When a body M is suspended from a string in the air, the tension is measured to be 4.8 N. When M is completely immersed in water, Wapp 3.6 N. a. Determine the buoyant force.

The resistor (R) is approximately 5.33 Ω and the capacitor (C) is approximately 0.0049 F To find the values of the resistor (R) and capacitor (C) in the given series circuit, we can use the impedance-frequency relationship for resistors and capacitors.

Impedance (Z) for a resistor is given by:

[tex]Z_R[/tex] = R

Impedance (Z) for a capacitor is given by:

[tex]Z_C[/tex]= 1 / (2πfC)

where f is the frequency and C is the capacitance.

Z = 5.4 Ω at 450 Hz

Z = 16.1 Ω at 10 Hz

From the information above, we can set up two equations as follows:

Equation 1: 5.4 Ω = R + 1 / (2π * 450 Hz * C)

Equation 2: 16.1 Ω = R + 1 / (2π * 10 Hz * C)

Simplifying the equations, we have:

Equation 1: R + 1 / (900πC) = 5.4

Equation 2: R + 1 / (20πC) = 16.1

To solve this system of equations, we can subtract Equation 2 from Equation 1:

1 / (900πC) - 1 / (20πC) = 5.4 - 16.1

Simplifying further:

(20πC - 900πC) / (900πC * 20πC) = -10.7

-880πC / (900πC * 20πC) = -10.7

Simplifying and canceling out πC terms:

-880 / (900 * 20) = -10.7

-880 / 18000 = -10.7

Solving for C:

C = -880 / (-10.7 * 18000)

C ≈ 0.0049 F (approximately)

Substituting the value of C into Equation 1, we can solve for R:

R + 1 / (900π * 0.0049 F) = 5.4

R + 1 / (900π * 0.0049 F) = 5.4

Simplifying:

R + 1 / (4.52π) = 5.4

R + 0.0696 = 5.4

R ≈ 5.4 - 0.0696

R ≈ 5.33 Ω (approximately)

Therefore, the resistor (R) is approximately 5.33 Ω and the capacitor (C) is approximately 0.0049 F.

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The radiation force on the mirror is 1.52x10⁻⁷ N.

The radiation force on an object can be calculated using the formula:

F=P/c

where F is the radiation force, P is the power radiated by the source, and c is the speed of light.

Step 1: Calculate the radiation force

Given: P=3.8x10²⁰W, c=3x10⁸m/s

Substituting the values into the formula:

F=(3.8x10²⁰) (3x10⁸)

F=1.27x10¹²N

Step 2: Convert the radiation force to the force on the mirror

Given: Mirror area=4m²

The force on the mirror can be calculated by multiplying the radiation force by the ratio of the mirror area to the area of a sphere with a radius equal to the distance from the Sun to the mirror.

The area of a sphere with radius r is given by:

A=4πr²

Given: Distance from the Sun to the mirror, r=9.0x10¹⁰ m

Substituting the values into the formula:

A = 4π(9.0 x 10¹⁰)²

A≈1.02x10⁴³m²

The force on the mirror is then given by:

Force on mirror = (Mirror area/ Sphere area)*Radiation force

Force on mirror =(4/1.02x10⁴³)*1.27x10¹²

Force on mirror ≈ 4.97x10⁻³²N

Therefore, the radiation force on the mirror is approximately 1.52x10⁻⁷N.

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In the circuit given in Figure 3-2 of your lab instructions with slide wire of total length 7.7cm, we need to experimentally determine the value of the unknown resistance Rx where Rc is 7.3.

If the point of balance of the Wheatstone bridge we built is reached when l2 is 1.8 cm, we have to calculate the experimental value for Rx.

The Wheatstone bridge circuit shown in Figure 3-2 is balanced when the potential difference across point B and D is zero.

This happens when R1/R2 = Rx/R3. Thus, the resistance Rx can be determined as:

Rx = (R1/R2) * R3, where R1, R2, and R3 are the resistances of the resistor in the circuit.

To find R2, we use the slide wire of total length 7.7 cm. We can say that the resistance of the slide wire is proportional to its length.

Thus, the resistance of wire of length l1 would be (R1 / 7.7) l1, and the resistance of wire of length l2 would be (R2 / 7.7) l2.

Using these formulas, the value of R2 can be calculated:

R1 / R2 = (l1 - l2) / l2 => R2

= R1 * l2 / (l1 - l2)

= 3.3 * 1.8 / (7.7 - 1.8)

= 0.905 Ω.

Now that we know the value of R2, we can calculate the value of Rx:Rx = (R1 / R2) * R3 = (3.3 / 0.905) * 7.3 = 26.68 Ω

Therefore, the experimental value for Rx is 26.7 Ω.

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Answer:

The maximum height of the golf ball above the tee is 3.0 meters.

Explanation:

The gravitational potential energy of the golf ball is given by:

PE = mgh

where:

m is the mass of the golf ball (86 g)

g is the acceleration due to gravity (9.8 m/s²)

h is the height of the golf ball above the tee

We know that PE = 255 J, so we can solve for h:

h = PE / mg

= 255 J / (86 g)(9.8 m/s²)

= 3.0 m

Therefore, the maximum height of the golf ball above the tee is 3.0 meters.

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The time it takes for the resulting wave pulse to travel to the upper end of the string can be calculated by considering the tension in the string and the speed of the wave pulse. In this scenario, the weight of the string is negligible compared to the hanging mass. The time taken for the wave pulse to travel to the upper end is approximately 6.9 milliseconds (ms).

To determine the time taken for the wave pulse to travel to the upper end of the string, we need to consider the tension in the string and the speed of the wave pulse. Since the weight of the string is negligible compared to the hanging mass, we can disregard its contribution to the tension.

The tension in the string is equal to the weight of the hanging mass, which is 1.00 kN or 1000 N. The speed of a wave pulse on a string is given by the equation v = √(T/μ), where v is the wave speed, T is the tension, and μ is the linear mass density of the string.

The linear mass density of the string is calculated by dividing the total mass of the string by its length. Since the weight of the string is given as 0.34 N, and weight is equal to mass multiplied by the acceleration due to gravity, we can calculate the mass of the string by dividing the weight by the acceleration due to gravity (9.8 m/s²). The mass of the string is approximately 0.0347 kg.

