac{2(88,888.89)}{0.00028}}

I=25,197.63\ A

(e) To find I_{max}, we'll assume all the electric energy is transformed to magnetic, so

\displaystyle I_{max}=\sqrt{\frac{2E_{max}}{L}}

\displaystyle I_{max}=\sqrt{\frac{2(100,000)}{0.00028}}

I_{max}=26,726.12\ A

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The circuit you should use to find the open-circuit voltage is
fiasKO [112]

Answer:

Incomplete questions check attachment for circuit diagram.

Explanation:

We are going to use superposition

So, we will first open circuit the current source and find the voltage Voc.

So, check attachment for open circuit diagram.

From the diagram

We notice that R3 is in series with R4, so its equivalent is given below

Req(3-4) = R3 + R4

R(34) = 20+40 = 60 kΩ

Notice that R2 is parallel to the equivalent of R3 and R4, then, the equivalent of all this three resistor is

Req(2-3-4) = R2•R(34)/(R2+R(34))

R(234) = (100×60)/(100+60)

R(234) = 37.5 kΩ

We notice that R1 and R(234) are in series, then, we can apply voltage divider rule to find voltage in R(234)

Therefore

V(234) = R(234) / [R1 + R(234)] × V

V(234) = 37.5/(25+37.5) × 100

V(234) = 37.5/62.5 × 100

V(234) = 60V.

Note, this is the voltage in resistor R2, R3 and R4.

Note that, R2 is parallel to R3 and R4. Parallel resistor have the same voltage, then voltage across R2 equals voltage across R34

V(34) = 60V.

Now, we also know that R3 and R4 are in series,

So we can know the voltage across R4 which is the Voc we are looking for.

Using voltage divider

V4 = Voc = R4/(R4 + R(34)) × V(34)

Voc = 40/(40+60) × 60

Voc = 24V

This is the open circuit Voltage

Now, finding the short circuit voltage when we short circuit the voltage source

Check attachment for circuit diagram.

From the circuit we notice that R1 and R2 are in parallel, so it's equivalent becomes

Req(1-2) = R1•R2/(R1+R2)

R(12) = 25×100/(25+100)

R(12) = 20 kΩ

We also notice that the equivalent of Resistor R1 and R2 is in series to R3. Then, the equivalent resistance of the three resistor is

Req(1-2-3) = R(12) + R(3)

R(123) = 20 + 20

R(123) = 40 kΩ

We notice that, the equivalent resistance of the resistor R1, R2, and R3 is in series to resistor R4.

So using current divider rule to find the current in resistor R4.

I(4) = R(123) / [R4+R(123)] × I

I(4) = 40/(40+40) × 8

I(4) = 4mA

Then, using ohms law, we can find the voltage across the resistor 4 and the voltage is the required Voc

V = IR

V4 = Voc = I4 × R4

Voc = 4×10^-3 × 40×10^3

Voc = 160V

Then, the sum of the short circuit voltage and the open circuit voltage will give the required Voc

Voc = Voc(open circuit) + Voc(short circuit)

Voc = 24 + 160

Voc = 184V.

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3 years ago
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Explanation:

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Confirm if this is correct or not. If it isn't correct, please correct it.
kow [346]

Answer:

d = 421.83 m

Explanation:

It is given that,

Height, h = 396.9 m

Horizontal speed, v = 46.87 m/s

We need to find the distance traveled by the ball horizontally. Let t is the time taken by the ball. Using second equation of motion for vertical direction. So,

396.9=0\times t+\dfrac{1}{2}\times 9.8 t^2\\\\t=9\ s

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