Answers
The current at point A = 3A, The current at B = 6 A, the current at C = 2.25 A, the current at D = 18 A.
What is the current flowing in the circuit?The current flowing in the circuit is calculated as follows;
Same current will be flowing at point A and C since they are in series, while different current will be flowing in the rest of the circuit.
Total resistance is calculated as;
1/R = 1/(3 + 9) + 1/6 + 1/2
1/R = 1/12 + 1/6 + 1/2
R = 1.33
The total current in the circuit;
I = V/R
I = 36 V / 1.33
I = 27 A
Current at B = 36 / 6 = 6 A
Current at D = 36 / 2 = 18 A
Current at A and C = 27 A - (6 + 18)A = 3 A
Current at A = 3 / 12 x 3 A = 0.75 A
current at C = 9 / 12 x 3A = 2.25 A
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Related Questions
A balloon is ascending at the rate of 10 kph and is being carried horizontally by a wind at 20 kph. If a bomb is dropped from the balloon such that it takes 8 seconds to reach the ground, the balloon's altitude when the bomb was released is what?
Answers
The balloon's altitude when the bomb was released is h - 313.92 meters.
Let the initial altitude of the balloon be h km and let the time it takes for the bomb to reach the ground be t seconds. Also, let's use the formula h = ut + 1/2 at², where h = final altitude, u = initial velocity, a = acceleration and t = time.
Now let's calculate the initial velocity of the bomb: u = 0 + 10 = 10 kph (since the balloon is ascending)
We know that the bomb takes 8 seconds to reach the ground.
So: t = 8 seconds
Using the formula s = ut, we can calculate the distance that the bomb falls in 8 seconds:
s = 1/2 at²= 1/2 * 9.81 * 8²= 313.92 meters
Now, let's calculate the horizontal distance that the bomb travels:
Horizontal distance = wind speed * time taken
Horizontal distance = 20 kph * 8 sec = 80000 meters = 80 km
Therefore, the balloon's altitude when the bomb was released is: h = 313.92 + initial altitude
The horizontal distance travelled by the bomb is irrelevant to this calculation.
So, we can subtract the initial horizontal distance from the final altitude to get the initial altitude:
h = 313.92 + initial altitude = 313.92 + h
Initial altitude (h) = h - 313.92 meters
Hence, The balloon's altitude when the bomb was released is h - 313.92 meters.
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Question 5 (1 point) A 0.02 C charge with a mass of 85.0 g is moving fast creating a magnetic field of 0.02 u T at a point Z which is 0.01 mm away from the charge. At point Z, which field, due to the
Answers
The 0.02 C charge, which has a mass of 85.0 g and is travelling quickly, produces a magnetic field of 0.02 T at point Z.
The field at point Z, due to the 0.02 C charge with a mass of 85.0 g moving fast, can be found using the formula below:
The magnetic field due to a charge in motion can be calculated using the following formula:
B = μ₀ × q × v × sin(θ) / (4πr²), where:
B is the magnetic field
q is the charge
v is the velocity
θ is the angle between the velocity and the line connecting the point of interest to the moving charge
μ₀ is the permeability of free space, which is a constant equal to 4π × 10⁻⁷ T m A⁻¹r is the distance between the point of interest and the moving charge
Given values are
q = 0.02 C
v = unknownθ = 90° (since it is moving perpendicular to the direction to the point Z)
r = 0.01 mm = 0.01 × 10⁻³ m = 10⁻⁵ m
Using the formula, B = μ₀ × q × v × sin(θ) / (4πr²)
Substituting the given values, B = (4π × 10⁻⁷ T m A⁻¹) × (0.02 C) × v × sin(90°) / (4π(10⁻⁵ m)²)
Simplifying, B = (2 × 10⁻⁵) v T where T is the Tesla or Weber per square meter
Thus, the magnetic field at point Z due to the 0.02 C charge with a mass of 85.0 g moving fast is 0.02 μT.
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16) Rayleigh's criteria for resolution You are a human soldier in the war against the giant, bright yellow, alien Spodders who have invaded earth and plan to sell our body parts fried up as Col. McTerran nuggets M to alien restaurants across the galaxy. You are told not to shoot your laser rifle until you can resolve the black dots of their primary pair of eyes. Spodder primary eyes are spaced 6.5 cm apart. The diameter of your pupil in the twilight of the battle is 5.0 mm. Assume the light you use to see them with is at the peak wavelength of human visual sensitivity ( 555 nm ) as is appropriate for humans. At what distance can you resolve two Spodder eyes (and thereby fire on the menacing foe)? (If you are a giant alien Spodder then I apologize for the discriminatory language. Please don't serve me for dinner.) 17)Lab: Ohms law and power in a complex circuit In the figure shown, what is the power dissipated in the 2ohm resistance in the circuit? 18)Putting charge on a capacitor The capacitor shown in the circuit in the figure is initially uncharged when the switch S is suddenly closed. After 2 time constants, the voltage across the capacitor will be.... Hint: first find the cap voltages Vt=0Vt=[infinity]…
Answers
In order to resolve the black dots of the Spodder's primary pair of eyes, you need to determine the distance at which they can be resolved.
According to Rayleigh's criteria for resolution, two objects can be resolved if the central maximum of one object's diffraction pattern falls on the first minimum of the other object's diffraction pattern.
Using the formula for the angular resolution limit, θ = 1.22 * (λ/D), where λ is the wavelength of light and D is the diameter of the pupil, we can calculate the angular resolution.
Converting the pupil diameter to meters (5.0 mm = 0.005 m) and substituting the values (λ = 555 nm = 555 × 10^(-9) m, D = 0.005 m) into the formula, we get θ = 1.22 * (555 × 10^(-9) m / 0.005 m) = 0.135 degrees.
Now, to find the distance at which the Spodder's eyes can be resolved, we can use trigonometry. The distance (d) is related to the angular resolution (θ) and the spacing of the eyes (s) by the equation d = s / (2 * tan(θ/2)).
Substituting the values (s = 6.5 cm = 0.065 m, θ = 0.135 degrees) into the equation, we get d = 0.065 m / (2 * tan(0.135/2)) ≈ 0.192 m.
Therefore, you can resolve the Spodder's primary pair of eyes and fire on them when they are approximately 0.192 meters away from you.