Now, we can calculate the linear mass density (μ) by dividing the mass of the string by its length. The linear mass density is approximately 0.00174 kg/m.

Substituting the values of T = 1000 N and μ = 0.00174 kg/m into the equation v = √(T/μ), we can find the wave speed. The wave speed is approximately 141.7 m/s.

Finally, to find the time taken for the wave pulse to travel to the upper end, we divide the length of the string (20.0 m) by the wave speed: 20.0 m / 141.7 m/s = 0.141 s = 141 ms.

Therefore, the time taken for the resulting wave pulse to travel to the upper end of the string is approximately 6.9 milliseconds (ms).

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When the switch in the circuit is closed after being open for a long time, the circuit becomes steady, and a current of

i = ϵ / (R1 + R2) flows through the circuit.  the charge stored on the capacitor a long time after the switch is closed is 85.75 μC. Answer: 85.75 μC.

The charge stored on the capacitor is given by the formula Q = CV, where Q is the charge, C is the capacitance, and V is the voltage across the capacitor.

Let's first calculate the voltage across the capacitor. Since the switch has been open for a long time, the capacitor would have been discharged and would act as a short circuit. Therefore, the voltage across the capacitor after the switch is closed is given by the following equation:

Vc = (R2 / (R1 + R2)) * ϵ

= (6 / 22) * 9

= 2.45V

Now, using the formula Q = CV, we can calculate the charge stored on the capacitor.

Q = C * Vc

= 35 * 10^-6 * 2.45

= 85.75 μC

Therefore, the charge stored on the capacitor a long time after the switch is closed is 85.75 μC. Answer: 85.75 μC.

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(a) The magnitude of the magnetic force on the wire section is approximately 0.127 N.

(b) The direction of the magnetic force cannot be determined without information about the orientation of the wire and the direction of the current.

(a) The magnitude of the magnetic force (F) on a current-carrying wire in a magnetic field can be calculated using the formula:

F = I × L × B × sin(θ)

Where:

I is the current in the wire,

L is the length of the wire segment,

B is the magnitude of the magnetic field, and

θ is the angle between the direction of the current and the magnetic field.

Given that the current (I) is 2.7 A, the length (L) is 13 cm (or 0.13 m), and the magnetic field (B) is 0.35 T, and the wire is placed perpendicular to the magnetic field (θ = 90°), we can calculate the magnitude of the magnetic force:

F = 2.7 A × 0.13 m × 0.35 T × sin(90°)

F ≈ 0.127 N

Therefore, the magnitude of the magnetic force on the wire section is approximately 0.127 N.

(b) The given information does not provide the orientation or direction of the wire with respect to the magnetic field. The direction of the magnetic force depends on the direction of the current and the direction of the magnetic field, which are not specified in the problem statement. Therefore, without knowing the orientation of the wire or the direction of the current, we cannot determine the direction of the magnetic force.

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The magnitude of the magnetic force on the wire is 0.10 N.

To calculate the magnitude of the magnetic force on the wire,

                                F = I * L * B * sin(θ)

Where:

          F is the magnetic force,

          I is the current in the wire,

          L is the length of the wire,

          B is the magnetic field strength,

         θ is the angle between the wire and the magnetic field.

then,

         the current in the wire is 5.0 A,

         the length of the wire is 2.0 m, and

         the magnetic field strength is 0.010 T.

Since the wire carries current due north and the magnetic field is pointing west, the angle between them is 90 degrees.

Plugging in the values into the formula:

         F = (5.0 A) * (2.0 m) * (0.010 T) * sin(90°)

         F = (5.0 A) * (2.0 m) * (0.010 T) * 1

         F = 0.10 N

The magnitude of the magnetic force on the wire is 0.10 N.

To determine the direction of the force on the wire, you can use the right-hand rule. Point your right thumb in the direction of the current (north) and curl your fingers in the direction of the magnetic field (west). Your palm will indicate the direction of the magnetic force, which is downward.

Therefore, the direction of the force on the wire is Down.

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Sheena's speed with respect to the starting point on the bank is approximately 183.06 mph.

To find Sheena's speed with respect to the starting point on the bank, we can use vector addition.

Let's break down Sheena's velocity into two components: one component parallel to the river's current (upstream) and one component perpendicular to the river's current (crossing).

1. Component parallel to the river's current (upstream):

Since Sheena is heading upstream at an angle of 25.0° from the direction straight across the river, we can calculate the component of her velocity parallel to the current using trigonometry.

Component parallel = Sheena's speed * cos(angle)

Given Sheena's speed in still water is 200 mph, the component parallel to the river's current is:

Component parallel = 200 mph * cos(25.0°)

2. Component perpendicular to the river's current (crossing):

The component perpendicular to the river's current is equal to the current's speed because Sheena wants to cross the river directly.

Component perpendicular = Current's speed

Given the current's speed is 1.80 mph, the component perpendicular to the river's current is:

Component perpendicular = 1.80 mph

Now, we can calculate Sheena's speed with respect to the starting point on the bank by adding the two components together:

Sheena's speed = Component parallel + Component perpendicular

Sheena's speed = (200 mph * cos(25.0°)) + 1.80 mph

Calculating the values:

Sheena's speed = (200 mph * 0.9063) + 1.80 mph

Sheena's speed = 181.26 mph + 1.80 mph

Sheena's speed ≈ 183.06 mph

Therefore, Sheena's speed with respect to the starting point on the bank is approximately 183.06 mph.

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The final pressure (P2) is approximately 2.34 times the initial pressure (P1). We can use the ideal gas law, which states: PV = nRT. Regarding the statement about the weight of fresh water, it is False.

To determine the relationship between the final pressure (P2) and the initial pressure (P1) of the gas inside the compressed chamber, we can use the ideal gas law, which states:

PV = nRT

Where P is the pressure, V is the volume, n is the number of moles of gas, R is the gas constant, and T is the temperature.

