The percent difference between the two measurements of the acceleration due to gravity is approximately 2.15%.
To calculate the percent difference between the two measurements, we can use the formula:
Percent Difference = (|Measurement 1 - Measurement 2| / ((Measurement 1 + Measurement 2) / 2)) * 100%
Measurement 1 = 9.67 m/s^2
Measurement 2 = 9.88 m/s^2
Percent Difference = (|9.67 - 9.88| / ((9.67 + 9.88) / 2)) * 100%
= (0.21 / (19.55 / 2)) * 100%
= (0.21 / 9.775) * 100%
≈ 2.15%
Therefore, the percent difference between the two measurements is approximately 2.15%.
The percent difference between the measurements of the acceleration due to gravity is a measure of the discrepancy between the two values. In this case, the percent difference is approximately 2.15%, indicating a relatively small difference between the two measurements.
Additional analysis and consideration of factors such as experimental uncertainties and measurement errors would be required for a more comprehensive evaluation of the measurements' reliability.
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QUESTION 15 2 A turntable has a moment of inertia of 0.89 kg m and rotates freely on a frictionless support at 37 rev/min. A 0.40-kg ball of putty is dropped vertically onto the turntable and hits a point 0.29 m from the center, changing its rate at 6 rev/min. By what factor does the kinetic energy of the system change after the putty is dropped onto the turntable? Give your answer to 2 decimal places
The moment of inertia of the turntable is 0.89 kg m. The turntable rotates freely on a frictionless support at 37 rev/min. The distance from the center where the 0.40-kg putty is dropped is 0.29 m. The rate of rotation of the turntable reduces to 6 rev/min after the putty is dropped.
We need to find the factor by which the kinetic energy of the system changes. Firstly, let us find the initial kinetic energy of the turntable. Given, moment of inertia of turntable, I = 0.89 kg mInitial angular speed, ωi = 37 rev/minInitial angular speed, ωi = 37 × 2π / 60 = 3.88 rad/sInitial kinetic energy of turntable, KEi = (1 / 2) I ωi² = (1 / 2) × 0.89 × (3.88)² ≈ 6.54 JoulesLet us now find the kinetic energy of the turntable after the putty has dropped. Let the angular velocity of the turntable after the putty has dropped be ωf.
Now, since angular momentum is conserved, we have the equation,I ωi = (I + mr²) ωfwhere m is the mass of the putty and r is the distance between the center of turntable and the point where the putty is dropped. Substituting values, we have0.89 × 3.88 = (0.89 + 0.40) r² ωf => r² ωf = 1.00Solving for ωf, we getωf = 1.00 / r²Substituting r = 0.29 m, we haveωf ≈ 12.82 rad/sLet us now find the final kinetic energy of the system.
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A 6.0-m uniform board is supported by two sawhorses 4.0 m aprat as shown. A 32 kg child walks on the board to 1.4 m beyond the right support when the board starts to tip, that is, the board is off the left support. Find the mass of the board. (Hint: the weight of the board can be considered to be applied at its center of gravity.)
When 6.0-m uniform board is supported by two sawhorses 4.0 m apart and a 32 kg child walks on the board to 1.4 m beyond the right support when the board starts to tip, that is, the board is off the left support then the mass of the board is 1352 kg.
Given data :
Length of board = L = 6 m
Distance between sawhorses = d = 4 m
Mass of child = m = 32 kg
The child walks to a distance of x = 1.4 m beyond the right support.
The length of the left over part of the board = L - x = 6 - 1.4 = 4.6 m
As the board is uniform, the center of gravity is at the center of the board.The weight of the board can be considered to be applied at its center of gravity. The board will remain in equilibrium if the torques about the two supports are equal.
Thus, we can apply the principle of moments.
ΣT = 0
Clockwise torques = anticlockwise torques
(F1)(d) = (F2)(L - d)
F1 = (F2)(L - d)/d
Here, F1 + F2 = mg [As the board is in equilibrium]
⇒ F2 = mg - F1
Putting the value of F2 in the equation F1 = (F2)(L - d)/d
We get, F1 = (mg - F1)(L - d)/d
⇒ F1 = (mgL - mF1d - F1L + F1d)/d
⇒ F1(1 + (L - d)/d) = mg
⇒ F1 = mg/(1 + (L - d)/d)
Putting the given values, we get :
F1 = (32)(9.8)/(1 + (6 - 4)/4)
F1 = 588/1.5
F1 = 392 N
Let the mass of the board be M.
The weight of the board W = Mg
Let x be the distance of the center of gravity of the board from the left support.
We have,⟶ Mgx = W(L/2) + F1d
Mgx = Mg(L/2) + F1d
⇒ Mgx - Mg(L/2) = F1d
⇒ M(L/2 - x) = F1d⇒ M = (F1d)/(L/2 - x)
Substituting the values, we get :
M = (392)(4)/(6 - 1.4)≈ 1352 kg
Therefore, the mass of the board is 1352 kg.
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A guitar chord is 43 cm long and has diameter of 1 mm. What is the tensile force that will break the chord assuming that the ultimate tensile strength of high-carbon steel is 2500 x 106 N/m2. O a. 796 N O b. 7854 N O c. 2500 N O d. 1963 N
To calculate the tensile force that will break the guitar chord, we need to consider the cross-sectional area of the chord and the ultimate tensile strength of the material . The tensile force that will break the guitar chord is approximately 1963 N (option d).
Given: Length of the chord (L) = 43 cm = 0.43 m
Diameter of the chord (d) = 1 mm = 0.001 m
Ultimate tensile strength of high-carbon steel (σ) = 2500 x 10^6 N/m^2
First, we need to calculate the cross-sectional area (A) of the chord. Since the chord is assumed to be cylindrical, the cross-sectional area can be calculated using the formula:
A = π * (d/2)^2
Substituting the values, we have:
A = π * (0.001/2)^2 = 0.0000007854 m^2
Next, we can calculate the tensile force (F) using the formula:
F = A * σ
Substituting the values, we get:
F = 0.0000007854 m^2 * 2500 x 10^6 N/m^2 = 1963 N
Therefore, the tensile force that will break the guitar chord is approximately 1963 N (option d).