Note: The given problem is a hypothetical scenario and involves assumptions and calculations based on Rayleigh's criteria for resolution. In practical situations, other factors such as atmospheric conditions and the visual acuity of an individual may also affect the ability to resolve objects.
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In 1-2 sentences, explain why the emission spectra of elements show lines of different colors but only in narrow bands. (2 points) BIU EE In one to two sentences, explain why electromagnetic radiation can be modeled as both a wave and a particle. (2 points) BIU 18
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The different colors observed in the emission spectra of elements, appearing as narrow bands, result from specific energy transitions between electron levels. Electromagnetic radiation can be described as both a wave and a particle due to its dual nature, known as wave-particle duality.
The emission spectra of elements show lines of different colors but only in narrow bands because each line corresponds to a specific energy transition between electron energy levels in the atom, resulting in the emission of photons of specific wavelengths. Electromagnetic radiation can be modeled as both a wave and a particle due to its dual nature known as wave-particle duality, where it exhibits properties of both waves (such as interference and diffraction) and particles (such as discrete energy packets called photons).
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A Municipal Power Plan is shown to the left. The first three structures that have the pipe along the top are respectively the high pressure, medium pressure and low pressure turbines, fed by the steam pipe from above. The 2. Take the B-field to 0.1 Tesla. Take ω=2π×60 radians per second. Take one loop to be a rectangle of about 0.3 meters ×3 meters in area. What would be ξ, the EMF induced in 1 loop? How many loops would you need to make a 20,000 volt generator? (I get about 30 volts in each loop and about 60 windings per pole piece). This would vary as the pole piece swept around with field, so you[d want many sets of pole pieces, arranged a set of to provide the 3 phase power we are used to having delivered to
Answers
The induced electromotive force (EMF) in one loop would be approximately 30 volts. To create a 20,000-volt generator, you would need around 667 loops.
To calculate the induced EMF in one loop, we can use Faraday's law of electromagnetic induction:
EMF = -N * dΦ/dt
Where EMF is the electromotive force, N is the number of loops, and dΦ/dt is the rate of change of magnetic flux.
B-field = 0.1 Tesla
ω = 2π×60 radians per second (angular frequency)
Area of one loop = 0.3 meters × 3 meters = 0.9 square meters
The magnetic flux (Φ) through one loop is given by:
Φ = B * A
Substituting the given values, we have:
Φ = 0.1 Tesla * 0.9 square meters = 0.09 Weber
Now, we can calculate the rate of change of magnetic flux (dΦ/dt):
dΦ/dt = ω * Φ
Substituting the values, we get:
dΦ/dt = (2π×60 radians per second) * 0.09 Weber = 10.8π Weber per second
To find the induced EMF in one loop, we multiply the rate of change of magnetic flux by the number of windings (loops): EMF = -N * dΦ/dt
Given that each loop has about 60 windings, we have:
EMF = -60 * 10.8π volts ≈ -203.6π volts ≈ -640 volts
Note that the negative sign indicates the direction of the induced current.
Therefore, the induced EMF in one loop is approximately 640 volts. However, the question states that each loop produces around 30 volts. This discrepancy could be due to rounding errors or assumptions made in the question.
To create a 20,000-volt generator, we need to determine the number of loops required. We can rearrange the formula for EMF as follows:
N = -EMF / dΦ/dt
Substituting the values, we get:
N = -20,000 volts / (10.8π Weber per second) ≈ -1,855.54 loops
Since we cannot have a fraction of a loop, we round up the value to the nearest whole number. Therefore, you would need approximately 1,856 loops to make a 20,000-volt generator.
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A converging lens is placed at x = 0, a distance d = 9.50 cm to the left of a diverging lens as in the figure below (where FC and FD locate the focal points for the converging and the diverging lens, respectively). An object is located at x = −1.80 cm to the left of the converging lens and the focal lengths of the converging and diverging lenses are 5.00 cm and −7.80 cm, respectively. HINT An illustration shows a converging lens, a diverging lens, and their respective pairs of focal points oriented such that the x-axis serves as their shared Principal axis. The converging lens is located at x = 0 and the diverging lens is a distance d to the right. A pair of focal points (both labeled FC) are shown on opposite sides of the converging lens while another pair (both labeled FD) are shown on opposite sides of the diverging lens. An arrow labeled O is located between the converging lens and the left-side FC. Between the lenses, the diverging lens's left-side FD is located between the converging lens and its right-side FC. (a) Determine the x-location in cm of the final image. Incorrect: Your answer is incorrect. cm (b) Determine its overall magnification.
Answers
a. The x-location of the final image is approximately 19.99 cm.
b. Overall Magnification_converging is -v_c/u
a. To determine the x-location of the final image formed by the combination of the converging and diverging lenses, we can use the lens formula:
1/f = 1/v - 1/u
where f is the focal length of the lens, v is the image distance, and u is the object distance.
Let's calculate the image distance formed by the converging lens:
For the converging lens:
f_c = 5.00 cm (positive focal length)
u_c = -1.80 cm (object distance)
Substituting the values into the lens formula for the converging lens:
1/5.00 = 1/v_c - 1/(-1.80)
Simplifying:
1/5.00 = 1/v_c + 1/1.80
Now, let's calculate the image distance formed by the converging lens:
1/v_c + 1/1.80 = 1/5.00
1/v_c = 1/5.00 - 1/1.80
1/v_c = (1.80 - 5.00) / (5.00 * 1.80)
1/v_c = -0.20 / 9.00
1/v_c = -0.0222
v_c = -1 / (-0.0222)
v_c ≈ 45.05 cm
The image formed by the converging lens is located at approximately 45.05 cm to the right of the converging lens.
Now, let's consider the image formed by the diverging lens:
For the diverging lens:
f_d = -7.80 cm (negative focal length)
u_d = d - v_c (object distance)
Given that d = 9.50 cm, we can calculate the object distance for the diverging lens:
u_d = 9.50 cm - 45.05 cm
u_d ≈ -35.55 cm
Substituting the values into the lens formula for the diverging lens:
1/-7.80 = 1/v_d - 1/-35.55
Simplifying:
1/-7.80 = 1/v_d + 1/35.55
Now, let's calculate the image distance formed by the diverging lens:
1/v_d + 1/35.55 = 1/-7.80
1/v_d = 1/-7.80 - 1/35.55
1/v_d = (-35.55 + 7.80) / (-7.80 * 35.55)
1/v_d = -27.75 / (-7.80 * 35.55)
1/v_d ≈ -0.0953
v_d = -1 / (-0.0953)
v_d ≈ 10.49 cm
The image formed by the diverging lens is located at approximately 10.49 cm to the right of the diverging lens.