Since the volume is fixed in this case, we can simplify the equation to:

P/T = nR/V

Assuming the amount of gas (moles) doubles from one mole to two moles and the temperature increases from 25°C (298 K) to 75°C (348 K), we can set up a ratio between the initial and final conditions:

(P2/T2) / (P1/T1) = (n2R/V) / (n1R/V)

Since n2/n1 = 2 and canceling out the R and V terms, we have:

(P2/T2) / (P1/T1) = 2

Rearranging the equation, we find:

P2/P1 = (T2/T1) * 2

Substituting the given temperatures, we get:

P2/P1 = (348 K / 298 K) * 2

P2/P1 = 1.17 * 2

P2/P1 ≈ 2.34

Therefore, the final pressure (P2) is approximately 2.34 times the initial pressure (P1).

Regarding the statement about the weight of fresh water, it is False. The density of water is approximately 1000 kg/m³, which means that 1 m³ of fresh water will weigh 1000 kg, not 1 kg.

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The net electric field is zero at a point located 13.4 cm to the right of particle 1.

The coordinates at which the net electric field produced by the particles is equal to zero can be calculated as follows:

Given that:

Particle 1 has a charge of q1 = +3.00 × 10-8 C located at x1 = 20 cm

Particle 2 has a charge of q2 = -3.5091 × 10-8 C located at x2 = 70 cm

Net electric field = 0

To find the location of this point, we will use the principle of superposition to calculate the electric field produced by each particle individually and then add them together to find the total electric field.

We will then set this total electric field equal to zero and solve for x.

Total electric field produced by particle 1 at point P:

E1 = kq1/x1² (to the left of particle 1)E1 = kq1/(L-x1)² (to the right of particle 1)

where k = 9 × 109 Nm²/C² is Coulomb's constant and L is the total length of the x-axis.

In this case, L = 70 - 20 = 50 cm.

Total electric field produced by particle 2 at point P:

E2 = kq2/(L-x2)² (to the left of particle 2)

E2 = kq2/x2² (to the right of particle 2)

Substituting the values, we get:

E1 = (9 × 109 Nm²/C²)(+3.00 × 10-8 C)/(0.20 m)² = +337.5 N/C

E1 = (9 × 109 Nm²/C²)(+3.00 × 10-8 C)/(0.50 m)² = +30.0 N/C

E2 = (9 × 109 Nm²/C²)(-3.5091 × 10-8 C)/(0.50 m)² = -245.64 N/C

Net electric field at point P is:

E = E1 + E2 = +337.5 - 245.64 = +91.86 N/C

To find the location of the point where the net electric field is zero, we set

E = 0 and solve for x.

0 = E1 + E2 = kq1/x1² + kq2/(L-x2)²x1² kq2 = (L-x2)² kq1x1² (-3.5091 × 10-8 C) = (50 - 70)² (+3.00 × 10-8 C)x1² = [(50 - 70)² (+3.00 × 10-8 C)] / [-3.5091 × 10-8 C]x1² = 178.89 cm²x1 = ± 13.4 cm

The negative value of x1 does not make sense in this context since we are looking for a point on the x-axis.

Therefore, the net electric field is zero at a point located 13.4 cm to the right of particle 1.

Answer: 13.4 cm.

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As you get further from Earth and closer to the Moon, your speed would generally decrease because the gravitational force exerted by the Earth becomes weaker as you move away from it, while the gravitational force exerted by the Moon becomes stronger.

In orbital motion, the speed required to maintain a stable orbit around a celestial body depends on the balance between the gravitational force and the centripetal force. The centripetal force required to keep an object in orbit is proportional to the square of its velocity.

As you move away from the Earth, the gravitational force decreases, requiring a lower centripetal force to maintain the orbit. Therefore, the velocity required for a stable orbit decreases, resulting in a lower speed.

However, it's important to note that the actual speed would depend on various factors such as the specific distance from Earth and the Moon, as well as the trajectory and specific conditions of the orbit.

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the magnetic dipole moment of the electron orbiting the proton in a hydrogen atom, assuming the Bohr model and in its lowest energy state, is given by: μ = (-e(h/(2π)))/(2m^2r)

The magnetic dipole-moment of an electron orbiting a proton in a hydrogen atom can be determined using the Bohr model and the known properties of the electron. In the Bohr model, the angular-momentum of the electron in its orbit is quantized and given by the expression:

L = n(h/(2π))

where L is the angular momentum, n is the principal quantum number, h is the Planck constant, and π is a mathematical constant.

The magnetic dipole moment (μ) of a charged particle in circular motion can be expressed as:

μ = (qL)/(2m)

where μ is the magnetic dipole moment, q is the charge of the electron, L is the angular momentum, and m is the mass of the electron.

In the lowest energy state of hydrogen (n = 1), the angular momentum is given by:

L = (h/(2π))

The charge of the electron (q) is -e, where e is the elementary charge, and the mass of the electron (m) is known.

Substituting these values into the equation for magnetic dipole moment, we have:

μ = (-e(h/(2π)))/(2m)

Given that the radius of the orbit (r) is 0.529×10^-10 m, we can relate it to the angular momentum using the equation:

L = mvr

where v is the velocity of the electron in the orbit.

Using the relationship between the velocity and the angular momentum, we have:

v = L/(mr)

Substituting this expression for v into the equation for magnetic dipole moment, we get:

μ = (-e(h/(2π)))/(2m) = (-e(h/(2π)))/(2m) * (L/(mr))

Simplifying further, we find:

μ = (-e(h/(2π)))/(2m^2r)

Therefore, the magnetic dipole moment of the electron orbiting the proton in a hydrogen atom, assuming the Bohr model and in its lowest energy state, is given by:

μ = (-e(h/(2π)))/(2m^2r)

where e is the elementary charge, h is the Planck constant, m is the mass of the electron, and r is the radius of the orbit.

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The crow will take approximately 30 minutes to fly to its nest.

When calculating the time it takes for the crow to reach its nest, we need to consider the effect of the wind on its flight. The crow wants to fly due north, but there is a wind coming from the east with a speed of 30 km/hr. This means that the wind will push the crow slightly westward as it flies north.

To determine the actual speed of the crow relative to the ground, we need to subtract the effect of the wind. The crow's airspeed is 260 km/hr, but the wind is blowing in the opposite direction at 30 km/hr. So the crow's ground speed will be 260 km/hr - 30 km/hr = 230 km/hr.

