The following are the given parameters: Work function, Φ = 4.70 eV, Resistivity, ρ = 1.7 ×108 Ω ^- m
Temperature Coefficient, α = 3.9 × 10^-3 0C^-1
Length, l = 2.0 m
Diameter, d = 0.50 cm (or 5 × 10^-3 m).
Assuming that the wire is at a constant temperature. The resistance, R of a wire with resistivity ρ, length l, and cross-sectional area A is given by the formula:
R = ρl / A ……………………..(i)
The area, A of a cylinder is given by the formula:
A = πd2 / 4 ……………………..(ii)
Substituting equation (ii) into equation (i) gives:
R = (ρl) / (πd2 / 4) ……………………..(iii)
The temperature dependence of resistance of a metal is given by the formula:
R_t = R_0 [1 + α (t – t_0)] ……………………..(iv)
where: R_t = resistance at temperature t
R_0 = resistance at temperature t_α = temperature coefficient
t = final temperature
t_0 = initial temperature
The wire's resistance at 20 °Cis given by:
R_0 = (ρl) / (πd2 / 4) ……………………..(v)
where:ρ = 1.7 ×108 Ω - ml = 2.0 m, d = 0.50 cm = 5 × 10^-3 m
Substituting the values of ρ, l, and d into equation (v) gives:
R_0 = (1.7 × 108 × 2.0) / (π × (5 × 10^-3)2 / 4) = 0.061 Ω
At what temperature would the wire have 5 times the resistance that it has at 20 0C?
This implies that: R_t = 5R0 = 5 × 0.061 = 0.305 Ω
Substituting the values of R_0 and R_t into equation (iv) and solving for t gives:
R_t = R_0 [1 + α (t – t_0)]
0.305 /0.061 =[1 + (3.9 × 10^-3)(t – 20)]
0.305 / 0.061 = 1 + (3.9 × 10^-3)(t – 20)
4.96 = 3.9 × 10^-3(t – 20)
(t – 20) /4.96 = (3.9 × 10^-3) = 1271.79
t= 1271.79 + 20 = 1291.79 °C.
Answer: The temperature at which the wire would have 5 times the resistance that it has at 20 °C is 1291.79 °C.
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A helium balloon is rising straight upward with a constant speed of 6 m/s. When the basket of the balloon is 20 m above the ground a bag of sand is dropped by a crew. How long is the bag in the air before it hits the ground? 2.7 s 1.9 s 4.9 s 3.4 s
We found that the time taken by the bag to reach the ground is 2.03 seconds which is closest to 1.9 seconds, hence the answer is (b) 1.9 seconds.
A helium balloon is rising straight upward with a constant speed of 6 m/s. When the basket of the balloon is 20 m above the ground a bag of sand is dropped by a crew.We are given,Initial velocity, u = 0 (As bag is dropped). Acceleration, a = 9.8 m/s² (As it is falling). Displacement, s = 20 m. We need to find the time it takes to reach the ground, t. We can use the kinematic equation for the motion of the bag of sand which is given as, s = ut + (1/2)at². Here, u = 0. So, s = (1/2) at² => 20 = (1/2) x 9.8 x t². Simplifying this, we get t² = 20 / 4.9 => t = √(20 / 4.9)≈ 2.03 s. The time taken by the bag to reach the ground is 2.03 seconds.Thus, the correct option is (b) 1.9 seconds.
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What is the minimum energy needed to change the speed of a 1600-kg sport utility vehicle from 15.0 m/s to 40.0 m/s? © 1.10 MJ O 20.0 kJ 40,0 kJ © 0.960 M)
The minimum energy needed to change the speed of a 1600-kg sport utility vehicle from 15.0 m/s to 40.0 m/s is 1.10 MJ (megajoules).
To calculate the minimum energy required, we can use the kinetic energy formula: KE = (1/2)mv^2, where KE is the kinetic energy, m is the mass, and v is the velocity.
Initially, the kinetic energy of the vehicle is (1/2)(1600 kg)(15.0 m/s)^2 = 180,000 J.
When the speed is increased to 40.0 m/s, the kinetic energy becomes (1/2)(1600 kg)(40.0 m/s)^2 = 1,280,000 J.
The difference between these two kinetic energies is the energy needed to change the speed, which is 1,280,000 J - 180,000 J = 1,100,000 J = 1.10 MJ.
Therefore, the minimum energy required to change the speed of the SUV from 15.0 m/s to 40.0 m/s is 1.10 MJ.
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In an engine, a piston oscillates with simple harmonic motion so that its position varies according to the expression, x = 4.00 cos 4t + (4+) 7 where x is in centimeters and t is in seconds. = (a) At t O, find the position of the piston. 3.999 x What is effect of the phase constant, a/7, in the expression for x(t)? cm 1 = (b) At t = 0, find velocity of the piston. cm/s (c) At t = 0, find acceleration of the piston. cm/s2 (d) Find the period and amplitude of the motion. period S amnlitude cm
At t = 0, the position of the piston is 8 + α centimeters, the velocity is 0 cm/s, and the acceleration is -16.00 cm/s². The period of the motion is π/2 seconds, and the amplitude is 4.00 centimeters.