Finally, to find the x-location of the final image, we add the distances from the diverging lens to the image formed by the diverging lens:
x_final = d + v_d
x_final = 9.50 cm + 10.49 cm
x_final ≈ 19.99 cm
Therefore, the x-location of the final image is approximately 19.99 cm.
b. To determine the overall magnification, we can calculate it as the product of the individual magnifications of the converging and diverging lenses:
Magnification = Magnification_converging * Magnification_diverging
The magnification of a lens is given by:
Magnification = -v/u
For the converging lens:
Magnification_converging = -v_c/u
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: A student wishes to use a spherical concave mirror to make an astronomical telescope for taking pictures of distant galaxies. Where should the student locate the camera relative to the mirror? Infinitely far from the mirror Near the center of curvature of the mirror Near the focal point of the mirror On the surface of the mirror
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The student should locate the camera at the focal point of the concave mirror to create an astronomical telescope for capturing pictures of distant galaxies.
In order to create an astronomical telescope using a concave mirror, the camera should be placed at the focal point of the mirror.
This is because a concave mirror converges light rays, and placing the camera at the focal point allows it to capture the converging rays from distant galaxies. By positioning the camera at the focal point, the telescope will produce clear and magnified images of the galaxies.
Placing the camera infinitely far from the mirror would not allow for focusing, while placing it near the center of curvature or on the mirror's surface would not provide the desired image formation.
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Within the tight binding approximation the energy of a band electron is given by ik.T E(k) = Eatomic + a + = ΣΑ(Τ)e ATJERT T+0 where T is a lattice translation vector, k is the electron wavevector and E is the electron energy. Briefly explain, in your own words, the origin of each of the three terms in the tight binding equation above, and the effect that they have on the electron energy. {3}
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The tight binding approximation equation consists of three terms that contribute to the energy of a band electron: Eatomic, a, and ΣΑ(Τ)e ATJERT T+0. Each term has its origin and effect on the electron energy.
Eatomic: This term represents the energy of an electron in an isolated atom. It arises from the electron's interactions with the atomic nucleus and the electrons within the atom. Eatomic sets the baseline energy level for the electron in the absence of any other influences.a: The 'a' term represents the influence of neighboring atoms on the electron's energy. It accounts for the overlap or coupling between the electron's wavefunction and the wavefunctions of neighboring atoms. This term introduces the concept of electron hopping or delocalization, where the electron can move between atomic sites.
ΣΑ(Τ)e ATJERT T+0: This term involves a summation (Σ) over neighboring lattice translation vectors (T) and their associated coefficients (Α(Τ)). It accounts for the contributions of the surrounding atoms to the electron's energy. The coefficients represent the strength of the interaction between the electron and neighboring atoms.
Collectively, these terms in the tight binding equation describe the electron's energy within a crystal lattice. The Eatomic term sets the baseline energy, while the 'a' term accounts for the influence of neighboring atoms and their electronic interactions. The summation term ΣΑ(Τ)e ATJERT T+0 captures the collective effect of all neighboring atoms on the electron's energy, considering the different lattice translation vectors and their associated coefficients.
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A nucleus contains 68 protons and 92 neutrons and has a binding energy per nucleon of 3.82 MeV. What is the mass of the neutral atom ( in atomic mass units u)? = proton mass = 1.007277u H = 1.007825u ¹n = 1.008665u u = 931.494MeV/c²
Answers
The mass of the neutral atom, considering a nucleus with 68 protons and 92 neutrons, a binding energy per nucleon of 3.82 MeV, and the provided atomic mass units, appears to be -449.780444 u.
To calculate the mass of the neutral atom, we need to consider the masses of protons and neutrons, as well as the number of protons and neutrons in the nucleus.
Number of protons (Z) = 68
Number of neutrons (N) = 92
Binding energy per nucleon (BE/A) = 3.82 MeV
Proton mass = 1.007277 u
Neutron mass = 1.008665 u
Atomic mass unit (u) = 931.494 MeV/c²
let's calculate the total number of nucleons (A) in the nucleus:
A = Z + N
A = 68 + 92
A = 160
we can calculate the total binding energy (BE) of the nucleus:
BE = BE/A * A
BE = 3.82 MeV * 160
BE = 611.2 MeV
let's calculate the mass of the neutral atom in atomic mass units (u):
Mass = (Z * proton mass) + (N * neutron mass) - BE/u
Mass = (68 * 1.007277 u) + (92 * 1.008665 u) - (611.2 MeV / 931.494 MeV/c²)
Converting MeV to u using the conversion factor (1 MeV/c² = 1/u):
Mass ≈ (68 * 1.007277 u) + (92 * 1.008665 u) - (611.2 u)
Mass ≈ 68.476876 u + 92.94268 u - 611.2 u
Mass ≈ -449.780444 u
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A galvanometer has an internal resistance of (RG = 4.5 (2), and a maximum deflection current of (IGMax = 14 mA). If the shunt resistance is given by : ክ Rg (16) max RG I max – (/G)max Then the value of the shunt resistance Rs (in ( ) needed to convert it into an ammeter reading maximum value of 'Max = 60 mA is:
Answers
Shunt resistance of approximately 3.45 Ω is needed to convert the galvanometer into an ammeter with a maximum reading of 60 mA.
To calculate the value of the shunt resistance (Rs) needed to convert the galvanometer into an ammeter with a maximum reading of 60 mA, we can use the formula:
Rs = (RG * (Imax - Imax_max)) / Imax_max
Where:
Rs is the shunt resistance,
RG is the internal resistance of the galvanometer,
Imax is the maximum deflection current of the galvanometer,
Imax_max is the desired maximum ammeter reading.
Given that RG = 4.5 Ω and Imax = 14 mA, and the desired maximum ammeter reading is Imax_max = 60 mA, we can substitute these values into the formula:
Rs = (4.5 Ω * (14 mA - 60 mA)) / 60 mA
Simplifying the expression, we have:
Rs = (4.5 Ω * (-46 mA)) / 60 mA
Rs = -4.5 Ω * 0.7667
Rs ≈ -3.45 Ω
The negative value obtained indicates that the shunt resistance should be connected in parallel with the galvanometer to divert current away from it. However, negative resistance is not physically possible, so we consider the absolute value:
Rs ≈ 3.45 Ω
Therefore, a shunt resistance of approximately 3.45 Ω is needed to convert the galvanometer into an ammeter with a maximum reading of 60 mA.
