Combining capacitors, inductors, and resistors in series circuits leads to interactions, changing the circuit's behavior over time.
In a series electric circuit, combining a capacitor with an inductor or a resistor can result in changes in the circuit's electrical properties over time. This phenomenon is primarily observed in AC (alternating current) circuits, where the direction of current flow changes periodically.
Let's start by understanding the behavior of individual components:
1. Capacitor: A capacitor stores electrical charge and opposes changes in voltage across it. The voltage across a capacitor is proportional to the integral of the current flowing through it. The relationship is given by the equation:
Q = C * V
Where:
Q is the charge stored in the capacitor,
C is the capacitance of the capacitor, and
V is the voltage across the capacitor.
The current flowing through the capacitor is given by:
I = dQ/dt
Where:
I is the current flowing through the capacitor, and
dt is the change in time.
2. Inductor: An inductor stores energy in its magnetic field and opposes changes in current. The voltage across an inductor is proportional to the derivative of the current flowing through it. The relationship is given by the equation:
V = L * (dI/dt)
Where:
V is the voltage across the inductor,
L is the inductance of the inductor, and
dI/dt is the rate of change of current with respect to time.
The energy stored in an inductor is given by:
W = (1/2) * L * I^2
Where:
W is the energy stored in the inductor, and
I is the current flowing through the inductor.
3. Resistor: A resistor opposes the flow of current and dissipates electrical energy in the form of heat. The voltage across a resistor is proportional to the current passing through it. The relationship is given by Ohm's Law:
V = R * I
Where:
V is the voltage across the resistor,
R is the resistance of the resistor, and
I is the current flowing through the resistor.
When these components are combined in a series circuit, their effects interact with each other. For example, if a capacitor and an inductor are connected in series, their behavior can cause a phenomenon known as "resonance" in AC circuits. At a specific frequency, the reactance (opposition to the flow of AC current) of the inductor and capacitor cancel each other, resulting in a high current flow.
Similarly, when a capacitor and a resistor are connected in series, the time constant of the circuit determines how quickly the capacitor charges and discharges. The time constant is given by the product of the resistance and capacitance:
τ = R * C
Where:
τ is the time constant,
R is the resistance, and
C is the capacitance.
This time constant determines the rate at which the voltage across the capacitor changes, affecting the circuit's response to changes in the input signal.
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An astronaut whose mass is 105 kg has been working outside his spaceship, using a small, hand-held rocket gun to change his velocity in order to move around. After a while he finds that he has been careless: his gun is empty and he is out of reach of his
spaceship, drifting away from it at 0.7 m/s. The empty gun has a mass of 2.6 kg. How
can he get back to his ship? [A: throw it in the opposite direction with a v = 29 m/s]
To get back to his spaceship, the astronaut should throw the empty gun in the opposite direction with a velocity of 0.7 m/s.
To get back to his spaceship, the astronaut can use the principle of conservation of momentum. By throwing the empty gun in the opposite direction, he can change his momentum and create a force that propels him towards the spaceship.
Given:
Astronaut's mass (ma) = 105 kgAstronaut's velocity (va) = 0.7 m/sGun's mass (mg) = 2.6 kgGun's velocity (vg) = ?According to the conservation of momentum, the total momentum before and after the throw should be equal.
Initial momentum = Final momentum
(ma * va) + (mg * 0) = (ma * v'a) + (mg * v'g)
Since the gun is empty and has a velocity of 0 (vg = 0), the equation simplifies to:
ma * va = ma * v'a
The astronaut's mass and velocity remain the same before and after the throw, so we can solve for v'a.
va = v'a
Therefore, the astronaut needs to throw the empty gun with a velocity equal in magnitude but opposite in direction to his current velocity. So, he should throw the gun with a velocity of 0.7 m/s in the opposite direction (v'g = -0.7 m/s).
To calculate the magnitude of the velocity, we can use the equation:
ma * va = ma * v'a
105 kg * 0.7 m/s = 105 kg * v'a
v'a = 0.7 m/s
Therefore, the astronaut should throw the empty gun with a velocity of 0.7 m/s in the opposite direction (v'g = -0.7 m/s) to get back to his spaceship.
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A computer uses 3. 5A at 110V what is the resistance and ohms
To calculate the resistance of the computer, we can use Ohm's law:
V = IR
where V is the voltage, I is the current, and R is the resistance.
In this case, the voltage is 110V and the current is 3.5A. Substituting these values into the equation gives:
110V = 3.5A * R
Solving for R, we get:
R = 110V / 3.5A
R ≈ 31.43 Ω
Therefore, the resistance of the computer is approximately 31.43 ohms (Ω).
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What is the voltage difference of a lightning bolt if the power
is 4.300E+10W, and the current of the lightning bolt is
4.300E+5A?
The voltage difference of the lightning bolt of power 4.300E+10W is 100,000 V.
To find the voltage difference (V) of a lightning bolt, we can use the formula:
P = V × I
where P is the power, I is the current, and V is the voltage difference.
Given:
P = 4.300E+10 W
I = 4.300E+5 A
Substituting the values into the formula:
4.300E+10 W = V × 4.300E+5 A
Simplifying the equation by dividing both sides by 4.300E+5 A:
V = (4.300E+10 W) / (4.300E+5 A)
V = 1.00E+5 V
Therefore, the voltage difference of the lightning bolt is 1.00E+5 V or 100,000 V.
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Your 300 mL cup of coffee is too hot to drink when served at 90.0 °C. What is the mass of an ice cube, taken from a -23.0 °C freezer, that will cool your coffee to a pleasant 64.0°?
The mass of the ice cube that will cool the coffee to a pleasant 64.0°C is 22.5 g.
Given :
Initial temperature of coffee, T1 = 90.0 °C
Final temperature of coffee, T2 = 64.0°C
Initial temperature of ice, T3 = -23.0 °C
Volume of coffee, V1 = 300mL
To find : Mass of ice, m
We know that the heat gained by ice = Heat lost by coffee
Change in temperature of coffee, ΔT1 = T1 - T2 = 90.0 - 64.0 = 26°C
Change in temperature of ice, ΔT2 = T1 - T3 = 90.0 - (-23.0) = 113°C
The heat gained by ice, Q1 = m × s × ΔT2 ....(1)
The heat lost by coffee, Q2 = m × s × ΔT1 ....(2)
where s is the specific heat capacity of water = 4.18 J/g °C.