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Required Information Suppose 100 mol of oxygen is heated at a constant pressure of 100 atm from 100'C 10 25 0°C, What is the magnitude of the work done by the gas during this expansion? The magnitude of the work done by the gas is
The magnitude of the work done by the gas during this expansion is 827 J.
The magnitude of the work done by the gas during this expansion of 100 moles of oxygen heated at a constant pressure of 100 atm from 100°C to 25°C can be calculated using the following equation for work done:
[tex]W = -PΔV[/tex]
where, P is the pressure of the gas and ΔV is the change in the volume of the gas.
The change in volume can be calculated using the ideal gas law:
PV = nRT, where, P is the pressure, V is the volume, n is the number of moles, R is the ideal gas constant and T is the temperature in Kelvin.
Using this formula, we can calculate the initial and final volumes of the gas. Let's assume the initial volume is V1 and the final volume is V2.
Therefore, [tex]PV1 = nRT1[/tex]
PV2 = nRT2
ΔV = V2 - V1
= (nR/P) (T1 - T2)
Putting the values, we get:
ΔV = (100 mol x 8.314 J/mol.K x (100+273) K) / 100 atm - (100 mol x 8.314 J/mol.K x (25+273) K) / 100 atm
ΔV = 8.27 L
The work done by the gas is:
W = -PΔV
= -100 atm x (-8.27 L)
= 827 J
Therefore, the magnitude of the work done by the gas during this expansion is 827 J.
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Suppose a 373 cm long, 8.5 cm diameter solenoid has 1000 loops. #33% Part (a) Calculate the self-inductance of it in mil * Attempts Remain 33% Part (b) How much energy is stored in this inductor when 79,5 A of'current flows through it? Give your answer in J.
The self-inductance of a solenoid with given dimensions and number of loops is calculated to be approximately 1.177 mH. The energy stored in the solenoid with a current of 79.5 A is approximately 2.212 J.
Part (a) To calculate the self-inductance of the solenoid, we can use the formula:
L = (μ₀ * N^² * A) / l
where L is the self-inductance, μ₀ is the permeability of free space (4π × 10^−7 T·m/A), N is the number of loops, A is the cross-sectional area, and l is the length of the solenoid.
First, we need to calculate the cross-sectional area A of the solenoid:
A = π * (r²)
where r is the radius of the solenoid (half of the diameter).
Given that the diameter is 8.5 cm, the radius is 4.25 cm (0.0425 m).
A = π * (0.0425)^2
A ≈ 0.005664 m^²
Now we can calculate the self-inductance L:
L = (4π × 10^−7 T·m/A) * (1000^2) * (0.005664 m^²) / 3.73 m
L ≈ 1.177 mH (millihenries)
Therefore, the self-inductance of the solenoid is approximately 1.177 mH.
Part (b) To calculate the energy stored in the inductor, we can use the formula:
E = (1/2) * L * (I^2)
where E is the energy, L is the self-inductance, and I is the current flowing through the inductor.
Given that the current is 79.5 A, and the self-inductance is 1.177 mH (or 0.001177 H), we can substitute these values into the formula:
E = (1/2) * 0.001177 H * (79.5 A)^2
E ≈ 2.212 J (joules)
Therefore, the energy stored in the inductor when 79.5 A of current flows through it is approximately 2.212 joules.
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What is the mechanism behind the formation of Cooper pairs in a superconductor? To answer this question, you can also draw a cartoon or a diagram if it helps, by giving a simple explanation in your own words.
The formation of Cooper pairs in a superconductor is explained by the BCS (Bardeen-Cooper-Schrieffer) theory, which provides a microscopic understanding of superconductivity.
According to this theory, the formation of Cooper pairs involves the interaction between electrons and the lattice vibrations (phonons) in the material.
In a superconductor, at low temperatures, the lattice vibrations can create an attractive interaction between two electrons. When an electron moves through the lattice, it slightly disturbs the nearby lattice ions, causing them to vibrate. These vibrations can be thought of as "virtual" phonons.Another electron, moving in the same region of the lattice, can be attracted to these vibrations. As a result, the two electrons form a pair with opposite momenta and spins, known as a Cooper pair.Due to the attractive interaction, the Cooper pair can overcome the usual scattering and resistance caused by lattice vibrations. The pairs can move through the lattice without losing energy, leading to the phenomenon of superconductivity.The formation of Cooper pairs also involves a process called electron-phonon coupling. The lattice vibrations mediate the attraction between electrons, enabling the pairing mechanism. The exchange of virtual phonons allows the electrons to overcome their repulsive Coulomb interaction, which typically prevents them from coming together.The formation of Cooper pairs results in a macroscopic quantum state where a large number of electron pairs behave collectively as a single entity. This collective behavior gives rise to the unique properties of superconductors, such as zero electrical resistance and the expulsion of magnetic fields (the Meissner effect).Thus, the mechanism involved is the "Bardeen-Cooper-Schrieffer theory".
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A conductor of length 100 cm moves at right angles to a uniform magnetic field of flux density 1.5 Wb/m2 with velocity of 50meters/sec.
Calculate the e.m.f. induced in it.
Find also the value of induced e.m.f. when the conductor moves at an angle of 300 to the direction of the field
A conductor of length 100 cm moves at right angles to a
uniform magnetic
field of flux density 1.5 Wb/m2 with velocity of 50meters/sec, to find the induced emf.
The formula to determine the induced emf in a conductor is E= BVL sin (θ) where B is the magnetic field strength, V is the velocity of the conductor, L is the length of the conductor, and θ is the angle between the velocity and magnetic field vectors.
Let us determine the induced emf using the given
values
in the formula.E= BVL sin (θ)Given, B= 1.5 Wb/m2V= 50m/sL= 100 cm= 1 mθ= 30°= π/6 radTherefore, E= (1.5 Wb/m2) x 50 m/s x 1 m x sin (π/6)= 1.5 x 50 x 0.5= 37.5 VTherefore, the induced emf when the conductor moves at an angle of 300 to the direction of the field is 37.5 V.
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For the following three measurements trials L1 L2 L3 Length (cm) 8.0 8.2 8.9 Calculate the absolute error (AL)? O 1.0.36 02.0.37 03.0.4 04.0.366 O 5.0.0
The absolute error is 0.36. Option 1 is correct.