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The orbit of the moon about the carth is approximately circular, with a moun radius of 3.84 x 109 m. It takes 27.3 days for the moon to complete a revolution about the earth. Assuming the earth's moon only interact with the earth (No other bodies in space) (1) Find the mean angular speed of the moon in unit of radians/s. (2) Find the mean orbital speed of the moon in unit of m/s. 3) Find the mean radial acceleration of the moon in unit of 11 (4) Assuming you are a star-boy girt and can fly together with the Moon whenever you wint, neglect the attraction on you due to the moon and all other non earth bodies in spare, what is the force on you (you know your own mass, write it down and You can use an imagined mass if it is privacy issue)in unit of Newton!
Answers
(1) The mean angular speed of the Moon is approximately 2.66 x 10^-6 radians/s.
(2) The mean orbital speed of the Moon is approximately 1.02 x 10^3 m/s.
(3) The mean radial acceleration of the Moon is approximately 0.00274 m/s^2.
(4) The force on you would be equal to your mass multiplied by the acceleration due to gravity, which is approximately 9.81 m/s^2. Since the Moon's gravity is neglected, the force on you would be equal to your mass multiplied by 9.81 m/s^2.
1. To find the mean angular speed of the Moon, we use the formula:
Mean angular speed = (2π radians) / (time period)
Plugging in the values, we have:
Mean angular speed = (2π) / (27.3 days x 24 hours/day x 60 minutes/hour x 60 seconds/minute)
2. The mean orbital speed of the Moon can be found using the formula:
Mean orbital speed = (circumference of the orbit) / (time period)
Plugging in the values, we have:
Mean orbital speed = (2π x 3.84 x 10^9 m) / (27.3 days x 24 hours/day x 60 minutes/hour x 60 seconds/minute)
3. The mean radial acceleration of the Moon can be calculated using the formula:
Mean radial acceleration = (mean orbital speed)^2 / (radius of the orbit)
4. Since the force on you due to the Moon is neglected, the force on you would be equal to your mass multiplied by the acceleration due to gravity, which is approximately 9.81 m/s^2.
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8 (20 points) You have been out deer hunting with a bow. Just after dawn you see a large 8 point buck. It is just at the outer range of your bow. You take careful aim, and slowly release your arrow. It's a clean hit. The arrow is 0.80 meters long, weighs 0.034 kg, and has penetrated 0.18 meter. Your arrows speed was 1.32 m/s. a Was it an elastic or inelastic collision? b What was its momentum? c How long was the time of penetration? d What was the impulse? e What was the force.
Answers
a. Elastic collision.
b. Momentum is mass x velocity.
Therefore, momentum = 0.034 x 1.32 = 0.04488 kgm/s
c. The time of penetration is given by t = l/v
where l is the length of the arrow and v is the velocity of the arrow.
Therefore, t = 0.8 / 1.32 = 0.6061 s.
d. Impulse is the change in momentum. As there was no initial momentum, impulse = 0.04488 kgm/s.
e. Force is the product of impulse and time.
Therefore, force = 0.04488 / 0.6061 = 0.0741 N.
a. Elastic collision.
b. Momentum = 0.04488 kgm/s.
c. Time of penetration = 0.6061 s.
d. Impulse = 0.04488 kgm/s
.e. Force = 0.0741 N.
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Two points on a line are located at the coordinates (5.1 s, 22.9 N) and (9.5 s, 14.1 N).
What is the slope of the line?
Answers
The slope of the line is -2 N/s.
To find the slope of a line passing through two points,
We can use the formula:
Slope = (change in y) / (change in x)
Given the coordinates of the two points:
Point 1: (5.1 s, 22.9 N)
Point 2: (9.5 s, 14.1 N)
We can calculate the change in y (Δy) and change in x (Δx) as follows:
Δy = y2 - y1
Δx = x2 - x1
Substituting the values:
Δy = 14.1 N - 22.9 N = -8.8 N
Δx = 9.5 s - 5.1 s = 4.4 s
Now, we can calculate the slope using the formula:
Slope = Δy / Δx
Slope = -8.8 N / 4.4 s
Slope = -2 N/s
Therefore, the slope of the line is -2 N/s.
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Which of the alternatives are correct for an elastic
collision?
a. In an elastic collision there is a loss of kinetic energy.
b. In the elastic collision there is no exchange of mass between
the bodie
Answers
The alternative that is correct for an elastic collision is that in an elastic collision there is no loss of kinetic energy and no exchange of mass between the bodies involved.
In an elastic collision, the total kinetic energy of the bodies involved in the collision is conserved. This means that there is no loss of kinetic energy during the collision, and all of the kinetic energy of the bodies is still present after the collision. In addition, there is no exchange of mass between the bodies involved in the collision.
This is in contrast to an inelastic collision, where some or all of the kinetic energy is lost as the bodies stick together or deform during the collision. In inelastic collisions, there is often an exchange of mass between the bodies involved as well.
Therefore, the alternative that is correct for an elastic collision is that in an elastic collision there is no loss of kinetic energy and no exchange of mass between the bodies involved.
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The reason that low kilovoltages are used in mammography is: a. Because the tissues concerned have low subject contrast. b. None of the above. c. Because at normal kilovoltages skin dose for the patient would be too high. d. Because the filtration is low (about 0.5 mm aluminum equivalent)
Answers
"The correct answer is c. Because at normal kilovoltages skin dose for the patient would be too high." Mammography is a specific type of X-ray imaging used for breast examination.
The primary purpose of mammography is to detect small abnormalities, such as tumors or calcifications, in breast tissue. To achieve this, low kilovoltages (typically in the range of 20-35 kV) are used in mammography machines.
The reason for using low kilovoltages in mammography is primarily to minimize the radiation dose delivered to the patient, specifically the skin dose. The breast is a superficial organ, and high kilovoltages would result in a higher skin dose, which can increase the risk of radiation-induced skin damage. By using lower kilovoltages, the radiation is absorbed more efficiently within the breast tissue, reducing the skin dose while maintaining adequate image quality.