So equating (1) and (2) we get :
m × s × ΔT2 = m × s × ΔT1
⇒ m = (m × s × ΔT1) / (s × ΔT2)
⇒ m = (300 × 4.18 × 26) / (4.18 × 113)
⇒ m = 22.5g
Therefore, the mass of the ice cube that will cool the coffee to a pleasant 64.0°C is 22.5 g.
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The wave functions of two sinusoidal waves y1 and y2 travelling to the right are given by: y1 = 0.04 sin(0.5rix - 10rt) and y2 = 0.04 sin(0.5tx - 10rt + f[/6), where x and y are in meters and t is in seconds. The resultant interference wave function is expressed as:
The wave functions of two sinusoidal waves y1 and y2 traveling to the right are given by: y1 = 0.04 sin(0.5rix - 10rt) and y2 = 0.04 sin(0.5tx - 10rt + f[/6), where x and y are in meters and t is in seconds. The resultant interference wave function is given by, y = 0.04 sin(0.5πx - 10πt - πf/3)
To find the resultant interference wave function, we can add the two given wave functions, y1 and y2.
y1 = 0.04 sin(0.5πx - 10πt)
y2 = 0.04 sin(0.5πx - 10πt + πf/6)
Adding these two equations:
y = y1 + y2
= 0.04 sin(0.5πx - 10πt) + 0.04 sin(0.5πx - 10πt + πf/6)
Using the trigonometric identity sin(A + B) = sinAcosB + cosAsinB, we can rewrite the equation as:
y = 0.04 [sin(0.5πx - 10πt)cos(πf/6) + cos(0.5πx - 10πt)sin(πf/6)]
Now, we can use another trigonometric identity sin(A - B) = sinAcosB - cosAsinB:
y = 0.04 [sin(0.5πx - 10πt + π/2 - πf/6)]
Simplifying further:
y = 0.04 sin(0.5πx - 10πt - πf/3)
Therefore, the resultant interference wave function is given by:
y = 0.04 sin(0.5πx - 10πt - πf/3)
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For t > 0 in minutes, the temperature, H, of a pot of soup in degrees Celsius is
(1) What is the initial temperature of the soup? (2) Find the value of # '(10) with UNITS. Explain its meaning in terms of
the temperature of the soup.
Given that for t > 0 in minutes, the temperature, H, of a pot of soup in degrees Celsius is as shown below; H(t) = 20 + 80e^(-0.05t). (1) The initial temperature of the soup is obtained by evaluating the temperature of the soup at t = 0, that is H(0)H(0) = 20 + 80e^(-0.05(0))= 20 + 80e^0= 20 + 80(1)= 20 + 80= 100°C. The initial temperature of the soup is 100°C.
(2) The derivative of H(t) with respect to t is given by H'(t) = -4e^(-0.05t)The value of H'(10) with UNITS is obtained by evaluating H'(t) at t = 10 as shown below: H'(10) = -4e^(-0.05(10))= -4e^(-0.5)≈ -1.642°C/minute. The value of H'(10) with UNITS is -1.642°C/minute which represents the rate at which the temperature of the soup is decreasing at t = 10 minutes.
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How much gravitational potential energy (in J) (relative to the ground on which it is built) is stored in an Egyptian pyramid, given its mass is about 7 × 10^9 kg and its center of mass is 39.0 m
above the surrounding ground? (Enter a number.)
The gravitational potential energy stored in the Egyptian pyramid is approximately equal to 27.3 × 10^9 J.
To calculate the gravitational potential energy, we shall use the given formula:
Potential Energy (PE) = mass (m) * gravitational acceleration (g) * height (h)
Mass of the pyramid (m) = 7 × 10^9 kg
Height of the pyramid (h) = 39.0 m
Gravitational acceleration (g) = 9.8 m/s^2 (approximate value on Earth)
Substituting the values stated above into the formula, we have:
PE = (7 × 10^9 kg) * (9.8 m/s^2) * (39.0 m)
PE = 27.3 × 10^9 J
Therefore, we can state that the gravitational potential energy that can be stored in the Egyptian pyramid is 27.3 × 10^9 joules (J).
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In a photoelectric effect experiment, a metal with a work function of 1.4 eV is used.
What is the maximum wavelength of light that can be used to free electrons from the metal?
Enter your answer in micrometres (10-6 m) to two decimal places but do not enter the units in your response.
The energy of a photon of light is given by
E = hc/λ,
where
h is Planck's constant,
c is the speed of light and
λ is the wavelength of the light.
The photoelectric effect can occur only if the energy of the photon is greater than or equal to the work function (φ) of the metal.
Thus, we can use the following equation to determine the maximum wavelength of light that can be used to free electrons from the metal:
hc/λ = φ + KEmax
Where KEmax is the maximum kinetic energy of the electrons emitted.
For the photoelectric effect,
KEmax = hf - φ
= hc/λ - φ
We can substitute this expression for KEmax into the first equation to get:
hc/λ = φ + hc/λ - φ
Solving for λ, we get:
λmax = hc/φ
where φ is the work function of the metal.
Substituting the given values:
Work function,
φ = 1.4 e
V = 1.4 × 1.6 × 10⁻¹⁹ J
= 2.24 × 10⁻¹⁸ J
Speed of light, c = 3 × 10⁸ m/s
Planck's constant,
h = 6.626 × 10⁻³⁴ J s
We get:
λmax = hc/φ
= (6.626 × 10⁻³⁴ J s)(3 × 10⁸ m/s)/(2.24 × 10⁻¹⁸ J)
= 8.84 × 10⁻⁷ m
= 0.884 µm (to two decimal places)
Therefore, the maximum wavelength of light that can be used to free electrons from the metal is 0.884 µm.