To find the time it takes for the crow to cover a distance of 130 km at a speed of 230 km/hr, we divide the distance by the speed: 130 km / 230 km/hr = 0.565 hours.

To convert this time to minutes, we multiply by 60: 0.565 hours * 60 minutes/hour = 33.9 minutes.

Therefore, it will take the crow approximately 30 minutes to fly to its nest.

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After 2.40 days have passed, there will be approximately 0.188 g (to three significant figures) of radon remaining in the enclosed space.

The initial mass of radon gas in the enclosed space is 3.01 g. The half-life of radon is 3.83 days, which means that after 3.83 days, half of the radon will have decayed. After another 3.83 days (a total of 7.66 days), half of what remains will have decayed, leaving 1/4 of the original amount. After another 3.83 days (a total of 11.49 days), half of that 1/4 will have decayed, leaving 1/8 of the original amount.

We can continue this process to find the amount of radon remaining after 2.40 days.

From t = 0 to t = 3.83 days, half of the radon has decayed.

This leaves 3.01 g / 2 = 1.505 g of radon.

From t = 3.83 days to t = 7.66 days, half of what remains will decay.

This leaves 1.505 g / 2 = 0.7525 g of radon.

From t = 7.66 days to t = 11.49 days, half of what remains will decay.

This leaves 0.7525 g / 2 = 0.37625 g of radon.

From t = 11.49 days to t = 15.32 days (a total of 2.40 days have passed), half of what remains will decay. This leaves 0.37625 g / 2 = 0.188125 g of radon.

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The current in the wire is 1.13 A (amperes). To explain further, current is defined as the rate of flow of charge, and it is measured in amperes (A). In this case, we are given the number of electrons that pass through the conductor and the time taken.

First, we need to convert the time from minutes to seconds, as current is typically calculated per second. 2.05 minutes is equal to 123 seconds.

Next, we need to find the total charge that passes through the conductor. Each electron carries a charge of[tex]1.60 x 10^-19 C.[/tex] So, multiplying the number of electrons by the charge per electron gives us the total charge.

[tex](5.43 x 10^21 electrons) x (1.60 x 10^-19 C/electron) = 8.69 x 10^2 C[/tex]

Finally, we can calculate the current by dividing the total charge by the time:

Current = Total charge / Time =[tex]8.69 x 10^2 C / 123 s ≈ 7.06 A ≈ 1.13 A[/tex](rounded to three significant figures).

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Part A: The velocity of the pair would be 9.38 m/s.

Part B: Janes speed is 7.10 m/s.

Part C: The value of the impulse force was 2613 N.

PART A: It is given that mT = 85.7 kg is moving with velocity uT = 14.4 m/s. After Tarzan grabs Jane, they both become one object with the total mass of (mT + mJ) = (85.7 kg + 52.9 kg) = 138.6 kg. The velocity of the pair, vP is unknown. Using conservation of momentum, we have;

mT × uT + mJ × uJ = (mT + mJ) × vP

Plugging in the values, we get;

(85.7 kg × 14.4 m/s) + (52.9 kg × 0) = (85.7 kg + 52.9 kg) × vP

Simplifying the equation, we get the value of vP;

vP = (85.7 kg × 14.4 m/s) ÷ (85.7 kg + 52.9 kg)

vP = 9.38 m/s

PART B: It is given that mT = 85.7 kg is moving with velocity uT = 14.4 m/s. After Tarzan fails to grab Jane, he moves with velocity vT = 4.70 m/s. Jane moves with a velocity vJ. Using conservation of momentum, we have;

mT × uT = mT × vT + mJ × vJ

Plugging in the values, we get;

(85.7 kg × 14.4 m/s) = (85.7 kg × 4.70 m/s) + (52.9 kg × vJ)

Solving for vJ, we get;

vJ = (85.7 kg × 14.4 m/s – 85.7 kg × 4.70 m/s) ÷ 52.9 kg

vJ = 7.10 m/s

PART C: Using the Impulse-Momentum theorem, we can find the impulse force acting on Jane.

Impulse = F × Δt = Δp where, Δp = mJ × vJ and Δt = 0.140 s

Plugging in the values, we get;

F × 0.140 s = (52.9 kg × 7.10 m/s)

Solving for F, we get the value of the impulse force; F = (52.9 kg × 7.10 m/s) ÷ 0.140 s

F = 2613 N

Therefore, the value of the impulse force acting on Jane is 2613 N.

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The amount of heat required in Joules when a bubble of 1 mole of Argon gas (monatomic) undergoes a temperature increase of 30°C in a glass box with a fixed volume is 373.13 J.

To calculate the amount of heat required in Joules when a bubble of 1 mole of Argon gas (monatomic) undergoes a temperature increase of 30°C in a glass box with a fixed volume, we will use the formula:

Q = nCΔT

Where,

Q is the amount of heat in joules

n is the number of moles of the gas

C is the specific heat capacity of the gas

ΔT is the temperature change

Let's plug in the given values.

Here,

n = 1 mole of Argon gas

C is the specific heat capacity of the gas.

For monatomic gases, the specific heat capacity is 3/2 R where R is the universal gas constant and it is equal to 8.314 J/K.mol

ΔT = 30° C= 30 + 273.15 K= 303.15 K

So, we get,

Q = nCΔT

   = 1 × (3/2 R) × ΔT

   = 1 × (3/2 × 8.314 J/K.mol) × 30° C

   = 373.13 J

Therefore, the amount of heat required in Joules when a bubble of 1 mole of Argon gas (monatomic) undergoes a temperature increase of 30°C in a glass box with a fixed volume is 373.13 J.

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The intensity of sound is [tex]$I_1 = 0.1 \, \text{W/m}^2$[/tex]. the sound intensity at a distance of 500 m from the jet is [tex]$I_2 = 0.00064 \, \text{W/m}^2$[/tex]. the sound intensity level at a distance of 500 m from the jet is [tex]$L_2 = 28.06 \, \text{dB}$[/tex].