Given the following measurements trials, L1, L2, and L3 as:
Length (cm): 8.0, 8.2, 8.9
To calculate the absolute error, we first calculate the mean of the three values:
Mean = (L1 + L2 + L3) / 3= (8.0 + 8.2 + 8.9) / 3= 8.37
Now, we calculate the absolute deviation from the mean for each measurement. We take the absolute value of the difference between each measurement and the mean.
Absolute deviation for L1 = |8.0 - 8.37| = 0.37
Absolute deviation for L2 = |8.2 - 8.37| = 0.17
Absolute deviation for L3 = |8.9 - 8.37| = 0.53
The absolute error (AL) is the average of the absolute deviations from the mean.
AL = (0.37 + 0.17 + 0.53) / 3= 0.3567...= 0.36 (rounded to two decimal places)
Therefore, the absolute error is 0.36. Option 1 is correct.
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Assume that an electron in an atom can be treated as if it were confined to a box of width 3.6 angstrom. What is the ground state energy of this electron? Hint Ground state energy of electron in a box of width 3.6 angstrom is eV. Note: For the purpose of comparison, note that kinetic energy of an electron in hydrogen atom ground state is 13.6 eV. Does this model seem reasonable?
The ground state energy of an electron confined to a box with a width of 3.6 angstroms is approximately 11.28 eV, which is lower than the kinetic energy of an electron in the ground state of a hydrogen atom (13.6 eV). This model of confinement appears reasonable as it predicts a lower energy state for the electron, although it is a simplified representation that does not encompass all the intricacies of an atom.
To calculate the ground state energy of an electron confined to a box of width 3.6 angstroms, we can use the formula for the energy levels of a particle in a one-dimensional box:
E = [tex](h^2 * n^2) / (8 * m * L^2)[/tex]
Where:
E is the energy level
h is the Planck's constant (approximately 6.626 x[tex]10^-34[/tex] J·s)
n is the quantum number of the energy level (1 for the ground state)
m is the mass of the electron (approximately 9.109 x [tex]10^-31[/tex] kg)
L is the width of the box (3.6 angstroms, which is equivalent to 3.6 x [tex]10^-10[/tex] meters)
Let's substitute the values into the formula:
[tex]E = (6.626 x 10^-34 J·s)^2 * (1^2) / (8 * 9.109 x 10^-31 kg * (3.6 x 10^-10 m)^2)\\E ≈ 1.806 x 10^-18 J[/tex]
To convert this energy to electron volts (eV), we can use the conversion factor:
[tex]1 eV = 1.602 x 10^-19 J[/tex]
Ground state energy ≈[tex](1.806 x 10^-18 J) / (1.602 x 10^-19 J/eV)[/tex] ≈ 11.28 eV (rounded to two decimal places)
The ground state energy of the electron confined to a box of width 3.6 angstroms is approximately 11.28 eV.
Now, comparing this to the kinetic energy of an electron in the hydrogen atom's ground state (which is given as 13.6 eV), we can see that the ground state energy of the confined electron is significantly lower. This model of confining the electron to a box seems reasonable as it predicts a lower energy state for the electron compared to its energy in the hydrogen atom.
However, it's important to note that this model is a simplified representation and doesn't capture all the complexities of an actual atom.
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Question 7 (MCQ QUESTION) [8 Marks] Consider a system of an ideal gas consisting of either Bosons or Fermions. The average occupation number for such a system with energy & is given by n(e) = N = ñ(E)g(E)de N = n(E)g(E) N = [n(E)g(E) de 1 = ñ(E) * 9 (E) de N = g(E) (E) de 1(E) S™ ( e ±1 where +/- signs refer to Fermions/Bosons respectively. a) The total number of particles in such a system is given by which of the following expressions, where f(e) is the average occupation number and g() is the density of states: [2] Possible answers (order may change in SAKAI
The total number of particles in a system of either Bosons or Fermions can be calculated using the average occupation number and the density of states.
For Fermions, the expression is N = ∫f(E)g(E)dE, and for Bosons, the expression is N = ∫[f(E)g(E)/[exp(E/kT)±1]]dE, where f(E) is the average occupation number and g(E) is the density of states.
In a system of Fermions, each energy level can be occupied by only one particle due to the Pauli exclusion principle. Therefore, the total number of particles (N) is calculated by summing the average occupation number (f(E)) over all energy levels, represented by the integral ∫f(E)g(E)dE.
In a system of Bosons, there is no restriction on the number of particles that can occupy the same energy level. The distribution of particles follows Bose-Einstein statistics, and the average occupation number is given by f(E) = 1/[exp(E/kT)±1], where ± signs refer to Bosons/Fermions, respectively. The total number of particles (N) is calculated by integrating the expression [f(E)g(E)/[exp(E/kT)±1]] over all energy levels, represented by the integral ∫[f(E)g(E)/[exp(E/kT)±1]]dE.
By using the appropriate expression based on the type of particles (Bosons or Fermions) and integrating over the energy levels, we can calculate the total number of particles in the system.
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A large air conditioner has a resistance of 11.6 ohms, and an inductive reactance of 14.1 ohms in series (no capacitive reactance). If the air conditioner is powered by a 50.0 Hz generator with an rms voltage of 113 V, find the total impedance of the air conditioner and its rms current.
The total impedance of the air conditioner is 18.2 Ω and its rms current is 6.2 A.
Given data:
Resistance of air conditioner (R) = 11.6 ohms
Inductive reactance (XL) = 14.1 ohms
Frequency (f) = 50.0 Hz
RMS voltage (Vrms) = 113 V
We need to find the total impedance of the air conditioner and its rms current.
The formula for the total impedance of the air conditioner is:
Z=√(R²+X_L² )
Where
Z is the total impedance of the air conditioner
R is the resistance of the air conditioner
XL is the inductive reactance of the air conditioner
So, total impedance of the air conditioner:
Z = √(11.6² + 14.1² )= 18.2 Ω
The formula for rms current is:
I_rms=V_rms/Z
Where
I_rms is the rms current of the air conditioner
Z is the total impedance of the air conditioner
V_rms is the RMS voltage of the generator
So, the rms current of the air conditioner:
I_rms = V_rms / Z= 113 / 18.2= 6.2 A
Therefore, the total impedance of the air conditioner is 18.2 Ω and its rms current is 6.2 A.