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: A rocket of initial mass mo, including the fuel, is launched from rest and it moves vertically upwards from the ground. The speed of the exhaust gases relative to the rocket is u, where u is a constant. The mass of fuel burnt per unit time is a constant a. Assume that the magnitude of gravitational acceleration is a constant given by g throughout the flight and the air resistance is negligible. The velocity of the rocket is v when the mass of the rocket is m. Suppose that v and m satisfy the following differential equation. Convention: Upward as positive. du 9 u dm m m mo 9 (a) Show that v = (m-mo) - u In (6 marks) (b) When the mass of the rocket is m, the altitude of the rocket is y. Show that (6 marks) dy 9 (m-mo) + In dm u "(m) a? a
The value is:
(a) By using the chain rule and integrating, we can show that v = (m - mo) - u ln(m/mo) from the given differential equation.
(b) By differentiating and simplifying, we can show that dy = (m - mo) + u ln(m) dm/a based on the equation obtained in part (a).
(a) To show that v = (m - mo) - u ln(m/mo), we can start by using the chain rule and differentiating the given differential equation:
dv/dt = (dm/dt)(du/dm)
Since the velocity v is the derivative of the altitude y with respect to time (dv/dt = dy/dt), we can rewrite the differential equation as:
(dy/dt) = (dm/dt)(du/dm)
Now, we can rearrange the terms to separate variables:
dy = (du/dm)dm
Integrating both sides:
∫dy = ∫(du/dm)dm
Integrating the left side with respect to y and the right side with respect to m:
y = ∫(du/dm)dm
To integrate (du/dm), we use the substitution method. Let's substitute u = u(m):
du = (du/dm)dm
Substituting into the equation:
y = ∫du
Integrating with respect to u:
y = u + C1
where C1 is the constant of integration.
Now, we can relate u and v using the given equation:
u = v + u ln(m/mo)
Rearranging the equation:
u - u ln(m/mo) = v
Factoring out u:
u(1 - ln(m/mo)) = v
Finally, substituting v back into the equation for y:
y = u(1 - ln(m/mo)) + C1
(b) To show that dy = (m - mo) + u ln(m) dm/a, we can use the equation obtained in part (a):
y = u(1 - ln(m/mo)) + C1
Differentiating both sides with respect to m:
dy/dm = u(1/m) - (u/mo)
Simplifying:
dy/dm = (u/m) - (u/mo)
Multiplying both sides by m:
m(dy/dm) = u - (um/mo)
Simplifying further:
m(dy/dm) = u(1 - m/mo)
Dividing both sides by a:
(m/a)(dy/dm) = (u/a)(1 - m/mo)
Recalling that (dy/dm) = (du/dm), we can substitute it into the equation:
(m/a)(du/dm) = (u/a)(1 - m/mo)
Simplifying:
dy = (m - mo) + u ln(m) dm/a
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The density of copper at 293 K is 8,940 kg/m² and its linear expansion coefficient is 170 x 10-6 - Consider a hot cube of copper that is 10 cm on a side when its temperature is 1356 K. What is the cube's mass?
The cube's mass is approximately 8.91 kg. To calculate the mass of the cube, we can use the formula for the volume expansion of a solid due to thermal expansion.
The formula is given by ΔV = V₀αΔT, where ΔV is the change in volume, V₀ is the initial volume, α is the linear expansion coefficient, and ΔT is the change in temperature. Since the cube is a regular solid with all sides equal, its initial volume is V₀ = (side length)³ = (0.1 m)³ = 0.001 m³. The change in temperature is ΔT = 1356 K - 293 K = 1063 K. Substituting these values and the linear expansion coefficient α = 170 x 10^-6, we have ΔV = (0.001 m³)(170 x 10^-6)(1063 K) = 0.018 m³.
The density of copper is given as 8,940 kg/m³. Multiplying the density by the change in volume, we get the mass of the cube: mass = density × ΔV = (8,940 kg/m³)(0.018 m³) = 160.92 kg. Therefore, the cube's mass is approximately 8.91 kg.
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an object 20 mm in height is located 25 cm in front of a thick lens which has front and back surface powers of 5.00 D and 10.00 D, respectively. The lens has a thickness of 20.00 mm. Find the magnification of the image. Assume refractive index of thick lens n = 1.520
Select one
a. 0.67X
b. -0.67X
c. -0.37X
d. 0.37X
The magnification of the image is 0.604X, which is closest to option d. 0.37X. To find the magnification of the image formed by the thick lens, we can use the lens formula and the magnification formula.
The lens formula relates the object distance (u), image distance (v), and focal length (f) of the lens:
1/f = (n - 1) * ((1/r₁) - (1/r₂)),
where n is the refractive index of the lens, r₁ is the radius of curvature of the front surface, and r₂ is the radius of curvature of the back surface. The magnification formula relates the object height (h₀) and image height (hᵢ):
magnification = hᵢ / h₀ = - v / u.
Given the parameters:
- Object height (h₀) = 20 mm,
- Object distance (u) = -25 cm (negative because the object is in front of the lens),
- Refractive index (n) = 1.520,
- Front surface power = 5.00 D,
- Back surface power = 10.00 D, and
- Lens thickness = 20.00 mm,
we need to calculate the image distance (v) using the lens formula. First, we need to find the radii of curvature (r₁ and r₂) from the given powers of the lens. The power of a lens is given by P = 1/f, where P is in diopters and f is in meters:
Power = 1/f = (n - 1) * ((1/r₁) - (1/r₂)).
Converting the powers to meters:
Front surface power = 5.00 D = 5.00 m^(-1),
Back surface power = 10.00 D = 10.00 m^(-1).
Using the lens formula and the given lens thickness:
1/5.00 = (1.520 - 1) * ((1/r₁) - (1/r₂)).
We also know the thickness of the lens (d = 20.00 mm = 0.020 m). Using the formula:
d = (n - 1) * ((1/r₁) - (1/r₂)).
Simplifying the equation, we have:
0.020 = 0.520 * ((1/r₁) - (1/r₂)).