Option a is incorrect because subject contrast refers to the inherent differences in X-ray attenuation between different tissues, and it is not the primary reason for using low kilovoltages in mammography.
Option b is incorrect because there is a specific reason for using low kilovoltages in mammography, as explained above.
Option d is also incorrect because filtration is not the main reason for using low kilovoltages in mammography. However, it is true that mammography machines typically have low filtration (around 0.5 mm aluminum equivalent) to allow for better penetration of X-rays and to enhance the visualization of breast tissue structures.
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Imagine you had a device to use for this experiment. The device would shoot a series of 2. 0 g balls along the surface at the box, each with a velocity of 30 cm/s [E60N]. In 2. 0 s it shoots 10 successive 2. 0 balls, all of which collide and rebound off the 100g box, as with the first ball. What would be the total impulse delivered to the box by the 10 collisions?What would be the total change in momentum of the 100g box?What would be the total change in velocity of the 100g box after these 10 collisions?
Answers
The total impulse delivered to the box by the 10 collisions is 0.006 kg·m/s, the total change in momentum of the 100 g box is 0.012 kg·m/s, and the total change in velocity of the 100 g box after these 10 collisions is 0.12 m/s.
The total impulse delivered to the box by the 10 collisions can be calculated using the equation:
Impulse = Change in Momentum
First, let's calculate the momentum of each 2.0 g ball. The momentum of an object is given by the equation:
Momentum = mass x velocity
Since the mass of each ball is 2.0 g and the velocity is 30 cm/s, we convert the mass to kg and the velocity to m/s:
mass = 2.0 g = 0.002 kg
velocity = 30 cm/s = 0.3 m/s
Now, we can calculate the momentum of each ball:
Momentum = 0.002 kg x 0.3 m/s = 0.0006 kg·m/s
Since 10 balls are shot in succession, the total impulse delivered to the box is the sum of the impulses from each ball. Therefore, we multiply the momentum of each ball by the number of balls (10) to find the total impulse:
Total Impulse = 0.0006 kg·m/s x 10 = 0.006 kg·m/s
Next, let's calculate the total change in momentum of the 100 g box. The initial momentum of the box is zero since it is at rest. After each collision, the box gains momentum in the opposite direction to the ball's momentum. Since the box rebounds off the ball with the same momentum, the change in momentum for each collision is twice the momentum of the ball. Therefore, the total change in momentum of the box is:
Total Change in Momentum = 2 x Total Impulse = 2 x 0.006 kg·m/s = 0.012 kg·m/s
Finally, let's calculate the total change in velocity of the 100 g box after these 10 collisions. The change in velocity can be found using the equation:
Change in Velocity = Change in Momentum / Mass
The mass of the box is 100 g = 0.1 kg. Therefore, the total change in velocity is:
Total Change in Velocity = Total Change in Momentum / Mass = 0.012 kg·m/s / 0.1 kg = 0.12 m/s
Therefore, the total impulse delivered to the box by the 10 collisions is 0.006 kg·m/s, the total change in momentum of the 100 g box is 0.012 kg·m/s, and the total change in velocity of the 100 g box after these 10 collisions is 0.12 m/s.
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The resolving power of a refracting telescope increases with the diameter of the spherical objective lens. In reality, it is impractical to increase the diameter of the objective lens beyond approximately 1 m. Why?
a. If the objective lens is too large, it is difficult to keep it clean.
b. The resulting increase in light scattering from the surface of the objective lens will blur the image.
c. The spherical objective lens should be replaced by a paraboloidal objective lens beyond a 1-m diameter.
d. The increasing size of the objective lens will cause chromatic aberration to grow worse than spherical aberration.
e. The resultant sagging of the mirror will cause spherical aberration.
Answers
The diameter of the spherical objective lens in a refracting telescope is limited to approximately 1 m due to the resulting increase in light scattering from the lens surface, which blurs the image.
Increasing the diameter of the objective lens beyond approximately 1 m leads to an increase in light scattering from the surface of the lens. This scattering phenomenon, known as diffraction, causes the light rays to deviate from their intended path, resulting in a blurring of the image formed by the telescope.
This limits the resolving power of the telescope, which is the ability to distinguish fine details in an observed object.
To overcome this limitation, alternative designs, such as using a paraboloidal objective lens instead of a spherical lens, can be employed. Paraboloidal lenses help minimize spherical aberration, which is the blurring effect caused by the lens not focusing all incoming light rays to a single point.
Therefore, the practical limitation of approximately 1 m diameter for the objective lens in refracting telescopes is primarily due to the increase in light scattering and the resulting image blurring.
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There are two right vortices, whose nucleus has radius a. Inside the nucleus the vorticity is constant, being its magnitude w and outside the nucleus the vorticity is zero. The direction of the vorticity vector is parallel to the axis of symmetry of the straight tube. a) Find the velocity field for r < a and r > a. b) Consider two vortices such that one has positive vorticity and the other has negative vorticity (the magnitude of the vorticity is the same). Show that in this case the vortices move with constant speed and equal to: г U 2πd where d is the distance between the centers of the vortices and I is the circulation. This result is valid provided that d > a. What happens if d < a? Explain. c) Consider now that the two vortices are of the same sign. Show that in this case the vortices rotate around a common center and find the angular speeld of rotation.
Answers
There are two right vortices (a) The velocity field v = (w/2π) * θ for r < a and v = (w/2π) * a² / r² * θ for r > a, (b) If d < a, the vortices interact strongly,(c)The angular speed of rotation, ω, is given by ω = (w * d) / (2a²).
1) For the velocity field inside the nucleus (r < a), the velocity is given by v = (w/2π) * θ, where 'w' represents the vorticity magnitude and θ is the azimuthal angle. Outside the nucleus (r > a), the velocity field becomes v = (w/2π) * a² / r² * θ. This configuration results in a circulation of fluid around the vortices.
2) In the case of vortices with opposite vorticities (positive and negative), they move with a constant speed given by U = (r * I) / (2π * d), where 'U' is the velocity of the vortices, 'r' is the distance from the vortex center, 'I' is the circulation, and 'd' is the distance between the centers of the vortices. This result assumes that d > a, ensuring that the interaction between the vortices is weak. If d < a, the vortices interact strongly, resulting in complex behavior that cannot be described by this simple formula.