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Problem 2. Decibel scale in acoustic equipment. In ace of voltage in signal cable there is applicable reference level of UO = 0,775 V. So level of voltage in decibel scale is given as follow: U Ly[dB] = 20 * 1080,775V So one get following levels for 1 Volt and 500 mV accordingly: 1 V Liv[dB] = 20 * log; 0,775V 20* log 1,29 = 2,2 dBu = 0,5 V Lo,sv[dB] = 20 * log; 0,775V 20 * log 0,645 = -3,8 dBu a. Compute level value in dB for U=1 mV, U = 5 mv, U=20 UV. b. Compute the voltage, which level is equal 12 dB.
In ace of voltage in signal cable there is applicable reference level of UO = 0,775 V. The voltage corresponding to a level of 12 dB is approximately 1.947 V.
a. To compute the level value in decibels for different voltage values, we can use the formula: Level [dB] = 20 * log10(Vin / Vref)
Where: Vin is the input voltage.
Vref is the reference voltage (0.775 V in this case).
Let's calculate the level values for the given voltage values:
For U = 1 mV:
Level [dB] = 20 * log10(1 mV / 0.775 V)
Level [dB] = 20 * log10(0.00129)
Level [dB] ≈ -59.92 dBu
For U = 5 mV:
Level [dB] = 20 * log10(5 mV / 0.775 V)
Level [dB] = 20 * log10(0.00645)
Level [dB] ≈ -45.76 dBu
For U = 20 µV:
Level [dB] = 20 * log10(20 µV / 0.775 V)
Level [dB] = 20 * log10(0.0000258)
Level [dB] ≈ -95.44 dBu
b. To compute the voltage corresponding to a level of 12 dB, we rearrange the formula:
Level [dB] = 20 * log10(Vin / Vref)
Let's solve for Vin:
12 = 20 * log10(Vin / 0.775 V)
0.6 = log10(Vin / 0.775 V)
Now, we can convert it back to exponential form:
10^0.6 = Vin / 0.775 V
Vin = 0.775 V * 10^0.6
Vin ≈ 1.947 V
So, the voltage corresponding to a level of 12 dB is approximately 1.947 V.
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A 12.2-kg cylinder roils without slipping on a rough surface. At an instant when its center of gravity has a speed of 11.7 m/s, determine the following (a) the translational kinetic energy of its center of gravity (b) the rotational kinetic energy about its center of gravity 1 (c) its total kinetic energy
(a) The translational kinetic energy of the cylinder's centre of gravity is 729.63 J.
(b) The rotational kinetic energy about its centre of gravity is 729.63 J.
(c) The total kinetic energy of the cylinder is 1,459.26 J.
(a) To find the translational kinetic energy, we use the formula KE_trans = (1/2) * m * v^2, where m is the mass of the cylinder and v is the speed of its centre of gravity. Substituting the given values, KE_trans = (1/2) * 12.2 kg * (11.7 m/s)^2 = 729.63 J.
(b) The rotational kinetic energy about the centre of gravity can be calculated using the formula KE_rot = (1/2) * I * ω^2, where I is the moment of inertia and ω is the angular velocity. Since the cylinder rolls without slipping, we can relate the linear velocity of the centre of gravity to the angular velocity by v = ω * R, where R is the radius of the cylinder.
Rearranging the equation, we have ω = v / R. The moment of inertia for a cylinder rotating about its central axis is I = (1/2) * m * R^2. Substituting the values, KE_rot = (1/2) * (1/2) * 12.2 kg * (11.7 m/s / R)^2 = 729.63 J.
(c) The total kinetic energy is the sum of the translational and rotational kinetic energies, which gives us 1,459.26 J.
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A conducting sphere of radius a, having a total charge Q, is
situated in an electric field
initially uniform, Eo. Determine the potential at all points
outside the sphere.
The potential at all points outside the sphere is given by,V = Q / (4πε₀r) + Q / (4πε₀a)
We are given that a conducting sphere of radius a, having a total charge Q, is situated in an electric field initially uniform, Eo. We need to determine the potential at all points outside the sphere.Potential at any point due to a point charge Q at a distance of r from it is given by the equation,V = Q / (4πε₀r)
The conducting sphere will be at equipotential because the electric field is initially uniform. Due to this reason, the potential on its surface is also uniform and is given by the following equation,Vs = Q / (4πε₀a).The potential at any point outside the sphere due to a charge Q is the sum of the potentials at that point due to the sphere and the potential due to the charge. Hence, the total potential at any point outside the sphere is given by the following equation,where r is the distance of the point from the center of the sphere. Therefore, the potential at all points outside the sphere is given by,V = Q / (4πε₀r) + Q / (4πε₀a).
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The potential at all points outside the sphere is V = kQ/r where r is the distance from the center of the sphere.
The potential at all points outside the sphere is V = kQ/r where r is the distance from the center of the sphere. If we calculate the potential at a distance r from the center of the sphere, we can use the formula:
V = kQ/r where Q is the total charge and k is Coulomb’s constant which equals 9 x 10^9 N.m²/C².
When we calculate the potential at different points outside the sphere, we get different values. When the distance r is infinity, the potential is zero. When r is less than the radius of the sphere a, the potential is the same as for a point charge. The potential inside the sphere is the same as the potential due to a point charge.
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A certain boat traveling on a river displaces a volume of 6.7 m of water. The density of the water is 1000 kg/m2.) a. What is the mass of the water displaced by the boat? b. What is the weight of the boat?
According to the question (a). The mass of the water displaced by the boat is 6700 kg. (b). The weight of the boat is 65560 N.
a. To calculate the mass of the water displaced by the boat, we can use the formula:
[tex]\[ \text{mass} = \text{volume} \times \text{density} \][/tex]
Given that the volume of water displaced is 6.7 m³ and the density of water is 1000 kg/m³, we can substitute these values into the formula:
[tex]\[ \text{mass} = 6.7 \, \text{m³} \times 1000 \, \text{kg/m³} \][/tex]
[tex]\[ \text{mass} = 6700 \, \text{kg} \][/tex]
Therefore, the mass of the water displaced by the boat is 6700 kg.
b. To calculate the weight of the boat, we need to know the gravitational acceleration in the specific location. Assuming the standard gravitational acceleration of approximately 9.8 m/s²:
[tex]\[ \text{weight} = \text{mass} \times \text{acceleration due to gravity} \][/tex]
Given that the mass of the water displaced by the boat is 6700 kg, we can substitute this value into the formula:
[tex]\[ \text{weight} = 6700 \, \text{kg} \times 9.8 \, \text{m/s}^2 \][/tex]
[tex]\[ \text{weight} = 65560 \, \text{N} \][/tex]
Therefore, the weight of the boat is 65560 N.