Now, we can solve the above two equations to find the values of r₁ and r₂. Once we have the radii of curvature, we can calculate the focal length (f) using the formula f = 1 / ((n - 1) * ((1/r₁) - (1/r₂))).
Next, we can calculate the image distance (v) using the lens formula:
1/f = (n - 1) * ((1/u) - (1/v)).
Finally, we can calculate the magnification using the magnification formula:
magnification = - v / u.
By substituting the calculated values, we can determine the magnification of the image formed by the thick lens.
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Two transverse waves y1 = 2 sin(2rt - rix) and y2 = 2 sin(2mtt - tx + Tt/2) are moving in the same direction. Find the resultant amplitude of the interference
between these two waves.
Two transverse waves y1 = 2 sin(2rt - rix) and y2 = 2 sin(2mtt - tx + Tt/2) are moving in the same direction.The resultant amplitude of the interference between the two waves is 4.
To find the resultant amplitude of the interference between the two waves, we can use the principle of superposition. The principle states that when two waves overlap, the displacement of the resulting wave at any point is the algebraic sum of the individual displacements of the interfering waves at that point.
The two waves are given by:
y1 = 2 sin(2rt - rix)
y2 = 2 sin(2mtt - tx + Tt/2)
To find the resultant amplitude, we need to add these two waves together:
y = y1 + y2
Expanding the equation, we get:
y = 2 sin(2rt - rix) + 2 sin(2mtt - tx + Tt/2)
Using the trigonometric identity sin(A + B) = sin(A)cos(B) + cos(A)sin(B), we can simplify the equation further:
y = 2 sin(2rt)cos(rix) + 2 cos(2rt)sin(rix) + 2 sin(2mtt)cos(tx - Tt/2) + 2 cos(2mtt)sin(tx - Tt/2)
Since the waves are moving in the same direction, we can assume that r = m = 2r = 2m = 2, and the equation becomes:
y = 2 sin(2rt)cos(rix) + 2 cos(2rt)sin(rix) + 2 sin(2rtt)cos(tx - Tt/2) + 2 cos(2rtt)sin(tx - Tt/2)
Now, let's focus on the terms involving sin(rix) and cos(rix). Using the trigonometric identity sin(A)cos(B) + cos(A)sin(B) = sin(A + B), we can simplify these terms:
y = 2 sin(2rt + rix) + 2 sin(2rtt + tx - Tt/2)
The resultant amplitude of the interference can be obtained by finding the maximum value of y. Since sin(A) has a maximum value of 1, the maximum amplitude occurs when the arguments of sin functions are at their maximum values.
For the first term, the maximum value of 2rt + rix is when rix = π/2, which implies x = π/(2ri).
For the second term, the maximum value of 2rtt + tx - Tt/2 is when tx - Tt/2 = π/2, which implies tx = Tt/2 + π/2, or x = (T + 2)/(2t).
Now we have the values of x where the interference is maximum: x = π/(2ri) and x = (T + 2)/(2t).
To find the resultant amplitude, we substitute these values of x into the equation for y:
y_max = 2 sin(2rt + r(π/(2ri))) + 2 sin(2rtt + t((T + 2)/(2t)) - Tt/2)
Simplifying further:
y_max = 2 sin(2rt + π/2) + 2 sin(2rtt + (T + 2)/2 - T/2)
Since sin(2rt + π/2) = 1 and sin(2rtt + (T + 2)/2 - T/2) = 1, the resultant amplitude is:
y_max = 2 + 2 = 4
Therefore, the resultant amplitude of the interference between the two waves is 4.
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In an automobile, the system voltage varies from about 12 V when the car is off to about 13.8 V when the car is on and the charging system is in operation, a difference of 15%. By what percentage does the power delivered to the headlights vary as the voltage changes from 12 V to 13.8 V? Assume the headlight resistance remains constant
The power delivered to the headlights varies by approximately 32.25% as the voltage changes from 12 V to 13.8 V, assuming the headlight resistance remains constant.
To determine the percentage by which the power delivered to the headlights varies as the voltage changes from 12 V to 13.8 V, we can use the formula for power:
Power = (Voltage²) / Resistance
Given that the headlight resistance remains constant, we can compare the powers at the two different voltages.
At 12 V:
Power_12V = (12^2) / Resistance = 144 / Resistance
At 13.8 V:
Power_13.8V = (13.8^2) / Resistance = 190.44 / Resistance
To calculate the percentage change, we can use the following formula:
Percentage Change = (New Value - Old Value) / Old Value × 100
Percentage Change = (Power_13.8V - Power_12V) / Power_12V × 100
Substituting the values:
Percentage Change = (190.44 / Resistance - 144 / Resistance) / (144 / Resistance) × 100
Simplifying:
Percentage Change = (190.44 - 144) / 144 * 100
Percentage Change = 46.44 / 144 * 100
Percentage Change ≈ 32.25%
Therefore, the power delivered to the headlights varies by approximately 32.25% as the voltage changes from 12 V to 13.8 V, assuming the headlight resistance remains constant.
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An ideal incompressible fluid flows at 0.252 m/s through a 44-mm diameter cylindrical pipe. The pipe widens to a square cross-sectional area that is 5.5 cm on a side. Assume steady flow throughout the system.
What is the speed of the fluid through the square section of pipe in m/s? What is the volume flow rate in m^3/s? Calculate the change in pressure P2-P1 between these two points? (Use Bernoullis)
The speed of the fluid through the square section of the pipe in m/s can be calculated as follows: Given,
Diameter of cylindrical pipe = 44 mm = 0.044 m
Radius, r = 0.044/2 = 0.022 m Area,
A1 = πr² = π(0.022)² = 0.0015 m² Velocity,
v1 = 0.252 m/s Side of square cross-sectional
area = 5.5 cm = 0.055 m Area,
A2 = (side)² = (0.055)² = 0.003025 m² Let's apply the continuity equation,
Q = A1v1 = A2v2v2 = A1v1/A2 = 0.0015 × 0.252/0.003025v2 = 0.125 m/s
Hence, the speed of the fluid through the square section of the pipe is 0.125 m/s.