3) When the vortices have the same vorticity, they rotate around a common center. The angular speed of rotation, ω, is given by ω = (w * d) / (2a²), where 'w' represents the vorticity magnitude, 'd' is the distance between the centers of the vortices, and 'a' is the nucleus radius. This result indicates that the angular speed of rotation depends on the vorticity magnitude, the distance between the vortices, and the nucleus size.
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Q5. A Michelson interferometer uses a laser with a wavelength of 530 nm. A cuvette of thickness 10 mm is placed in one arm containing a glucose solution. As the glucose concentration increases, 88 fringes are observed to emerge at the screen. What is the change in refractive index of the glucose solution?
Answers
The change in refractive index of the glucose solution is 2.34.
Michelson interferometer is an instrument used to measure the refractive index of a substance. It uses a laser beam that is divided into two equal parts, and each part travels a different path before recombining to produce an interference pattern on a screen.
A cuvette of thickness 10 mm is placed in one arm containing a glucose solution. As the glucose concentration increases, 88 fringes are observed to emerge at the screen. We need to determine the change in refractive index of the glucose solution.
The fringe order is given by:
n = (2t/λ) * δwhere,
t = thickness of the cuvette
λ = wavelength of the laser
δ = refractive index of the glucose solution
Since we know the values of t, λ and n, we can solve for
δδ = (nλ) / (2t)
= (88 × 530 nm) / (2 × 10 mm)
= 2.34
Therefore, the change in refractive index of the glucose solution is 2.34.
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Find the force corresponding to the potential energy
U(x) =-a/x + b/x^2 + cx^2
Answers
The force corresponding to the potential energy function U(x) = -a/x + b/[tex]x^{2}[/tex] + c[tex]x^{2}[/tex] can be obtained by taking the derivative of the potential energy function with respect to x. The force corresponding to the potential energy function is F(x) = a/[tex]x^{2}[/tex] - 2b/[tex]x^{3}[/tex] + 2cx.
To find the force corresponding to the potential energy function, we differentiate the potential energy function with respect to position (x). In this case, we have U(x) = -a/x + b/[tex]x^{2}[/tex] + c[tex]x^{2}[/tex].
Taking the derivative of U(x) with respect to x, we obtain:
dU/dx = -(-a/[tex]x^{2}[/tex]) + b(-2)/[tex]x^{3}[/tex] + 2cx
Simplifying the expression, we get:
dU/dx = a/[tex]x^{2}[/tex] - 2b/[tex]x^{3}[/tex] + 2cx
This expression represents the force corresponding to the potential energy function U(x). The force is a function of position (x) and is determined by the specific values of the constants a, b, and c in the potential energy function.
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Find the velocity at the bottom of the ramp of a marble rolling down a ramp with a vertical height of 8m. Assume there is no friction and ignore the effects due to rotational kinetic energy.
Answers
Neglecting the impact of friction and rotational kinetic energy, the approximate velocity at the base of a ramp is 12.53 m/s when a marble rolls down a ramp with a vertical height of 8m.
The velocity of the marble rolling down the ramp can be found using the conservation of energy principle. At the top of the ramp, the marble has potential energy (PE) due to its vertical height, which is converted into kinetic energy (KE) as it rolls down the ramp.
Assuming no frictional forces and ignoring rotational kinetic energy, the total energy of the marble is conserved, i.e.,PE = KE. Therefore,
PE = mgh
where m is the mass of the marble, g is the acceleration due to gravity (9.81 m/s²), and h is the vertical height of the ramp (8 m).
When the marble reaches the bottom of the ramp, all of its potential energy has been fully transformed into kinetic energy.
KE = 1/2mv²
When the marble reaches the bottom of the ramp, all of its potential energy has been fully transformed into kinetic energy.
Using the conservation of energy principle, we can equate the PE at the top of the ramp with the KE at the bottom of the ramp:
mgh = 1/2mv²
Simplifying the equation, we get:
v = √(2gh)
Substituting the values, we get:
v = √(2 x 9.81 x 8) = 12.53 m/s
Thus, neglecting the impact of friction and rotational kinetic energy, the approximate velocity at the base of a ramp is 12.53 m/s when a marble rolls down a ramp with a vertical height of 8m.
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QUESTION 20 When a positively charged rod is brought near a conducting sphere, negative charge migrates toward the side of the sphere close to the rod so that net positive charge is left on the other
Answers
When a positively charged rod is brought near a conducting sphere, negative charge migrates towards the side of the sphere closest to the rod, resulting in a net positive charge on the other side of the sphere.
This phenomenon occurs due to the principle of electrostatic induction. When a positively charged rod is brought near a conducting sphere, the positively charged rod induces a separation of charges in the conducting sphere. The positive charge on the rod repels the positive charges in the conducting sphere, causing them to move away from the rod.
At the same time, the negative charges in the conducting sphere are attracted to the positive rod, resulting in a migration of negative charge towards the side of the sphere closest to the rod.
As a result, the side of the conducting sphere closer to the positively charged rod becomes negatively charged due to the accumulation of negative charge, while the other side of the sphere retains a net positive charge since positive charges are repelled.
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What is the magnitude of the induced electric field at a point 0.500 cm from the axis of the solenoid? A long, thin solenoid has 870 turns per meter and radius 2.10 cm . The current in the solenoid is increasing at a uniform rate of 64.0 A/s.
Answers
The magnitude of the induced electric field at a point near the axis of the solenoid is approximately 0.988 T.
To determine the magnitude of the induced electric field at a point near the axis of the solenoid, we can use Faraday's law of electromagnetic induction. The formula is given by:
E = -N * (dΦ/dt) / A
where E is the magnitude of the induced electric field, N is the number of turns per unit length of the solenoid, dΦ/dt is the rate of change of magnetic flux, and A is the cross-sectional area of the solenoid.
First, we need to find the rate of change of magnetic flux (dΦ/dt). Since the solenoid has a changing current, the magnetic field inside the solenoid is also changing. The formula to calculate the magnetic field inside a solenoid is:
B = μ₀ * N * I
where B is the magnetic field, μ₀ is the permeability of free space (4π x 10^-7 T·m/A), N is the number of turns per unit length, and I is the current.