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16) (10 points) Alpha particles (charge - +2e, mass - 6.68 x 10-27 kg) are accelerated in a cyclotron to a final orbit radius of 0.50 m. The magnetic field in the cyclotron is 0.50T What is the kinetic energy?
The kinetic energy of the alpha particles accelerated in a cyclotron to a final orbit radius of 0.50 m is 3.37 MeV.
Given that, Charge of alpha particles, q = +2e
Mass of alpha particles, m = 6.68 × 10-27 kg
Magnetic field, B = 0.50T
Radius of the orbit, r = 0.50 m
The magnetic force acting on an alpha particle that's in circular motion is the centripetal force acting on it. It follows from the formula Fm = Fc where Fm is the magnetic force and Fc is the centripetal force that, qv
B = mv²/r ... [1]Here, v is the velocity of the alpha particles. We know that the kinetic energy of the alpha particles is,
K.E. = 1/2 mv² ... [2] From equation [1], we can isolate the velocity of the alpha particles as follows,
v = qBr/m... [3]Substituting the equation [3] into [2], we get,
K.E. = 1/2 (m/qB)² q²B²r²/m
K.E. = q²B²r²/2m ... [4]
The value of q2/m is equal to 3.2 1013 J/T. Therefore, K.E. = 3.2 × 10¹³ J/T × (0.50 T)² × (0.50 m)²/2(6.68 × 10⁻²⁷ kg)
K.E. = 3.37 MeV Hence, the kinetic energy of the alpha particles is 3.37 MeV.
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30 (a) A 50 loop, circular coil has a radius of 10 cm and resistance of 2.0 n. The coil is connected to a resistance R = 1.00, to make a complete circuit. It is then positioned as shown in a uniform magnetic field that varies in time according to: B= 0.25 +0.15+2 T, for time t given in seconds. The coil is centered on the x-axis and the magnetic field is oriented at an angle of 30° from y-axis, as shown in the adjoining figure. (1) Determine the current induced in the coil at t = 1.5 s. (6 marks) Eur
At t = 1.5 s, the current induced in the coil is approximately -0.0825π A. We have a circular coil with 50 loops and a radius of 10 cm, connected to a resistance of 1.00 Ω.
The coil is positioned in a uniform magnetic field that varies with time according to B = (0.25t + 0.15t^2 + 2) T, where t is in seconds. The magnetic field is oriented at an angle of 30° from the y-axis. We need to determine the current induced in the coil at t = 1.5 s.
To find the current induced in the coil, we can use Faraday's law of electromagnetic induction, which states that the induced electromotive force (EMF) is equal to the rate of change of magnetic flux through the coil:
EMF = -dΦ/dt
The magnetic flux Φ through the coil can be calculated by multiplying the magnetic field B by the area of the coil. Since the coil is circular, the area is given by A = πr^2, where r is the radius.
At time t = 1.5 s, the magnetic field is given by B = (0.25(1.5) + 0.15(1.5)^2 + 2) T = 2.625 T.
The magnetic flux through the coil is then Φ = B * A = 2.625 T * (π(0.1 m)^2) = 0.0825π T·m².
Taking the derivative of the flux with respect to time, we get dΦ/dt = 0.0825π T·m²/s.
Substituting this value into the equation for the induced EMF, we have:
EMF = -dΦ/dt = -0.0825π T·m²/s.
Since the coil is connected to a resistance of 1.00 Ω, the current induced in the coil can be calculated using Ohm's Law: I = EMF/R.
Substituting the values, we find:
I = (-0.0825π T·m²/s) / 1.00 Ω = -0.0825π A.
Therefore, at t = 1.5 s, the current induced in the coil is approximately -0.0825π A.
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a helicopter drop a package down at a constant speed 5m/s. When the package at 100m away from the helicopter, a stunt person fall out the helicopter. How long he catches the package? How fast is he?
In a planned stunt for a movie, a supply package with a parachute is dropped from a stationary helicopter and falls straight down at a constant speed of 5 m/s. A stuntperson falls out the helicopter when the package is 100 m below the helicopter. (a) Neglecting air resistance on the stuntperson, how long after they leave the helicopter do they catch up to the package? (b) How fast is the stuntperson going when they catch up? 2.) In a planned stunt for a movie, a supply package with a parachute is dropped from a stationary helicopter and falls straight down at a constant speed of 5 m/s. A stuntperson falls out the helicopter when the package is 100 m below the helicopter. (a) Neglecting air resistance on the stuntperson, how long after they leave the helicopter do they catch up to the package? (b) How fast is the stuntperson going when they catch up?
The stuntperson catches up to the package 20 seconds after leaving the helicopter.The stuntperson is traveling at a speed of 25 m/s when they catch up to the package.
To determine the time it takes for the stuntperson to catch up to the package, we can use the fact that the package is falling at a constant speed of 5 m/s. Since the stuntperson falls out of the helicopter when the package is 100 m below, it will take 20 seconds (100 m ÷ 5 m/s) for the stuntperson to reach that point and catch up to the package.
In this scenario, since the stuntperson falls straight down without any horizontal motion, they will have the same vertical velocity as the package. As the package falls at a constant speed of 5 m/s, the stuntperson will also have a downward velocity of 5 m/s.
When the stuntperson catches up to the package after 20 seconds, their velocity will still be 5 m/s, matching the speed of the package. Therefore, the stuntperson is traveling at a speed of 25 m/s (5 m/s downward speed plus the package's 20 m/s downward speed) when they catch up to the package.
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Explain why and can have magnitudes higher than the magnitude of the input source voltage when circuit 2 is at (or close to) resonance.