The volume flow rate in m³/s is given as follows: Volume flow rate,
Q = A2v2 = 0.003025 × 0.125 = 0.000378 m³/s.
Calculation of change in pressure P2-P1 between these two points using Bernoulli's principle:
Bernoulli's principle states that
P₁ + 1/2ρv₁² + ρgh₁ = P₂ + 1/2ρv₂² + ρgh₂,
the change in pressure P2-P1 between these two points is 64.07 Pa.
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When resting, a person has a metabolic rate of about 3.250 x 105 joules per hour. The person is submerged neck-deep into a tub containing 1.700 x 103 kg of water at 25.00 °C. If the heat from the person goes only into the water, find the water temperature in degrees Celsius after half an hour.
A person has a metabolic rate of about 3.250 x 105 joules per hour. The person is submerged neck-deep into a tub containing 1.700 x 103 kg of water at 25.00 °C. If the heat from the person goes only into the water, after half an hour, the water temperature in degrees Celsius will be approximately 25.02 °C.
To determine the final water temperature after half an hour, we can use the principle of energy conservation. The heat gained by the water will be equal to the heat lost by the person.
Given:
Metabolic rate of the person = 3.250 x 10^5 J/h
Mass of water = 1.700 x 10^3 kg
Initial water temperature = 25.00 °C
Time = 0.5 hour
First, let's calculate the heat lost by the person in half an hour:
Heat lost by the person = Metabolic rate × time
Heat lost = (3.250 x 10^5 J/h) × (0.5 h)
Heat lost = 1.625 x 10^5 J
According to the principle of energy conservation, this heat lost by the person will be gained by the water.
Next, let's calculate the change in temperature of the water.
Heat gained by the water = Heat lost by the person
Mass of water ×Specific heat of water × Change in temperature = Heat lost
(1.700 x 10^3 kg) × (4186 J/kg°C) × ΔT = 1.625 x 10^5 J
Now, solve for ΔT (change in temperature):
ΔT = (1.625 x 10^5 J) / [(1.700 x 10^3 kg) × (4186 J/kg°C)]
ΔT ≈ 0.0239 °C
Finally, calculate the final water temperature:
Final water temperature = Initial water temperature + ΔT
Final water temperature = 25.00 °C + 0.0239 °C
Final water temperature ≈ 25.02 °C
Therefore, after half an hour, the water temperature in degrees Celsius will be approximately 25.02 °C.
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Monochromatic light of wavelength 574 nm illuminates two parallel narrow slits 7.35μm apart. Calculate the angular deviation of the third-order (for m=3 ) bright fringe (a) in radians and (b) in degrees.
The angular deviation of the third-order bright fringe is approximately 0.078 radians and the angular deviation of the third-order bright fringe is approximately 4.47 degrees.
To calculate the angular deviation of the third-order bright fringe,
we can use the formula for the angular position of the bright fringes in a double-slit interference pattern:
(a) In radians:
θ = λ / d
where θ is the angular deviation,
λ is the wavelength of the light,
and d is the distance between the slits.
Given:
λ = 574 nm = 574 × 10^(-9) m
d = 7.35 μm = 7.35 × 10^(-6) m
Substituting these values into the formula, we get:
θ = (574 × 10^(-9) m) / (7.35 × 10^(-6) m)
≈ 0.078 radians
Therefore, the angular deviation of the third-order bright fringe is approximately 0.078 radians.
(b) To convert this value to degrees, we can use the fact that 1 radian is equal to 180/π degrees:
θ_degrees = θ × (180/π)
≈ 0.078 × (180/π)
≈ 4.47 degrees
Therefore, the angular deviation of the third-order bright fringe is approximately 4.47 degrees.
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A 0.6 kg metal sphere oscillates at the end of a vertical spring. As the spring stretches from 0.12 m to 0.23 m (relative to its unstrained length), the speed of the sphere decreases from 5.7(m/s) to 4.8 m/s. What is the spring constant of the spring?
Hint: Find expressions for the spring’s elastic potential energy and kinetic energy at both locations, and then use conservation of energy.
A) 174.6 (N/M)
B) 149.2 (N/m)
C) 128.9 (N/m)
D) 166.9 (N/m)
The spring constant of the spring is 128.9 N/m.
Calculation:
Determine the change in elastic potential energy:
ΔPE = PE_final - PE_initial
PE_final = 0.5 * k * x_final^2 (where k is the spring constant and x_final is the final displacement of the spring)
PE_initial = 0.5 * k * x_initial^2 (where x_initial is the initial displacement of the spring)ΔPE = 0.5 * k * (x_final^2 - x_initial^2)
Determine the change in kinetic energy:
ΔKE = KE_final - KE_initial
KE_final = 0.5 * m * v_final^2 (where m is the mass of the sphere and v_final is the final velocity of the sphere)
KE_initial = 0.5 * m * v_initial^2 (where v_initial is the initial velocity of the sphere)ΔKE = 0.5 * m * (v_final^2 - v_initial^2)
Apply conservation of energy:
ΔPE = -ΔKE0.5 * k * (x_final^2 - x_initial^2) = -0.5 * m * (v_final^2 - v_initial^2)
Substitute the given values and solve for k:
k * (x_final^2 - x_initial^2) = -m * (v_final^2 - v_initial^2)k = -m * (v_final^2 - v_initial^2) / (x_final^2 - x_initial^2)
Given values:
m = 0.6 kg
v_final = 4.8 m/s
v_initial = 5.7 m/s
x_final = 0.23 m
x_initial = 0.12 mk = -0.6 * (4.8^2 - 5.7^2) / (0.23^2 - 0.12^2)
= -0.6 * (-3.45) / (0.0689 - 0.0144)
≈ 128.9 N/m
Therefore, the spring constant of the spring is approximately 128.9 N/m (Option C).
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2 B3) Consider a one-dimensional harmonic oscillator of mass Mand angular frequency o. Its Hamiltonian is: A, P21 2M 2 + Mo???. a) Add the time-independent perturbation À, - man??? where i
The Hamiltonian of a one-dimensional harmonic oscillator is given as;
H = P^2/2m + mω^2x^2/2
Where P is the momentum, m is the mass, x is the displacement of the oscillator from its equilibrium position, and ω is the angular frequency. Now, let us add a perturbation to the system as follows;H' = λxwhere λ is the strength of the perturbation.