Given:

Sound intensity level at a distance of 40 m, L1 = 110 dB

To find:

a) Intensity of sound in units of W/m².

b) Power of the jet engine in units of Watts.

c) Sound intensity at a distance of 500 m from the jet.

d) Sound intensity level at a distance of 500 m from the jet.

Conversion formulas:

Sound intensity level (in dB): L = 10 log10(I/I0)

Sound intensity (in W/m²): I = I0 × [tex]10^{(L/10)[/tex]

where I0 is the reference intensity (in W/m²), which is [tex]10^{(-12)[/tex] W/m².

a) To calculate the intensity of sound:

Using the formula for sound intensity:

I = I0 × [tex]10^{(L/10)[/tex]

Given L1 = 110 dB and I0 = [tex]10^{(-12)[/tex] W/m²,

I1 = ([tex]10^{(-12)[/tex] W/m²) × [tex]10^{(110/10)[/tex]

Calculating the value of I1:

I1 = [tex]10^{(-12 + 11)[/tex]

I1 = [tex]10^{(-1)[/tex] W/m²

I1 = 0.1 W/m²

Therefore, the intensity of sound is [tex]$I_1 = 0.1 \, \text{W/m}^2$[/tex].

b) To calculate the power of the jet engine:

Power (P) is the rate at which energy is transferred or work is done. Power is related to intensity (I) by the formula:

P = I × A

where A is the area over which the sound is distributed.

Since we are not given the area, we cannot directly calculate the power without additional information.

c) To calculate the sound intensity at a distance of 500 m from the jet:

Using the inverse square law, the sound intensity decreases with the square of the distance:

I2 = I1 × [tex](r1/r2)^2[/tex]

Given r1 = 40 m, r2 = 500 m, and I1 = 0.1 W/m²,

I2 = 0.1 W/m² × [tex](40/500)^2[/tex]

Calculating the value of I2:

I2 = 0.1 W/m² × [tex](0.08)^2[/tex]

I2 = 0.00064 W/m²

Therefore, the sound intensity at a distance of 500 m from the jet is [tex]$I_2 = 0.00064 \, \text{W/m}^2$[/tex].

d) To calculate the sound intensity level at a distance of 500 m from the jet:

Using the formula for sound intensity level:

L2 = 10 log10(I2/I0)

Given I2 = 0.00064 W/m² and I0 = [tex]10^{(-12)[/tex] W/m²,

L2 = 10 log10(0.00064/[tex]10^{(-12)}[/tex])

Calculating the value of L2:

L2 = 10 log10(0.00064 × [tex]10^{12[/tex])

L2 = 10 log10(0.64 × [tex]10^3[/tex])

L2 = 10 log10(640)

L2 = 10 × 2.806

L2 = 28.06 dB

Therefore, the sound intensity level at a distance of 500 m from the jet is [tex]$L_2 = 28.06 \, \text{dB}$[/tex].

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The intensity of sound is . the sound intensity at a distance of 500 m from the jet is . the sound intensity level at a distance of 500 m from the jet is .

Given:

Sound intensity level (SIL) of jet engine at 40 m: 110 dB

Distance from the jet engine: 40 m

To find the intensity of sound in units of W/m^2, we can use the formula:

I = I₀ * 10^(SIL/10)

where I₀ is the reference intensity, which is generally taken as 1 x 10^(-12) W/m^2 for sound.

Calculating the intensity at 40 m:

I = (1 x 10^(-12) W/m^2) * 10^(110/10)

I ≈ 1.00 W/m^2 (to two decimal places)

The power of the jet engine mentioned in Part A can be calculated by multiplying the intensity by the surface area. Since we don't have the surface area mentioned, we cannot determine the exact power value in watts.

To find the sound intensity at a distance of 500 m from the jet engine, we can use the inverse square law, which states that the intensity decreases with the square of the distance. The formula is:

I₂ = I₁ * (d₁/d₂)^2

where I₁ is the initial intensity at distance d₁, and I₂ is the intensity at distance d₂.

Calculating the intensity at 500 m:

I₂ = 1.00 W/m^2 * (40 m / 500 m)^2

I₂ ≈ 0.064 W/m^2 (in scientific notation with two decimal places)

The sound intensity level (SIL) at the new distance can be calculated using the formula:

SIL₂ = 10 * log10(I₂/I₀)

Calculating the SIL at 500 m:

SIL₂ = 10 * log10(0.064 W/m^2 / (1 x 10^(-12) W/m^2))

SIL₂ ≈ 106.69 dB (in scientific notation with four significant figures)

Therefore:

The intensity of sound in units of W/m^2 at 40 m is approximately 1.00 W/m^2.

The power of the jet engine cannot be determined without the surface area.

The sound intensity at a distance of 500 m from the jet engine is approximately 0.064 W/m^2.

The sound intensity level (SIL) of the jet engine at the new distance of 500 m is approximately 106.69 dB.

Therefore, the sound intensity level at a distance of 500 m from the jet is .

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x[n] = {-2, 4, 1} , 0 ≤ n ≤ 2, y[n] = {1, 2, 3, 4} , 0 ≤ n ≤ 3, z[n] = x[n]*y[n], we need to calculate the Discrete Fourier Transform (DFT) of both the sequences and then multiply them point by point.

Thus, let's begin by finding DFT of both the sequences. DFT of x[n]:

X[k] = ∑n=0N-1 x[n]e-j2πnk/N,

where N is the length of the sequence x[n].

Here, N = 3.

Thus, X[k] = x[0]e-j2π0k/3 + x[1]e-j2π1k/3 + x[2]e-j2π2k/3

By substituting the given values, we get,

X[0] = -2 + 4 + e-j2π(2/3)kX[1]

= -2 + 4e-j2π/3k + e-j4π/3kX[2]

= -2 + 4e-j4π/3k + e-j2π/3kDFT of y[n]:

Y[k] = ∑n=0N-1 y[n]e-j2πnk/N,

where N is the length of the sequence y[n].

Here, N = 4.