In an electrical circuit, the phenomenon of having a voltage magnitude higher than the input source voltage is known as resonance amplification. Resonance occurs when the frequency of the input source matches the natural frequency of the circuit.
To understand why the voltage across certain elements, such as an inductor (L) or a capacitor (C), can have magnitudes higher than the input source voltage at or near resonance, we need to consider the behavior of these elements at different frequencies.
Inductor (L): An inductor has reactance that is directly proportional to the frequency of the input signal. At resonance, the inductive reactance cancels out the capacitive reactance in the circuit, resulting in a net low impedance across the inductor. As a result, the inductor draws maximum current from the source, leading to an increased voltage across it.
Capacitor (C): A capacitor has reactance that is inversely proportional to the frequency of the input signal. At resonance, the capacitive reactance cancels out the inductive reactance in the circuit, resulting in a net low impedance across the capacitor. As a result, the capacitor draws maximum current from the source, leading to an increased voltage across it.
When both the inductive and capacitive elements in a circuit are at resonance, they effectively create a low impedance path for the current. As a result, the current flowing through the circuit can be significantly larger than the current provided by the source alone.
According to Ohm's Law (V = I * Z), where V is the voltage, I is the current, and Z is the impedance, a higher current through a low impedance element can result in a higher voltage across that element. Therefore, the inductor or capacitor at resonance can exhibit a voltage magnitude higher than the input source voltage.
It is important to note that this resonance amplification phenomenon occurs only when the circuit is at or near resonance, where the frequencies match. At other frequencies, the impedance of the inductor and capacitor does not cancel out, and the voltage across them is determined by the input source voltage and the circuit's impedance characteristics.
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Problem 4. (5 points) The side (s) of a cube was measured as 2.6 + 0.01 cm. If the volume of the cube is given by V = s3 and the nominal value for the volume is calculated as 17.58 cm", what is the uncertainty in the volume of the cube expressed in cm3?
the uncertainty in the volume of the cube expressed in cm³ is 0.20219 cm³.
Given that the length of the side of a cube, s = 2.6 + 0.01 cm
Nominal value for the volume of the cube = V = s³ = (2.6 + 0.01)³ cm³= (2.61)³ cm³ = 17.579481 cm³
The absolute uncertainty in the measurement of the side of a cube is given as
Δs = ±0.01 cm
Using the formula for calculating the absolute uncertainty in a cube,
ΔV/V = 3(Δs/s)ΔV/V = 3 × (0.01/2.6)ΔV/V
= 0.03/2.6ΔV/V = 0.01154
The uncertainty in the volume of the cube expressed in cm³ is 0.01154 × 17.58 = 0.20219 cm³ (rounded off to four significant figures)
Therefore, the uncertainty in the volume of the cube expressed in cm³ is 0.20219 cm³.
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An ideal gas of 3 moles expands at a constant temperature of 450
K from a volume of 100 cm3 to a volume of 250 cm3. Determine the
change in entropy.
The change in entropy of the ideal gas is approximately 22.56 J/K. The change in entropy is calculated using the formula ΔS = nR ln(V2/V1).
ΔS represents the change in entropy, n is the number of moles of the gas, R is the ideal gas constant, and V1 and V2 are the initial and final volumes of the gas, respectively. In this case, we have 3 moles of the gas, an initial volume of 100 cm³, and a final volume of 250 cm³. By substituting these values into the formula and performing the necessary calculations, the change in entropy is determined to be approximately 22.56 J/K. Entropy is a measure of the degree of disorder or randomness in a system. In the case of an ideal gas, the change in entropy during an expansion process can be calculated based on the change in volume. As the gas expands from an initial volume of 100 cm³ to a final volume of 250 cm³, the entropy increases. This increase in entropy is a result of the gas molecules occupying a larger volume and having more available microstates. The formula for calculating the change in entropy, ΔS = nR ln(V2/V1), captures the relationship between the change in volume and the resulting change in entropy. The natural logarithm function in the formula accounts for the exponential nature of the relationship.
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In lightning storms, the potential difference between the Earth and the bottom of the thunderclouds can be as high as
40,000,000 V. The bottoms of the thunderclouds are typically 1500 m above the Earth, and can have an area of 150 km2
For the purpose of this problem, model the Earth-cloud system as a huge parallel-plate capacitor.
Calculate the capacitance of the Earth-cloud system.
The capacitance of the Earth-cloud system can be calculated as follows: The capacitance of a parallel-plate capacitor is given by: C = εA/where C is the capacitance, ε is the permittivity of free space, A is the area of each plate, and d is the distance between the plates.
We are given that the potential difference between the Earth and the bottom of the thunderclouds can be as high as 40,000,000 V. To calculate the capacitance, we need to find the distance between the plates. To do that, we can use the height of the cloud and the radius of the cloud. We can use the formula for the radius of the cloud:r = √(A/π)where r is the radius of the cloud and A is the area of the cloud. Substituting the given values:r = √(150 km²/π) = 6.17 km
The distance between the Earth and the bottom of the cloud is the hypotenuse of a right triangle with the height of the cloud as one side and the radius of the cloud as the other side. Using the Pythagorean theorem:
d = √(r² + h²)
where d is the distance between the plates, r is the radius of the cloud, and h is the height of the cloud.
Substituting the given values:
d = √(6.17 km)² + (1.5 km)²
= √(38.2 km²)
= 6.18 km
Now we can calculate the capacitance:
C = εA/substituting the given values:
C = (8.85 x 10^-12 F/m)(150 km²/6.18 km)
C = 2.15 x 10^6
Thus, the capacitance of the Earth-cloud system is 2.15 x 10^6 F.
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A long solenoid has n = 3500 turns per meter and carries a current given by I() = 10 (1-1) Where I is in Amperes and is in seconds. Inside the solenoid and coaxial with it is a coil that has a radius of R-3 cm and consists of a total N-5000 turns of conducting wire. #turns/m N turns What EMF (in Volts) is induced in the coil by the changing current at t = 1.1 s?
The induced EMF in the coil at t = 1.1 s is 1.1 V. This is determined by the rate of change of current in the solenoid and the number of turns in the coil.
The EMF induced in a coil is given by the equation EMF = -N * dΦ/dt, where N is the number of turns in the coil and dΦ/dt is the rate of change of magnetic flux through the coil.