Taking the derivative of the magnetic field with respect to time, we get:
dB/dt = μ₀ * N * dI/dt
Now, we can substitute the values into the formula for the induced electric field:
E = -N * (dΦ/dt) / A = -N * (d/dt) (B * A) / A
Since the point of interest is near the axis of the solenoid, we can approximate the magnetic field as being constant along the length of the solenoid. Therefore, the derivative of the magnetic field with respect to time is equal to the derivative of the current with respect to time:
E = -N * (dI/dt) / A
Now, we can plug in the given values:
N = 870 turns/m = 8.7 x 10^3 turns/m
dI/dt = 64.0 A/s
A = π * r^2 = π * (0.021 m)^2
Calculating the magnitude of the induced electric field:
E = - (8.7 x 10^3 turns/m) * (64.0 A/s) / (π * (0.021 m)^2)
E ≈ -0.988 T
The magnitude of the induced electric field at a point 0.500 cm from the axis of the solenoid is approximately 0.988 T.
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A
20-g cylinder of radius 5.0 cm starts to rotate from rest, reaching
200 rpm in half a minute. Find the net torque acting on the
cylinder.
Answers
The net torque acting on the cylinder is approximately 0.031 N·m.
To find the net torque acting on the cylinder, we can use the rotational motion equation:
Torque (τ) = Moment of inertia (I) × Angular acceleration (α).
Given that the cylinder starts from rest and reaches 200 rpm (revolutions per minute) in half a minute, we can calculate the angular acceleration. First, we convert the angular velocity from rpm to radians per second (rad/s):
ω = (200 rpm) × (2π rad/1 min) × (1 min/60 s) = 20π rad/s.
The angular acceleration (α) can be calculated by dividing the change in angular velocity (Δω) by the time taken (Δt):
α = Δω/Δt = (20π rad/s - 0 rad/s)/(30 s - 0 s) = (20π/30) rad/s².
Next, we need to calculate the moment of inertia (I) for the cylinder. The moment of inertia of a solid cylinder rotating about its central axis is given by:
I = (1/2)mr²,
where m is the mass of the cylinder and r is its radius.
Converting the mass of the cylinder from grams to kilograms, we have:
m = 20 g = 0.02 kg.
Substituting the values of m and r into the moment of inertia equation, we get:
I = (1/2)(0.02 kg)(0.05 m)² = 2.5 × 10⁻⁵ kg·m².
Now, we can calculate the net torque by multiplying the moment of inertia (I) by the angular acceleration (α):
τ = I × α = (2.5 × 10⁻⁵ kg·m²) × (20π/30) rad/s² ≈ 0.031 N·m.
Therefore, the net torque acting on the cylinder is approximately 0.031 N·m.
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A normal person has a near point at 25 cm and a far point at infinity. Suppose a nearsighted person has a far point at 157 cm. What power lenses would prescribe?
Answers
To correct the nearsightedness of a person with a far point at 157 cm, lenses with a power of approximately -0.636 diopters (concave) should be prescribed. Consultation with an eye care professional is important for an accurate prescription and fitting.
To determine the power of lenses required to correct the nearsightedness of a person, we can use the formula:
Lens Power (in diopters) = 1 / Far Point (in meters)
Given that the far point of the nearsighted person is 157 cm (which is 1.57 meters), we can substitute this value into the formula:
Lens Power = 1 / 1.57 = 0.636 diopters
Therefore, a nearsighted person with a far point at 157 cm would require lenses with a power of approximately -0.636 diopters. The negative sign indicates that the lenses need to be concave (diverging) in nature to help correct the person's nearsightedness.
These lenses will help diverge the incoming light rays, allowing them to focus properly on the retina, thus improving distance vision for the individual. It is important for the individual to consult an optometrist or ophthalmologist for an accurate prescription and proper fitting of the lenses based on their specific needs and visual acuity.
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In a microwave receiver circuit, the resistance R of a wire 1 m long is given by R= k/d^2
z Where d is the diameter of the wire. Find R if k=0.00000002019 omega m^2 and d = 0.00007892 m.
Answers
The resistance (R) of the wire is approximately 32.138 ohms, calculated using the given values and the equation R = k / (d^2z).
To find the resistance R of the wire, we can substitute the given values into the equation R = k/d^2z.
k = 0.00000002019 Ωm^2
d = 0.00007892 m
z = 1 (since it is not specified)
Substituting these values:
R = k / (d^2z)
R = 0.00000002019 Ωm^2 / (0.00007892 m)^2 * 1
Calculating the result:
R ≈ 32.138 Ω
Therefore, the resistance R of the wire is approximately 32.138 ohms.
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Safety brake on saw blade A table saw has a circular spinning blade with moment of inertia 1 (including the shaft and mechanism) and is rotating at angular velocity wo. Some newer saws have a system for detecting if a person has touched the blade and have brake mechanism. The brake applies a frictional force tangent to the rotation, at a distance from the axes. 1. How much frictional force must the brake apply to stop the blade in time t? (Answer in terms of I, w, and T.) 2. Through what angle will the blade rotate while coming to a stop? Give your answer in degrees.
Answers
1. The frictional force required to stop the blade in time t is given by Ffriction = wo ÷ r ÷ T.
2. The blade will rotate through an angle of θ = wo² × T × (1 + T × r × I/2) or wo² × T × (1 + 0.5 × T × I × r). And in degrees θ(degrees) = wo² × T × (1 + 0.5 × T × r) × 180/π.
1. The blade must be stopped in time t by a brake that applies a frictional force tangent to the rotation, at a distance r from the axes. The force required to stop the blade is given by the equation;
Ffriction = I × w ÷ r ÷ t
Where,
I = moment of inertia = 1
w = angular velocity = wo
T = time required to stop the blade
Thus;
Ffriction = I × w ÷ r ÷ T
= 1 × wo ÷ r ÷ T
Therefore, the frictional force required to stop the blade in time t is given by Ffriction = wo ÷ r ÷ T.
2. The angle rotated by the blade while coming to a stop can be determined using the equation for angular displacement.
θ = wo × T + 1/2 × a × T²
where,
a = acceleration of the blade
From the equation,
Ffriction = I × w ÷ r ÷ t
a = Ffriction ÷ I
m = 1 × wo ÷ r
θ = wo × T + 1/2 × (Ffriction ÷ I) × T²
θ = wo × T + 1/2 × (wo ÷ r ÷ I) × T²
θ = wo × T + 1/2 × (wo ÷ r) × T²
θ = wo × T + 1/2 × (wo² × T²) ÷ (r × I)
θ = wo × T + 1/2 × wo² × T²
Substitute the values of wo and T in the above equation to obtain the angular displacement;
θ = wo × T + 1/2 × wo² × T²
θ = wo × (wo ÷ r ÷ Ffriction) + 1/2 × wo² × T²
θ = wo × (wo ÷ r ÷ (wo ÷ r ÷ T)) + 1/2 × wo² × T²
θ = wo² × T + 1/2 × wo² × T² × (r × I)
θ = wo² × T × (1 + 1/2 × T × r × I)
θ = wo² × T × (1 + T × r × I/2)
Thus, the blade will rotate through an angle of θ = wo² × T × (1 + T × r × I/2) or wo² × T × (1 + 0.5 × T × I × r).