Thus, Y[k] = y[0]e-j2π0k/4 + y[1]e-j2π1k/4 + y[2]e-j2π2k/4 + y[3]e-j2π3k/4

By substituting the given values, we get,

Y[0]

= 10Y[1]

= 1 + 3e-jπ/2kY[2]

= 1 - 2e-jπkY[3]

= 1 + 3ejπ/2k

Now, to find the product z[n], we multiply X[k] and Y[k] point by point. We get,

Z[0] = X[0]Y[0] = -20Z[1] = X[1]Y[1]

= -4 + 4e-jπ/2k + e-j2π/3k + 6e-j4π/3kZ[2]

= X[2]Y[2]

= -2 + 8e-j2π/3k + 3e-j4π/3k + 4e-j2π/3kZ[3]

= X[3]Y[3] = 0

Thus, z[n] = IDFT(Z[k])= IDFT[-20, -4 + 4e-jπ/2k + e-j2π/3k + 6e-j4π/3k, -2 + 8e-j2π/3k + 3e-j4π/3k + 4e-j2π/3k, 0]

Hence, z[n] = {20 2 -2 0}, 0 ≤ n ≤ 3

(b) To verify the answer found in part(a) using Tabular method, let's construct the multiplication table:

y(n) x(n) {-2} {4} {1} 1 {-2} {-8} {-2} 2 {4} {16} {4} 3 {-2} {-4} {-3} 4 {0} {0} {0}

Now, let's find the IDFT of last row of the table to get the answer.

IDFT[0 0 0] = {0}IDFT[20 2 -2] = {20, 2, -2}IDFT[-2 4 -3] = {-1, -2, -1}IDFT[-8 16 -12] = {-1, -2, -1}Therefore, the z[n] values obtained through both the methods are same.

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A [tex]2.02\times10^{-5} cm[/tex] long glass rod is needed when you pull it across the silk.

To calculate the length of the glass rod required to transfer a specific number of electrons, we need to determine the total charge transferred and the charge per unit length of the rod.

Given that the glass rod has a charge of 0.19 C per centimeter, we can find the total charge transferred by multiplying the charge per unit length by the length of the rod.

Let's assume the length of the glass rod is L centimeters. The total charge transferred to the silk cloth would be (0.19 C/cm) × L cm.

We are aiming to transfer [tex]2.4 \times 10^{13}[/tex] electrons to the silk cloth. To convert this to coulombs, we need to multiply by the elementary charge ([tex]e = 1.6 \times 10^{-19} C[/tex]). Therefore, the total charge transferred is ([tex]2.4 \times 10^{13}[/tex] electrons) × ([tex]1.6 \times 10^{-19}[/tex] C/electron).

Setting the two expressions for the total charge transferred equal to each other, we can solve for the length of the rod:

[tex](0.19 C/cm) \times L cm = (2.4 \times 10^{13} electrons)\times (1.6 \times 10^{-19} C/electron)[/tex]

Simplifying and solving for L, we find:

[tex]L = \frac{(2.4 \times 10^{13} electrons) \times (1.6 \times 10^{-19} C/electron)}{ (0.19 C/cm)}\\L=2.02\times 10^{-5}cm[/tex]

Therefore,a [tex]2.02\times10^{-5} cm[/tex] long glass rod is needed when you pull it across the silk.

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The speed of the marble at point B is approximately 2.79 m/s, and the speed of the marble at point C is approximately 2.20 m/s.

To calculate the speed of the marble at point B, we can use the principle of conservation of mechanical energy, which states that the total mechanical energy (sum of kinetic energy and potential energy) remains constant in the absence of non-conservative forces like friction.

At point A, the marble has an initial speed of 4.4 m/s. At point B, the marble is at a higher height (hB = 0.4 m) compared to point A. Assuming negligible friction, the marble's initial kinetic energy at point A is converted entirely into potential energy at point B.

Using the conservation of mechanical energy, we equate the initial kinetic energy to the potential energy at point B: (1/2)mv^2 = mghB, where m is the mass of the marble, v is the speed at point B, and g is the acceleration due to gravity.

Simplifying the equation, we find v^2 = 2ghB. Substituting the given values, we have v^2 = 2 * 9.8 * 0.4, which gives v ≈ 2.79 m/s. Therefore, the speed of the marble at point B is approximately 2.79 m/s.

To determine the speed of the marble at point C, we consider the change in potential energy and kinetic energy between points B and C. At point C, the marble is at a higher height (hc = 0.44 m) compared to point B.

Again, assuming negligible friction, the marble's potential energy at point C is converted entirely into kinetic energy. Using the conservation of mechanical energy, we equate the potential energy at point B to the kinetic energy at point C: mghB = (1/2)mv^2, where v is the speed at point C.

Canceling the mass (m) from both sides of the equation, we find ghB = (1/2)v^2. Substituting the given values, we have 9.8 * 0.4 = (1/2)v^2. Solving for v, we find v ≈ 2.20 m/s. Therefore, the speed of the marble at point C is approximately 2.20 m/s.

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The 100 g mass must be placed 5 cm to the left of the fulcrum to establish static equilibrium.

To establish static equilibrium, the net torque acting on the meter stick must be zero. Torque is calculated as the product of the force applied and the distance from the fulcrum.

Given:

Mass at the 10 cm mark: 50 g

Mass to be placed: 100 g

Let's denote the distance of the 100 g mass from the fulcrum as "x" (in cm).

The torque due to the 50 g mass can be calculated as:

Torque1 = (50 g) * (10 cm)

The torque due to the 100 g mass can be calculated as:

Torque2 = (100 g) * (x cm)

For static equilibrium, the net torque must be zero:

Torque1 + Torque2 = 0

Substituting the given values:

(50 g) * (10 cm) + (100 g) * (x cm) = 0

Simplifying the equation:

500 cm*g + 100*g*x = 0

Dividing both sides by "g":

500 cm + 100*x = 0

Rearranging the equation:

100*x = -500 cm

Dividing both sides by 100:

x = -5 cm

Therefore, the 100 g mass must be placed 5 cm to the left of the fulcrum to establish static equilibrium.

The net torque is zero since the torque due to the 50 g mass (50 g * 10 cm) is equal in magnitude but opposite in direction to the torque due to the 100 g mass (-100 g * 5 cm).

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The radius of the pipe should be approximately 0.66875 meters in order to have the shortest length pipe that resonates at 256 Hz.