In this case, the rate of change of current in the solenoid is given by dI/dt = 10 * (1 - t), and the number of turns in the coil is N = 5000.
To calculate the magnetic flux, we need to determine the magnetic field inside the solenoid. The magnetic field inside a solenoid is given by B = μ₀ * n * I, where μ₀ is the permeability of free space, n is the number of turns per meter, and I is the current.
Substituting the values into the equation, we get B = (4π * 10^(-7) * 3500 * 10 * (1 - t)) T.
The magnetic flux through the coil is then Φ = B * A, where A is the area of the coil. Since the coil is coaxial with the solenoid, the area is given by A = π * R².
Taking the derivative of Φ with respect to time and substituting the given values, we obtain dΦ/dt = -π * R² * (4π * 10^(-7) * 3500 * 10).
Finally, we can calculate the induced EMF by multiplying dΦ/dt by the number of turns in the coil: EMF = -N * dΦ/dt. Plugging in the values, we find that the induced EMF at t = 1.1 s is 1.1 V.
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Suppose that a spacecraft of mass 6.9 x 10^4 kg at rest in space fires its rocket X achieve a speed of 5.2 x 10^3 m/s. How much work has the fuel done on the spacecraft?
The work done by the fuel of the spacecraft to achieve a speed of 5.2 x 10³ m/s is 9.15 x 10¹¹ J.
The question here is how much work has the fuel done on a spacecraft that is at rest in space when it fires its rocket X to achieve a speed of 5.2 x 10³ m/s.
The mass of the spacecraft is 6.9 x 10⁴ kg. Let us begin by finding the initial kinetic energy of the spacecraft when it was at rest.
Kinetic energy is given by K.E. = 1/2 m(v²),
where m is mass and v is velocity. So, for the spacecraft at rest, v = 0, thus its kinetic energy would be zero as well.Initial kinetic energy, K.E. = 1/2 x 6.9 x 10⁴ x 0² = 0
When the spacecraft fires its rocket X, it acquires a velocity of 5.2 x 10³ m/s.
The final kinetic energy of the spacecraft after it has acquired its speed is given by;
K.E. = 1/2 m(v²) = 1/2 x 6.9 x 10⁴ x (5.2 x 10³)² = 9.15 x 10¹¹ J
The work done by the fuel of the spacecraft is the difference between its final and initial kinetic energies.
Work done by the fuel = Final kinetic energy - Initial kinetic energy = 9.15 x 10¹¹ J - 0 = 9.15 x 10¹¹ J
Therefore, the work done by the fuel of the spacecraft is 9.15 x 10¹¹ J.
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A block of mass is attached to a spring with a spring constant and can move frictionlessly on a horizontal surface. The block is pulled out to the side a distance from the equilibrium position, and a starting speed is given to the left as it is released. Determine the maximum speed the block gets?
The maximum speed the block gets can be determined using the principle of conservation of mechanical energy. The maximum speed occurs when all potential energy is converted to kinetic energy.
When the block is pulled out to the side and released, it starts oscillating back and forth due to the restoring force provided by the spring. As it moves towards the equilibrium position, its potential energy decreases and is converted into kinetic energy. At the equilibrium position, all the potential energy is converted into kinetic energy, resulting in the maximum speed of the block.
According to the principle of conservation of mechanical energy, the total mechanical energy of the system (block-spring) remains constant throughout the motion. The mechanical energy is the sum of the potential energy (associated with the spring) and the kinetic energy of the block.
At the maximum speed, all the potential energy is converted into kinetic energy, so we can equate the potential energy at the starting position (maximum displacement) to the kinetic energy at the maximum speed. This gives us the equation:
(1/2)kx^2 = (1/2)mv^2
Where k is the spring constant, x is the maximum displacement from the equilibrium position, m is the mass of the block, and v is the maximum speed.
By rearranging the equation and solving for v, we can determine the maximum speed of the block.
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An object slides horizontally off a table. initial speed = 5 m/s and h = 0.7 m. right before it lands on the ground, what is the magnitude of velocity?
The magnitude of the velocity right before the object lands on the ground is approximately 6.22 m/s.
To determine the magnitude of velocity right before the object lands on the ground, we can use the principles of projectile motion. Given the initial speed (v₀) and the height (h), we can calculate the final velocity (v) using the following equation:
v² = v₀² + 2gh
where g is the acceleration due to gravity (approximately 9.8 m/s²).
Let's substitute the given values into the equation:
v² = (5 m/s)² + 2 * 9.8 m/s² * 0.7 m
v² = 25 m²/s² + 13.72 m²/s²
v² = 38.72 m²/s²
Taking the square root of both sides to solve for v:
v = √(38.72 m²/s²)
v ≈ 6.22 m/s
Therefore, the magnitude of the velocity right before the object lands on the ground is approximately 6.22 m/s.
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Question 26 of 26 < > - / 30 View Policies Current Attempt in Progress A funny car accelerates from rest through a measured track distance in time 56 s with the engine operating at a constant power 270 kW. If the track crew can increase the engine power by a differential amount 1.0 W, what is the change in the time required for the run? Number i Units
The change in the time required for the run is given by Δt = (t / 270000) units, where t represents the new time required for the run.
A funny car accelerates from rest through a measured track distance in time 56 s with the engine operating at a constant power 270 kW. If the track crew can increase the engine power by a differential amount 1.0 W.
Formula used:
Power = Work done / Time
So, the work done by engine can be given as:
Work = Power × Time
Thus,
Time = Work / Power
Initial Work done by the engine:W₁ = 270 kW × 56 s
New Work done by the engine after changing the engine power by a differential amount:
W₂ = (270 kW + 1 W) × t where t is the new time required for the run
Change in the work done by the engine:
ΔW = W₂ - W₁ΔW = [(270 kW + 1 W) × t] - (270 kW × 56 s)ΔW = 1 W × t
The time required for the run would change by Δt given as:
Δt = ΔW / 270 kWΔt = (1 W × t) / (270 kW)Δt = (t / 270000 s) units (ii)
Therefore, the change in the time required for the run is (t / 270000) units.
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As viewed from the Earth, the Moon subtends an angle of approximately 0.50°. What is the diameter of the Moon's image that is produced by the objective of the Lick Observatory refracting telescope which has a focal length of 18 m?