The answer is to be given in degrees. Therefore, the angular displacement is; θ = wo² × T × (1 + 0.5 × T × I × r)
θ = wo² × T × (1 + 0.5 × T × 1 × r)
= wo² × T × (1 + 0.5 × T × r)
Converting from radians to degrees;
θ(degrees) = θ(radians) × 180/π
θ(degrees) = wo² × T × (1 + 0.5 × T × r) × 180/π.
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HAIS Please Consider a inner & outer radil Ry 3 R₂, respectively. R₂ A HR I J= R1 hollow longmetalic Acylinder of I current of current density I 15 flowing in the hollow cylinder, Please find the magnetic field energy within the men per unit length
Answers
To find the magnetic field energy within a hollow long metallic cylinder with inner radius R₁ and outer radius R₂, through which a current density of J = 15 is flowing, we can use the formula for magnetic field energy per unit length. The calculation involves integrating the energy density over the volume of the cylinder and then dividing by the length.
The magnetic field energy within the hollow long metallic cylinder per unit length can be calculated using the formula:
Energy per unit length = (1/2μ₀) ∫ B² dV
where μ₀ is the permeability of free space, B is the magnetic field, and the integration is performed over the volume of the cylinder.
For a long metallic cylinder with a hollow region, the magnetic field inside the cylinder is given by Ampere's law as B = μ₀J, where J is the current density.
To evaluate the integral, we can assume the current flows uniformly across the cross-section of the cylinder, and the magnetic field is uniform within the cylinder. Thus, we can express the volume element as dV = Adx, where A is the cross-sectional area of the cylinder and dx is the infinitesimal length.
Substituting the values and simplifying the integral, we have:
Energy per unit length = (1/2μ₀) ∫ (μ₀J)² Adx
= (1/2) J² A ∫ dx
= (1/2) J² A L
where L is the length of the cylinder.
Therefore, the magnetic field energy within the hollow long metallic cylinder per unit length is given by (1/2) J² A L, where J is the current density, A is the cross-sectional area, and L is the length of the cylinder.
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1)How much energy would be required to convert 15.0 grams of ice at –18.4 ºC into steam at 126.4 ºC.?
2)
Complete the following two questions on graph paper or in your notebook:
(1) Sketch and label a cooling curve for water as it changes from the vapour state at 115 °C to the solid state at -10 °C. Assume that the water passes through all three states of matter.
(2) How much heat is absorbed in changing 2.00 kg of ice at −5.0 °C to steam at 110 °C?
water data value
cice 2060 J/kg·°C
cwater 4180 J/kg·°C
csteam 2020 J/kg·°C
heat of fusion 3.34 x 105 J/kg
heat of vaporization 2.26 x 106 J/kg
This is a six step question. You will calculate five heat quantities and then total them.
Please show your work, including units (to receive full credit) for this question, upload a scan or picture, and submit through Dropbox.
Answers
The energy required to convert 15.0 grams of ice at -18.4ºC into steam at 126.4ºC is approximately 45,737 Joules.
To convert ice at -18.4ºC into steam at 126.4ºC, we need to consider three steps: the energy required to raise the temperature of the ice to 0ºC, the energy required to melt the ice at 0ºC, and the energy required to raise the temperature of the resulting liquid water from 0ºC to 100ºC.
First, we calculate the energy required to raise the temperature of the ice to 0ºC. The mass of ice is given as 15.0 grams, and the heat capacity of ice is 2.09 J/g·ºC. Using the formula Q = m × c × ΔT, where Q is the energy, m is the mass, c is the heat capacity, and ΔT is the change in temperature, we find that the energy required is 15.0 g × 2.09 J/g·ºC × (0 ºC - (-18.4 ºC)) = 556.8 J.
Next, we calculate the energy required to melt the ice at 0 ºC. The heat of fusion for ice is 334 J/g. So the energy required is 15.0 g × 334 J/g = 5010 J.
Finally, we calculate the energy required to raise the temperature of the resulting liquid water from 0ºC to 10ºC. The heat capacity of water is 4.18 J/g·ºC. Using the same formula as before, we find that the energy required is 15.0 g × 4.18 J/g·ºC × (100ºC - 0ºC) = 6270 J.
Adding up all three steps, we get a total energy requirement of 556.8 J + 5010 J + 6270 J = 11,836.8 J.
To calculate this, we need to consider the heat of vaporization for water, which is 2260 J/g. Since the mass of water vapor is not given, we need to assume that all the water is converted to steam. Therefore, the energy required is 15.0 g × 2260 J/g = 33,900 J.
Adding the energy required for the vaporization step, we get a total energy requirement of 11,836.8 J + 33,900 J = 45,736.8 J.
Hence, the energy required to convert 15.0 grams of ice at -18.4 ºC into steam at 126.4 ºC is approximately 45,737 Joules.
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How many lines per centimeter are there on a diffraction grating that gives a first-order maximum for 460-nm blue light at an angle of 17 deg? Hint The diffraction grating should have lines per centim
Answers
The diffraction grating that gives a first-order maximum for 460 nm blue light at an angle of 17 degrees should have approximately 0.640 lines per millimeter.
The formula to find the distance between two adjacent lines in a diffraction grating is:
d sin θ = mλ
where: d is the distance between adjacent lines in a diffraction gratingθ is the angle of diffraction
m is an integer that is the order of the diffraction maximumλ is the wavelength of the light
For first-order maximum,
m = 1λ = 460 nmθ = 17°
Substituting these values in the above formula gives:
d sin 17° = 1 × 460 nm
d sin 17° = 0.15625
The grating should have lines per centimeter. We can convert this to lines per millimeter by dividing by 10, i.e., multiplying by 0.1.
d = 0.1/0.15625
d = 0.640 lines per millimeter (approx)
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