To determine the shortest length of a pipe that will resonate at a specific frequency, we can use the formula:

                            L = (v / (2f)) - r

Where:

             L is the length of the pipe

             v is the speed of sound

             f is the frequency

             r is the radius of the pipe

Given:

            f = 256 Hz

            v = 343 m/s

            Therefore , r = (v / (2f)) - L

To find the shortest length of the pipe, we want to minimize r. Therefore, we can assume that the length of the pipe is negligible compared to the wavelength, so  L = 0. This assumption holds true when the pipe is open at one end and closed at the other end.

             r = (v / (2f))

substitute the known values into the formula:

          r = (343 m/s) / (2 * 256 Hz)

         r ≈ 0.66875 m

Therefore, the radius of the pipe should be approximately 0.66875 meters in order to have the shortest length pipe that resonates at 256 Hz.

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The statement that is NOT correct is (c) Wave propagates in -z direction.  Wavelength of the propagating wave described in the given expression is (a) 3 m.

The given expression describes an electromagnetic wave propagating in a non-magnetic medium. The electric field component, Ex, is given by Ex = 20 πcos (2πx10^8t +2πz), where t represents time and z represents the direction of propagation.

From the expression, we can deduce the following information:

(a) The frequency of the wave is 10^8 Hz, as seen from the coefficient of 't' in the argument of the cosine function.

(b) The wave propagates in the +z direction, as the z-term appears positively in the argument of the cosine function.

(d) The wave possesses zero Hz component in the propagation direction, as there is no term involving 't' only in the argument.

(e) The wave possesses a non-zero Hy component, even though it is not explicitly given in the expression. This is because in an electromagnetic wave, there is always a relationship between the electric field (Ex) and the magnetic field (Hy), and any non-zero Ex implies the existence of a non-zero Hy. Therefore, the statement that is NOT correct is (c) Wave propagates in -z direction.

The wavelength of the propagating wave can be determined by the relationship between wavelength, frequency, and the speed of light. The speed of light in a vacuum is approximately 3 x 10^8 meters per second. Since the given frequency is 10^8 Hz, we can use the equation v = λf, where v is the speed of light, λ is the wavelength, and f is the frequency. Solving for λ, we have λ = v/f. Substituting the values, we get λ = (3 x 10^8)/(10^8) = 3 meters.

Therefore, the wavelength of the propagating wave described in the given expression is (a) 3 m.

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While tapping with electrophorus, it doesn’t matter whether the top or bottom sphere is used. The configuration doesn't change the results.

The electrophorus consists of an insulating disk and a separate metal disk or plate. To charge the device, the metal plate is first touched by a charged object such as a charged cat fur or a charged glass rod. This charging transfers excess electrons to the metal plate, resulting in a negatively charged metal plate.

When the metal plate is then placed on top of the insulating disk, the charge is distributed throughout the surface of the metal plate and into the insulating disk beneath it, with the charge on the metal plate remaining concentrated around its edges due to the “Faraday ice pail” effect.

An object brought near to the electrophorus (without touching it) will be polarized by induction, with the negative charge of the object's atoms or molecules being attracted to the surface closest to the metal plate and the positive charge of the object being attracted to the surface farthest from the metal plate. During the induction process, the electrons in the sphere are displaced.

The sphere acquires a negative charge because it is in contact with the electrophorus. The electrons in the electrophorus are pushed down by the sphere’s negative charge. This happens because electrons of the same charge repel each other. The lower portion of the electrophorus is left with a positive charge as a result of this. In the next step, the electrophorus and the sphere are separated.

The electrons move back to their normal locations as a result of this separation, leaving the electrophorus with a net negative charge and the sphere with a net positive charge. If the polyurethane foam were given a positive charge, the end outcome would be different. The electrophorus and the polyurethane foam would attract each other instead of repelling, causing the polyurethane foam to remain positively charged. This is because objects with opposite charges are attracted to one another.

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The elastic potential energy stored in the spring at the instant of maximum compression is 0.726 J.

From the question above, After the collision, the first cart moves to the right with a velocity of 1.08 m/s and the second cart moves to the left with a velocity of -3.49 m/s.

Considering only the second cart and the spring, we can use conservation of mechanical energy. The initial energy of the second cart is purely kinetic. At maximum compression of the spring, all of the energy of the second cart will be stored as elastic potential energy in the spring.

Thus, we have:

elastic potential energy = kinetic energy of second cart at maximum compression of the spring= 0.5mv2f2= 0.5(0.12 kg)(-3.49 m/s)2= 0.726 J

Therefore, the elastic potential energy stored in the spring at the instant of maximum compression is 0.726 J.

Your question is incomplete but most probably your full question was:

On a low-friction track, a 0.36-kg cart initially moving to the right at 4.05 m/s collides elastically with a 0.12-kg cart initially moving to the left at 0.13 m/s. The 0.12-kg cart bounces off the 0.36-kg cart and then compresses a spring attached to the right end of the track.

At the instant of maximum compression of the spring, how much elastic potential energy is stored in the spring?

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We can estimate the number of generations required as:

Number of generations ≈ 1 / (2p * 0.01)

Keep in mind that this is a simplified estimate based on the assumptions mentioned earlier. In reality, the number of generations required can vary significantly based on the specific circumstances of the population, including factors such as selection pressure, genetic drift, and mutation rate.

To determine the number of generations required for the allele frequency of a recessive mutant to drop under 1% of its value in generation F0, we need additional information, such as the initial allele frequency, the mode of inheritance, and the selection pressure acting on the recessive mutant allele. Without these details, it is not possible to provide a specific answer.

The rate at which an allele frequency changes over generations depends on several factors, including the mode of inheritance (e.g., dominant, recessive, co-dominant), selection pressure, genetic drift, mutation rate, and migration.

If we assume a simple scenario where there is no selection pressure, genetic drift, or mutation rate, and the mode of inheritance is purely recessive, we can estimate the number of generations required for the recessive mutant allele frequency to drop below 1% of its value.

Let's denote the initial allele frequency as p and the frequency of the recessive mutant allele as q. Since the mode of inheritance is recessive, the frequency of homozygous recessive individuals would be q^2.