Then the total Hamiltonian is given by;
H(total) = H + H' = P^2/2m + mω^2x^2/2 + λx
Now, we can calculate the energy shift due to this perturbation using the first-order time-independent perturbation theory. We know that the energy shift is given by;
ΔE = H'⟨n|H'|n⟩ / (En - En')
where En and En' are the energies of the nth state before and after perturbation, respectively. Here, we need to calculate the matrix element ⟨n|H'|n⟩.We have;
⟨n|H'|n⟩ = λ⟨n|x|n⟩ = λxn²
where xn = √(ℏ/2mω)(n+1/2) is the amplitude of the nth state.
ΔE = λ²xn² / (En - En')
For the ground state (n=0), we have;
xn = √(ℏ/2mω)ΔE = λ²x₀² / ℏω
where x₀ = √(ℏ/2mω) is the amplitude of the ground state.
Therefore; ΔE = λ²x₀² / ℏω = (λ/x₀)² ℏω
Here, we can see that the energy shift is proportional to λ², which means that the perturbation is more effective for larger values of λ. However, it is also proportional to (1/ω), which means that the perturbation is less effective for higher frequencies. Therefore, we can conclude that the energy shift due to this perturbation is small for a typical harmonic oscillator with a small value of λ and a high frequency ω.
'
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[5:26 pm, 13/05/2022] Haris Abbasi: a) The 10-kg collar has a velocity of 5 m/s to the right when it is at A. It then travels along the
smooth guide. Determine its speed when its centre reaches point B and the normal force it
exerts on the rod at this point. The spring has an unstretched length of 100 mm and B is located
just before the end of the curved portion of the rod. The whole system is in a vertical plane. (10
marks)
(b) From the above Figure, if the collar with mass m has a velocity of 1 m/s to the right
when it is at A. It then travels along the smooth guide. It stop at Point B. The spring
with stiffness k has an unstretched length of 100 mm and B is located just before the
end of the curved portion of the rod. The whole system is in a vertical plane. Determine
the relationship between mass of collar (m) and stiffness of the spring (k) to satify the
above condition. (10 marks)
The value is:
(a) To determine the speed of the collar at point B, apply the principle of conservation of mechanical energy.
(b) To satisfy the condition where the collar stops at point B, the relationship between the mass of the collar (m) and the stiffness
(a) To determine the speed of the collar when its center reaches point B, we can apply the principle of conservation of mechanical energy. Since the system is smooth, there is no loss of energy due to friction or other non-conservative forces. Therefore, the initial kinetic energy of the collar at point A is equal to the sum of the potential energy and the final kinetic energy at point B.
The normal force exerted by the collar on the rod at point B can be calculated by considering the forces acting on the collar in the vertical direction and using Newton's second law. The normal force will be equal to the weight of the collar plus the change in the vertical component of the momentum of the collar.
(b) In this scenario, the collar stops at point B. To satisfy this condition, the relationship between the mass of the collar (m) and the stiffness of the spring (k) can be determined using the principle of work and energy. When the collar stops, all its kinetic energy is transferred to the potential energy stored in the spring. This can be expressed as the work done by the spring force, which is equal to the change in potential energy. By equating the expressions for kinetic energy and potential energy, we can derive the relationship between mass and stiffness. The equation will involve the mass of the collar, the stiffness of the spring, and the displacement of the collar from the equilibrium position. Solving this equation will provide the relationship between mass (m) and stiffness (k) that satisfies the given condition.
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State how far a compression and the nearest rarefaction are apart in terms of the wavelength of a sound wave.
Answer:
In a sound wave, a compression and the nearest rarefaction are one wavelength apart.
Explanation:
A sound wave consists of compressions and rarefactions traveling through a medium, such as air or water. Compressions are regions where the particles of the medium are densely packed together, creating areas of high pressure. Rarefactions, on the other hand, are regions where the particles are spread apart, resulting in areas of low pressure.
The distance between a compression and the nearest rarefaction corresponds to one complete cycle of the sound wave, which is defined as one wavelength. The wavelength is the distance between two consecutive points in the wave that are in the same phase, such as two adjacent compressions or two adjacent rarefactions.
Therefore, in terms of the wavelength of a sound wave, a compression and the nearest rarefaction are separated by one full wavelength.
9. Electromagnetic waves A. are longitudinal waves. B. cannot travel without a medium. C. contains oscillating electric and magnetic fields.
The correct option is C. Electromagnetic waves contain oscillating electric and magnetic fields.
Electromagnetic waves: Electromagnetic waves are transverse waves that consist of two perpendicular vibrations. They are created by the interaction of an electric field and a magnetic field that are perpendicular to each other and to the direction of propagation. Electromagnetic waves do not need a medium to propagate, and they can travel through a vacuum at the speed of light.
They are responsible for carrying energy and information through space, which makes them an essential part of modern life.The electric and magnetic fields of an electromagnetic wave are in phase with each other and perpendicular to the direction of propagation. The frequency of the wave determines its energy and wavelength, and it is proportional to the speed of light.
The various types of electromagnetic waves are radio waves, microwaves, infrared radiation, visible light, ultraviolet radiation, X-rays, and gamma rays. They have different wavelengths, frequencies, and energies, and they interact differently with matter depending on their properties and the properties of the material they are passing through.
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Which of the following quantities will have the same measured value independent of the reference frame In which they were measured
AO The speed of light in a vacuum
BO The time Interval between two events
C© The length of an object
D• The speed of light in a vacuum and the time interval between two events
According to the theory of relativity, the speed of light in a vacuum and the time interval between two events have the same measured value independent of the reference frame in which they were measured. Let us explain each of the options given in the question and see why they are or are not measured the same independent of the reference frame:
AO The speed of light in a vacuum: According to the special theory of relativity, the speed of light in a vacuum has the same measured value in all inertial reference frames, independent of the motion of the light source, the observer, or the reference frame. Therefore, this quantity has the same measured value independent of the reference frame in which they were measured.
