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Chapter 23, Problem 50P

(a)

To determine

The rate of deliver of energy

(a)

Expert Solution
Check Mark

Answer to Problem 50P

The rate of deliver of energy is 66.0W.

Explanation of Solution

The rate of deliver of energy is the power of the battery. Write the equation for the power of the battery.

    P=IΔV        (I)

Here, I is the current and ΔV is the voltage of the battery.

Conclusion:

Substitute 3.00A for I and 22.0V for ΔV.

    P=(3.00A)(22.0V)=66.0W        (II)

Therefore, the rate of deliver of energy by the battery is 66.0W.

(b)

To determine

The power delivered to the resistance of the coil

(b)

Expert Solution
Check Mark

Answer to Problem 50P

The power delivered to the resistance of the coil is 45.0W.

Explanation of Solution

Write the equation for the power delivered to the resistance of the coil.

    P=IΔVR        (III)

Here, I is the current and ΔVR is the voltage across the resistance.

Write the equation for the voltage across the resistance.

    ΔVR=IR        (IV)

Here, I is the current and R is the resistance of the resistor. Substitute equation (IV) in equation (III).

    P=I2R

Conclusion:

Substitute 3.00A for I and 5.00Ω for R.

    P=(3.00A)2(5.00Ω)=45.0W        (V)

Therefore, the power delivered to the resistance of the coil is 45.0W.

(c)

To determine

The rate of energy storage

(c)

Expert Solution
Check Mark

Answer to Problem 50P

The rate of storage of energy is 21.0W.

Explanation of Solution

Consider the inductor being ideal and connect in series with an ideal resistor. According to Kirchhoff’s voltage rule, the algebraic sum of all the voltages in any closed loop in a circuit is zero.

Write the equation for the algebraic sum of the voltages across the coil.

+22.0V(3.00A)(5.00Ω)ΔVL=0        (VI)

Here, +22.0V is the voltage across the battery, (3.00A)(5.00Ω) is the voltage across the resistor and ΔVL is the voltage across the inductor.

The rate of storage of energy is the power. Write the equation for the power stored in the inductor.

P=IΔVL        (VII)

Here, I is the current in the current and ΔVL is the voltage across the inductor.

Conclusion:

Rearrange equation (VI) and solve for ΔVL.

ΔVL=+22.0V(3.00A)(5.00Ω)=7.00V

Substitute 3.00A for I and 7.0V for ΔVL in equation (VII).

P=(3.00A)(7.0V)=21.0W        (VIII)

Therefore, the rate of storage of energy in the magnetic field is 21.0W.

(d)

To determine

The relation between the three power values

(d)

Expert Solution
Check Mark

Answer to Problem 50P

The power from the battery is the sum of the power across the internal resistance and the power in the magnetic field.

Explanation of Solution

From equation (II), the battery is delivering energy at a rate of 66.0W.

From equation (V), the power delivered to the resistance of the coil is 45.0W.

From equation (VIII), the rate of storage of energy in the magnetic field is 21.0W.

From the value of different powers given in equation (II), equation (V) and equation (VIII), it can be inferred that 45.0W+21.0W=66.0W

Conclusion:

Therefore, the power delivered from the battery is the sum of the power delivered to the internal resistance and the power stored in the magnetic field.

(e)

To determine

The validity of the relation

(e)

Expert Solution
Check Mark

Answer to Problem 50P

Yes, it is valid in other instants as well

Explanation of Solution

The relation between the powers is that the power from the battery is the sum of the power across the internal resistance and the power in the magnetic field.

At any instant, the power generated by the battery is the sum of the power delivered to the internal resistance and the power stored in the magnetic field.

Conclusion:

Therefore, it is true that the relation between the power is valid at any istant.

(f)

To determine

The relation between the power at given instants

(f)

Expert Solution
Check Mark

Answer to Problem 50P

The power delivered to the resistance is zero at t=0 and all the power is delivered to the resistance after several seconds.

Explanation of Solution

From equation (III) and equation (IV), write the equation for the power delivered to the resistance.

P=I2R

Here, I is the current and R is the resistance of the resistor.

Write the equation for the power delivered by the magnetic field.

P=LdIdt

Here, L is the inductance of the coil and I is the current which changes with time t.

Conclusion:

Immediately after t=0, the power I2R delivered to the internal resistance of the coil is almost zero. At this moment the power delivered to the magnetic field L(dI/dt) is high that almost all the power generated from the battery is stored in the magnetic field.

After some time, the current does not change anymore and hence there is no power being stored in the magnetic field. All the power from the battery is delivered to the resistance of the coil.