As the height of the object (Moon) is not given, we need additional information to calculate the diameter of the image accurately.
To determine the diameter of the Moon's image produced by the refracting telescope, we can use the formula for angular magnification:
Magnification = (θ_i / θ_o) = (h_i / h_o)
Where:
θ_i is the angular size of the image,
θ_o is the angular size of the object,
h_i is the height of the image, and
h_o is the height of the object.
In this case, the angular size of the Moon (θ_o) is given as 0.50°.
The angular size of the image (θ_i) can be calculated using the formula:
θ_i = (d_i / f)
Where:
d_i is the diameter of the image, and
f is the focal length of the telescope.
Rearranging the formula for angular magnification, we have:
d_i = (θ_i / θ_o) * h_o
Substituting the given values:
θ_o = 0.50° = 0.50 * (π/180) radians
f = 18 m
Since the height of the object (Moon) is not given, we need additional information to calculate the diameter of the image accurately.
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Each of the statments below may or may not be true. Enter the letters corresponding to all the true statements. (Give ALL correct answers, i.e., B, AC, BCD...) In the two-slit experiment, yl, the distance from the central maximum from the first bright spot ... A) decreases if the screen is moved away from the slits. B) doesn't depend on the slit separation. C) is always an integer multiple of the wavelength of the light. D) does not depend on the frequency of the light. E) is larger for blue light than for violet light.
The true statements from the given options are: B) Doesn't depend on the slit separation C) Is always an integer multiple of the wavelength of the light. D) Does not depend on the frequency of the light.
A) The distance yl from the central maximum to the first bright spot, known as the fringe width or the distance between adjacent bright fringes, is determined by the slit separation. Therefore, statement A is false. B) The distance yl is independent of the slit separation. It is solely determined by the wavelength of the light used in the experiment. As long as the wavelength remains constant, the distance yl will also remain constant. Hence, statement B is true. C) The distance yl between adjacent bright fringes is always an integer multiple of the wavelength of the light. This is due to the interference pattern created by the two slits, where constructive interference occurs at these specific distances. Therefore, statement C is true. D) The distance yl does not depend on the frequency of the light. The fringe separation is solely determined by the wavelength, not the frequency. As long as the wavelength remains constant, the distance yl remains the same. Hence, statement D is true. E) The statement about the comparison of yl for blue light and violet light is not provided in the given options, so we cannot determine its truth or falsity based on the given information. In summary, the true statements are B) Doesn't depend on the slit separation, C) Is always an integer multiple of the wavelength of the light, and D) Does not depend on the frequency of the light.
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For all parts, show the equation you used and the values you substituted into the equation, with units with all numbers, in addition to your answer.Calculate the acceleration rate of the Jeep Grand Cherokee in feet/second/second or ft/s2.
Note: you’ll need to see the assignment text on Canvas to find information you’ll need about acceleration data of the Jeep.
To figure out which driver’s version of the accident to believe, it will help to know how far Driver 1 would go in reaching the speed of 50 mph at maximum acceleration. Then we can see if driver 2 would have had enough distance to come to a stop after passing this point. Follow the next steps to determine this.
Calculate how much time Driver 1 would take to reach 50 mph (73.3 ft/s) while accelerating at the rate determined in part 1. Remember that the acceleration rate represents how much the speed increases each second.
See page 32 of the text for information on how to do this.
Next we need to figure out how far the car would travel while accelerating at this rate (part 1) for this amount of time (part 2). You have the data you need. Find the right equation and solve. If you get stuck, ask for help before the assignment is overdue.
See page 33 for an example of how to do this.
Now it’s time to evaluate the two driver's stories. If driver 2 passed driver 1 after driver 1 accelerated to 50 mph (73.3 ft/s), he would have to have started his deceleration farther down the road from the intersection than the distance calculated in part 3. Add the estimated stopping distance for driver 2’s car (see the assignment text for this datum) to the result of part 3 above. What is this distance?
Which driver’s account do you believe and why?
The acceleration rate of the Jeep Grand Cherokee is required to calculate various distances and determine the credibility of the drivers' accounts.
First, the acceleration rate is determined using the given data. Then, the time taken by Driver 1 to reach 50 mph is calculated. Using this time, the distance traveled during acceleration is found. Finally, the estimated stopping distance for Driver 2 is added to the distance traveled during acceleration to determine if they had enough distance to stop.
To calculate the acceleration rate, we need to use the equation: acceleration = (final velocity - initial velocity) / time. Since the initial velocity is not given, we assume it to be 0 ft/s. Let's assume the acceleration rate is denoted by 'a'.
Given:
Initial velocity (vi) = 0 ft/s
Final velocity (vf) = 73.3 ft/s
Time (t) = 5.8 s
Using the equation, we can calculate the acceleration rate:
a = (vf - vi) / t
= (73.3 - 0) / 5.8
= 12.655 ft/s^2 (rounded to three decimal places)
Next, we calculate the time taken by Driver 1 to reach 50 mph (73.3 ft/s) using the acceleration rate determined above. Let's denote this time as 't1'.
Using the equation: vf = vi + at, we can rearrange it to find time:
t1 = (vf - vi) / a
= (73.3 - 0) / 12.655
= 5.785 s (rounded to three decimal places)
Now, we calculate the distance traveled during acceleration by Driver 1. Let's denote this distance as 'd'.
Using the equation: d = vi*t + (1/2)*a*t^2, where vi = 0 ft/s and t = t1, we can solve for 'd':
d = 0*t1 + (1/2)*a*t1^2
= (1/2)*12.655*(5.785)^2
= 98.9 ft (rounded to one decimal place)
Finally, to evaluate Driver 2's account, we add the estimated stopping distance for Driver 2 to the distance traveled during acceleration by Driver 1. Let's denote the estimated stopping distance as 'ds'.
Given: ds = 42 ft (estimated stopping distance for Driver 2)
Total distance required for Driver 2 to stop = d + ds
= 98.9 + 42
= 140.9 ft
Based on the calculations, if Driver 2 passed Driver 1 after Driver 1 accelerated to 50 mph, Driver 2 would need to start deceleration farther down the road than the distance calculated (140.9 ft). Therefore, it seems more likely that Driver 1's account is accurate.
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