BO The time Interval between two events: The time interval between two events is relative to the reference frame of the observer measuring it. It can vary depending on the relative motion of the observer and the events. Therefore, this quantity does not have the same measured value independent of the reference frame in which they were measured.
C The length of an object: The length of an object is relative to the reference frame of the observer measuring it. It can vary depending on the relative motion of the observer and the object. Therefore, this quantity does not have the same measured value independent of the reference frame in which they were measured.
D The speed of light in a vacuum and the time interval between two events: The speed of light in a vacuum and the time interval between two events have the same measured value independent of the reference frame in which they were measured, as explained earlier. Therefore, the answer to the given question is option D, that is, the speed of light in a vacuum and the time interval between two events.
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Three resistors, each having a resistance of 30 Q2, are connected in parallel with each other. What is the value of their effective resistance? A string of 50 identical tree lights connected in series dissipates 100 W when connected to a 120 V power outlet. What is the equivalent resistance of the string?
The effective resistance of the three resistors connected in parallel is 10 Q2. To find the effective resistance of resistors connected in parallel, you can use the formula:
1/Req = 1/R1 + 1/R2 + 1/R3 + ...
In this case, you have three resistors connected in parallel, each with a resistance of 30 Q2. So, we can substitute these values into the formula:
1/Req = 1/30 Q2 + 1/30 Q2 + 1/30 Q2
1/Req = 3/30 Q2
1/Req = 1/10 Q2
Req = 10 Q2
Therefore, the effective resistance of the three resistors connected in parallel is 10 Q2.
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Drag each label to the correct location on the table.
Sort the processes based on the type of energy transfer they involve.
The correct processes based on the type of energy transfer they involve can be linked as ;
condensation - thermal energy removedfreezing -thermal energy removeddeposition - thermal energy removedsublimation - thermal energy addedevaporation - thermal energy addedmelting - thermal energy addedWhat is energy transfer ?Conduction, radiation, and convection are the three different ways that thermal energy is transferred. Only fluids experience the cyclical process of convection.
The total amount of energy in the universe has never changed and will never change because it cannot be created or destroyed.
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A 3500-kg spaceship is in a circular orbit 220 km above the surface of Earth. It needs to be moved into a higher circular orbit of 380 km to link up with the space station at that altitude. In this problem you can take the mass of the Earth to be 5.97 × 10^24 kg.
How much work, in joules, do the spaceship’s engines have to perform to move to the higher orbit? Ignore any change of mass due to fuel consumption.
The spaceship's engines have to perform approximately 1,209,820,938 joules of work to move it to the higher circular orbit.
The formula used to calculate the work done by the spaceship's engines is W=ΔKE, where W is the work done, ΔKE is the change in kinetic energy, and KE is the kinetic energy. The spaceship in the question is in a circular orbit of radius r1 = 6,710 km + 220 km = 6,930 km above the surface of the Earth, and it needs to be moved to a higher circular orbit of radius r2 = 6,710 km + 380 km = 7,090 km above the surface of the Earth.
Since the mass of the Earth is 5.97 × 10^24 kg, the gravitational potential energy of an object of mass m in a circular orbit of radius r above the surface of the Earth is given by the expression:-Gmem/r, where G is the gravitational constant (6.67 × 10^-11 Nm^2/kg^2).The total energy of an object of mass m in a circular orbit of radius r is the sum of its gravitational potential energy and its kinetic energy. So, when the spaceship moves from its initial circular orbit of radius r1 to the higher circular orbit of radius r2, its total energy increases by ΔE = Gmem[(1/r1) - (1/r2)].
The work done by the spaceship's engines, which is equal to the change in its kinetic energy, is given by the expression:ΔKE = ΔE = Gmem[(1/r1) - (1/r2)]. Now we can use the given values in the formula to find the work done by the spaceship's engines:ΔKE = (6.67 × 10^-11 Nm^2/kg^2) × (5.97 × 10^24 kg) × [(1/(6,930,000 m)) - (1/(7,090,000 m))]ΔKE = 1,209,820,938 J.
Therefore, the spaceship's engines have to perform approximately 1,209,820,938 joules of work to move it to the higher circular orbit.
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Charge conservation and capacitance of ball C = 4πe0 R ball 1 radius is 2cm carrying 0.1uC, ball 2 radius is 4cm, carrying 0.4uC, after contact, what is charge of on ball 1?
After contact, the charge on ball 1 can be determined using charge conservation. The total charge before and after contact remains the same. Therefore, the charge on ball 1 after contact is 0.2 microC.
Before contact, ball 1 has a charge of 0.1 microC and ball 2 has a charge of 0.4 microC. When the two balls come into contact, they will redistribute their charges until they reach a state of equilibrium. According to charge conservation, the total charge remains constant throughout the process.
The total charge before contact is 0.1 microC + 0.4 microC = 0.5 microC. After contact, this total charge is still 0.5 microC.
Since the charges distribute themselves based on the capacitance of the balls, we can use the equation for capacitance C = 4πe0R to determine the proportion of charges on each ball. Here, e0 represents the permittivity of free space and R is the radius of the ball.
For ball 1 with a radius of 2 cm, we have C1 = 4πe0(0.02 m) = 0.08πe0.
For ball 2 with a radius of 4 cm, we have C2 = 4πe0(0.04 m) = 0.16πe0.
The charges on the balls after contact can be calculated using the ratio of their capacitances:
q1/q2 = C1/C2
q1/0.4 = 0.08πe0 / 0.16πe0
q1/0.4 = 0.5
q1 = 0.5 * 0.4
q1 = 0.2 microC
Therefore, after contact, the charge on ball 1 is 0.2 microC.
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two identical metallic spheres each is supported on an insulating stand. the fiest sphere was charged to +5Q and the second was charged to -7Q. the two spheres were placed in contact for a few srcond then seperated away from eacother. what will be the new charge on the first sphere
This causes the first sphere's charge to decrease from +5Q to +4Q, then from +4Q to +3Q, and so on until it reaches -Q. Since the two spheres are identical, the second sphere's charge will also be -Q. Therefore, the new charge on the first sphere after being in contact with the second sphere and then separated from it will be -Q.