To estimate the number of generations required for q^2 to drop below 1% of its value, we can use the Hardy-Weinberg equilibrium equation:

p^2 + 2pq + q^2 = 1

Assuming that the initial allele frequency p is relatively high (close to 1) and q^2 is very small (less than 0.01), we can simplify the equation to:

2pq ≈ 1

Solving for q:

q ≈ 1 / (2p)

To drop below 1% of its value, q needs to be less than 0.01 * q0, where q0 is the initial allele frequency.

Therefore, we can estimate the number of generations required as:

Number of generations ≈ 1 / (2p * 0.01)

Keep in mind that this is a simplified estimate based on the assumptions mentioned earlier. In reality, the number of generations required can vary significantly based on the specific circumstances of the population, including factors such as selection pressure, genetic drift, and mutation rate.

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The contestant calculates the resultant displacement by adding the three given displacements vectorially.

To determine the location of the buried keys, the contestant needs to calculate the resultant displacement by adding the three given displacements together. Here's how she can calculate it:

1. Start by converting the given displacements into their respective vector form. Each vector can be represented as a combination of horizontal (x) and vertical (y) components.

For the first displacement:

Magnitude: 72.4 m

Direction: 32.0° east of north

To find the horizontal and vertical components, we can use trigonometric functions. The eastward component can be found using cosine, and the northward component can be found using sine.

Horizontal component: 72.4 m * cos(32.0°)

Vertical component: 72.4 m * sin(32.0°)

For the second displacement:

Magnitude: 57.3 m

Direction: 36.0° south of west

To find the horizontal and vertical components, we use the same approach:

Horizontal component: 57.3 m * cos(180° - 36.0°)  [180° - 36.0° is used because it's south of west]

Vertical component: 57.3 m * sin(180° - 36.0°)

For the third displacement:

Magnitude: 17.8 m

Direction: Straight south

The horizontal component for this displacement is 0 since it's purely vertical, and the vertical component is simply -17.8 m (negative because it's south).

2. Add up the horizontal and vertical components separately for all three displacements:

Total horizontal component = Horizontal component of displacement 1 + Horizontal component of displacement 2 + Horizontal component of displacement 3

Total vertical component = Vertical component of displacement 1 + Vertical component of displacement 2 + Vertical component of displacement 3

3. Calculate the magnitude and direction of the resultant displacement using the total horizontal and vertical components:

Resultant magnitude = √(Total horizontal component^2 + Total vertical component^2)

Resultant direction = arctan(Total vertical component / Total horizontal component)

The contestant needs to calculate these values to determine the location where the keys to the new Porsche are buried.

The complete question should be:

The three finalists in a contest are brought to the center of a large, flat field. Each is given a meter stick, a compass, a calculator, a shovel, and (in a different order for each contestant) the following three displacements:

The three displacements lead to the point where the keys to a new Porsche are buried. Two contestants start measuring immediately, but the winner first calculates where to go. What does she calculate?

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The current in the RLC series circuit for t > 0 is zero, regardless of the circuit parameters and initial conditions.

To determine the current in the RLC series circuit for t > 0, we can solve the differential equation that governs the circuit using the given circuit parameters. The differential equation is derived from Kirchhoff's voltage law (KVL) and is given by:

L(di/dt) + Ri + (1/C)q = E(t)

Where:

L = Inductance (6 H)

C = Capacitance (0.04 F)

R = Resistance (210 Ω)

E(t) = Voltage source (35 V)

q = Charge on the capacitor

Since the initial current is zero (i(0) = 0) and the initial charge on the capacitor is 8 C (q(0) = 8 C), we can substitute these values into the equation. Let's solve the differential equation step by step.

Differentiating the equation with respect to time, we have:

L(d²i/dt²) + R(di/dt) + (1/C)(dq/dt) = dE(t)/dt

Since E(t) = 35 V (constant), its derivative is zero:

L(d²i/dt²) + R(di/dt) + (1/C)(dq/dt) = 0

We also know that q = CV, where V is the voltage across the capacitor. In an RLC series circuit, the voltage across the capacitor is the same as the voltage across the inductor and resistor. Therefore, V = iR, where i is the current. Substituting this into the equation:

L(d²i/dt²) + R(di/dt) + (1/C)(d(CiR)/dt) = 0

Simplifying further:

L(d²i/dt²) + R(di/dt) + iR/C = 0

This is a second-order linear homogeneous differential equation. We can solve it by assuming a solution of the form i(t) = e^(st), where s is a complex constant. Substituting this into the equation, we get:

L(s²e^(st)) + R(se^(st)) + (1/C)(e^(st))(R/C) = 0

Factoring out e^(st):

e^(st)(Ls² + Rs + R/C) = 0

For a nontrivial solution, the expression in parentheses must be equal to zero:

Ls² + Rs + R/C = 0

Now we have a quadratic equation in s. We can solve it using the quadratic formula:

s = (-R ± √(R² - 4L(R/C))) / (2L)

Plugging in the values R = 210 Ω, L = 6 H, and C = 0.04 F:

s = (-210 ± √(210² - 4(6)(210/0.04))) / (2(6))

Simplifying further:

s = (-210 ± √(44100 - 84000)) / 12

s = (-210 ± √(-39900)) / 12

Since the discriminant (√(-39900)) is negative, the roots of the quadratic equation are complex conjugates. Let's express them in terms of radicals:

s = (-210 ± i√(39900)) / 12

Simplifying further:

s = (-35 ± i√(331)) / 2

Now that we have the values of s, we can write the general solution for i(t):

i(t) = Ae^((-35 + i√(331))t/2) + Be^((-35 - i√(331))t/2)

where A and

B are constants determined by the initial conditions.

To find the specific solution for the given initial conditions, we need to solve for A and B. Since the initial current is zero (i(0) = 0), we can substitute t = 0 and set i(0) = 0:

i(0) = A + B = 0

Since the initial charge on the capacitor is 8 C (q(0) = 8 C), we can substitute t = 0 and set q(0) = C * V(0):

q(0) = CV(0) = 8 C

Since V(0) = i(0)R, we can substitute the value of i(0):

CV(0) = 0 * R = 0

Therefore, A and B must be zero. The final solution for i(t) is:

i(t) = 0

So, the current in the circuit for t > 0 is zero.

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