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Chapter 23 Solutions

Bundle: Principles of Physics: A Calculus-Based Text, 5th + WebAssign Printed Access Card for Serway/Jewett's Principles of Physics: A Calculus-Based Text, 5th Edition, Multi-Term

Ch. 23 - Prob. 2OQCh. 23 - Prob. 3OQCh. 23 - A circular loop of wire with a radius of 4.0 cm is...Ch. 23 - A rectangular conducting loop is placed near a...Ch. 23 - Prob. 6OQCh. 23 - Prob. 7OQCh. 23 - Prob. 8OQCh. 23 - A square, flat loop of wire is pulled at constant...Ch. 23 - The bar in Figure OQ23.10 moves on rails to the...Ch. 23 - Prob. 11OQCh. 23 - Prob. 12OQCh. 23 - A bar magnet is held in a vertical orientation...Ch. 23 - Prob. 14OQCh. 23 - Two coils are placed near each other as shown in...Ch. 23 - A circuit consists of a conducting movable bar and...Ch. 23 - Prob. 17OQCh. 23 - Prob. 1CQCh. 23 - Prob. 2CQCh. 23 - Prob. 3CQCh. 23 - Prob. 4CQCh. 23 - Prob. 5CQCh. 23 - Prob. 6CQCh. 23 - Prob. 7CQCh. 23 - Prob. 8CQCh. 23 - Prob. 9CQCh. 23 - Prob. 10CQCh. 23 - Prob. 11CQCh. 23 - Prob. 12CQCh. 23 - Prob. 13CQCh. 23 - Prob. 14CQCh. 23 - Prob. 15CQCh. 23 - Prob. 16CQCh. 23 - Prob. 1PCh. 23 - An instrument based on induced emf has been used...Ch. 23 - A flat loop of wire consisting of a single turn of...Ch. 23 - Prob. 4PCh. 23 - Prob. 5PCh. 23 - Prob. 6PCh. 23 - A loop of wire in the shape of a rectangle of...Ch. 23 - When a wire carries an AC current with a known...Ch. 23 - Prob. 9PCh. 23 - Prob. 10PCh. 23 - Prob. 11PCh. 23 - A piece of insulated wire is shaped into a figure...Ch. 23 - A coil of 15 turns and radius 10.0 cm surrounds a...Ch. 23 - Prob. 14PCh. 23 - Figure P23.15 shows a top view of a bar that can...Ch. 23 - Prob. 16PCh. 23 - Prob. 17PCh. 23 - A metal rod of mass m slides without friction...Ch. 23 - Review. After removing one string while...Ch. 23 - Prob. 20PCh. 23 - The homopolar generator, also called the Faraday...Ch. 23 - Prob. 22PCh. 23 - A long solenoid, with its axis along the x axis,...Ch. 23 - Prob. 24PCh. 23 - Prob. 25PCh. 23 - Prob. 26PCh. 23 - A coil of area 0.100 m2 is rotating at 60.0 rev/s...Ch. 23 - A magnetic field directed into the page changes...Ch. 23 - Within the green dashed circle shown in Figure...Ch. 23 - Prob. 30PCh. 23 - Prob. 31PCh. 23 - Prob. 32PCh. 23 - Prob. 33PCh. 23 - Prob. 34PCh. 23 - Prob. 35PCh. 23 - Prob. 36PCh. 23 - Prob. 37PCh. 23 - Prob. 38PCh. 23 - Prob. 39PCh. 23 - Prob. 40PCh. 23 - Prob. 41PCh. 23 - Prob. 42PCh. 23 - Prob. 43PCh. 23 - Prob. 44PCh. 23 - Prob. 45PCh. 23 - Prob. 46PCh. 23 - Prob. 47PCh. 23 - Prob. 48PCh. 23 - Prob. 49PCh. 23 - Prob. 50PCh. 23 - Prob. 51PCh. 23 - Prob. 52PCh. 23 - Prob. 53PCh. 23 - Prob. 54PCh. 23 - Prob. 55PCh. 23 - Prob. 56PCh. 23 - Prob. 57PCh. 23 - Figure P23.58 is a graph of the induced emf versus...Ch. 23 - Prob. 59PCh. 23 - Prob. 60PCh. 23 - The magnetic flux through a metal ring varies with...Ch. 23 - Prob. 62PCh. 23 - Prob. 63PCh. 23 - Prob. 64PCh. 23 - Prob. 65PCh. 23 - Prob. 66PCh. 23 - Prob. 67PCh. 23 - Prob. 68PCh. 23 - Prob. 69PCh. 23 - Prob. 70PCh. 23 - Prob. 71PCh. 23 - Prob. 72PCh. 23 - Review. The use of superconductors has been...Ch. 23 - Prob. 74PCh. 23 - Prob. 75P
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