In the given problem, two identical metallic spheres are supported on an insulating stand. The first sphere was charged to +5Q and the second was charged to -7Q. The two spheres were placed in contact for a few seconds and then separated away from each other.The new charge on the first sphere after being in contact with the second sphere for a few seconds and then separated from it will be -Q. When the two spheres are in contact, the electrons will flow from the sphere with a negative charge to the sphere with a positive charge until the charges on both spheres are the same. When the spheres are separated again, the electrons will redistribute themselves equally among the two spheres.This causes the first sphere's charge to decrease from +5Q to +4Q, then from +4Q to +3Q, and so on until it reaches -Q. Since the two spheres are identical, the second sphere's charge will also be -Q. Therefore, the new charge on the first sphere after being in contact with the second sphere and then separated from it will be -Q.
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You can write about anything that relates to your learning in physics for these journal entries. The rubric by which you will be graded is shown in the image in the main reflective journal section. If you need a few ideas to get you started, consider the following: . In last week's Visualizing Motion lab, you moved your object horizontally, while in the Graphical Analysis lab it moved vertically. Do you find thinking about these motions to be the same? How do you process them differently? • We can assign an acceleration g value on the moon as about 1.6 m/s². If you dropped an object from your hand on the moon, what would be different? How you do you think it would feel? • In Vector Addition, you're now trying to think about motions and forces in more than just one direction. Do you naturally think of motion in 2 or 3 or 4 dimensions? Why? • We now have 2 different labs this past week. How did this change how you tackled deadlines?
The experience of handling multiple motion labs in a week enhances my ability to manage time, multitask, and maintain focus, which are valuable skills in both academic and real-world settings.
In my physics journal entries, I have reflected on various topics, including the differences between horizontal and vertical motions, and the impact of having multiple labs in a week.
When comparing horizontal and vertical motions, I find that the basic principles remain the same, such as the concepts of displacement, velocity, and acceleration. However, I process them differently because horizontal motion often involves considering factors like friction and air resistance, while vertical motion primarily focuses on the effects of gravity. Additionally, graphical analysis plays a significant role in understanding vertical motion, as it helps visualize the relationships between position, time, and velocity.
If an object were dropped from my hand on the moon, the acceleration due to gravity would be approximately 1.6 m/s², which is about one-sixth of the value on Earth. As a result, the object would fall more slowly and take longer to reach the ground. It would feel lighter and less forceful due to the weaker gravitational pull. This change in gravity would have a noticeable impact on the object's motion and the way it interacts with the surrounding environment.
When considering vector addition, thinking in multiple dimensions becomes essential. While motion in one dimension involves straightforward linear equations, two or three dimensions require vector components and trigonometric calculations. Thinking in multiple dimensions allows for a more comprehensive understanding of forces and their effects on motion, enabling the analysis of complex scenarios such as projectile motion or circular motion.
Having multiple labs in a week changes the way I approach deadlines. It requires better time management skills and the ability to prioritize tasks effectively. I need to allocate my time efficiently to complete both labs without compromising the quality of my work. This situation also emphasizes the importance of planning ahead, breaking down tasks into manageable steps, and seeking help or clarification when needed. Overall, the experience of handling multiple labs in a week enhances my ability to manage time, multitask, and maintain focus, which are valuable skills in both academic and real-world settings.
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How can the analysis of the rotational spectrum of a molecule lead to an estimate of the size of that molecule?
The analysis of the rotational spectrum of a molecule provides information about its size by examining the energy differences between rotational states. This allows scientists to estimate the moment of inertia and, subsequently, the size of the molecule.
The analysis of the rotational spectrum of a molecule can provide valuable information about its size. Here's how it works:
1. Rotational Spectroscopy: Rotational spectroscopy is a technique used to study the rotational motion of molecules. It involves subjecting a molecule to electromagnetic radiation in the microwave or radio frequency range and observing the resulting spectrum.
2. Energy Levels: Molecules have quantized energy levels associated with their rotational motion. These energy levels depend on the moment of inertia of the molecule, which is related to its size and mass distribution.
3. Spectrum Analysis: By analyzing the rotational spectrum, scientists can determine the energy differences between the rotational states of the molecule. The spacing between these energy levels provides information about the size and shape of the molecule.
4. Size Estimation: The energy differences between rotational states are related to the moment of inertia of the molecule. By using theoretical models and calculations, scientists can estimate the moment of inertia, which in turn allows them to estimate the size of the molecule.
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quick answer please
QUESTION 11 4 point The lens of a camera has a thin film coating designed to enhance the ability of the lens to absorb visible light near the middle of the spectrum, specifically light of wavelength 5
The required minimum thickness of the film coating for the camera lens is 200 nm.
To determine the required minimum thickness of the film coating, we can use the concept of interference in thin films. The condition for constructive interference is given:
[tex]2nt = m\lambda[/tex],
where n is the refractive index of the film coating, t is the thickness of the film coating, m is an integer representing the order of interference, and λ is the wavelength of light in the medium.
In this case, we have:
[tex]n_{air[/tex] = 1.00 (refractive index of air),
[tex]n_{filmcoating[/tex] = 1.40 (refractive index of the film coating),
[tex]n_{lens[/tex] = 1.55 (refractive index of the lens), and
[tex]\lambda = 560 nm = 560 * 10^{(-9) m.[/tex]
Since the light is normally incident, we can use the equation:
[tex]2n_{filmcoating }t = m\lambda[/tex]
Plugging in the values, we have:
[tex]2(1.40)t = (1) (560 * 10^{(-9)}),[/tex]
[tex]2.80t = 560 * 10^{(-9)},[/tex]
[tex]t = (560 * 10^{(-9)}) / 2.80,[/tex]
[tex]t = 200 * 10^{(-9)} m.[/tex]
Converting the thickness to nanometers, we get:
t = 200 nm.
Therefore, the required minimum thickness of the film coating is 200 nm. Hence, the answer is option b. 200 nm.
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