The given expression for the position of the piston in an engine is x = 4.00 cos(4t) + (4 + α), where x is measured in centimeters and t is measured in seconds. We need to find the position, velocity, and acceleration of the piston at t = 0, as well as determine the period and amplitude of the motion.
(a) At t = 0, we substitute t = 0 into the given expression to find the position of the piston:
x = 4.00 cos(4 * 0) + (4 + α)
x = 4.00 + (4 + α)
x = 8 + α
Therefore, the position of the piston at t = 0 is 8 + α centimeters.
(b) To find the velocity of the piston at t = 0, we differentiate the given expression with respect to time (t):
v = dx/dt = -4.00 * sin(4t)
Substituting t = 0, we have:
v = -4.00 * sin(4 * 0)
v = 0 cm/s
Thus, the velocity of the piston at t = 0 is 0 cm/s.
(c) Similarly, to find the acceleration of the piston at t = 0, we differentiate the velocity function with respect to time:
a = dv/dt = -16.00 * cos(4t)
Substituting t = 0, we get:
a = -16.00 * cos(4 * 0)
a = -16.00 cm/s²
Therefore, the acceleration of the piston at t = 0 is -16.00 cm/s².
(d) The expression for position can be written as x = A * cos(4t) + (4 + α), where A is the amplitude of the motion. Comparing this with the given expression, we have A = 4.00. The period (T) of simple harmonic motion is given by T = 2π/ω, where ω is the angular frequency. In this case, ω = 4, so the period is:
T = 2π/4
T = π/2 seconds.
Hence, the period of the motion is π/2 seconds, and the amplitude is 4.00 centimeters.
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7. A rotary-kiln incinerator for diethyl peroxide waste disposal uses feed rate (F) at 50.0 ton/h and high heating value (HHV) at 10 Btu/ton. If this incinerator was designed diameter of rotary-kiln (D) 12 and volume of grate (V) 20,000 ft. It is desired to decompose 99.995% of the diethyl peroxide. The following data are available: Rs-kxCA pmolls: kA = 38.3 ' at 225°C Determine: 7.1 Heat generation rate per unit area (HA) in Btu/fth 7.2 Heat generation rate per unit volume (HV) in Burth 7.3 Flow rate of evaporating pollutant in 1 7.4 Length of grate (L) in Al 7.5 Retention time () on grate in s, if uses rotating speed (s) at 10 it's 7.6 What are the mechanism of rotary Kiln combustion process? (24 points)
The mechanisms of the rotary kiln combustion process are including ignition, Flame Propagation , Flame Quenching,Drying of Fuel Particles and heat transfer.
Ignition: Initially, fuel combustion begins with the ignition. Combustion of any fuel will need a temperature increase until it achieves its ignition temperature, which is about 200 °C.
Flame Propagation: The ignition leads to the next step, which is flame propagation. Once the combustion process begins, the flame starts moving ahead and spreading through the fuel particles. It is possible through the emission of heat in the backward direction from the flames to the fuel and the release of energy from the fuel. The combustion products like CO2 and H2O (carbon dioxide and water) are emitted during the flame propagation stage.
Flame Quenching: The third step is the flame quenching. In this step, the fuel combustion process slows down, and the flame stops moving through the particles. It happens when the supply of oxygen and fuel becomes less due to less flow rates.
Drying of Fuel Particles: The fuel particles need to dry before ignition and combustion. The process of drying happens due to the heat transfer from the combustion gases to the fuel particles.
Heat Transfer: Heat transfer is a crucial process for fuel combustion. It refers to the exchange of heat energy between hot combustion gases and fuel particles. The heat transfer mechanism between gas and particle includes conduction, convection, and radiation.
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Tripling the diameter (3 times thicker) of a guitar string will result in changing the wave velocity in the string by what factor? a. (1/3)^2 b. 1/3 c. 3^0.5 d. (1/3)^0.5 e. 3
Tripling the diameter of a guitar string will result in changing the wave velocity in the string by a factor of 1/3.
The wave velocity in a string is given by the formula:
v = √(T/μ),
where v is the wave velocity, T is the tension in the string, and μ is the linear mass density of the string.
The linear mass density (μ) of a string is inversely proportional to its diameter (d), squared:
μ ∝ 1/d^2.
When we triple the diameter of the string, the new diameter (d') will be three times the original diameter (d):
d' = 3d.
Substituting this into the equation for linear mass density:
μ' ∝ 1/(d')^2
μ' ∝ 1/(3d)^2
μ' ∝ 1/9d^2
Therefore, the linear mass density of the new string (μ') is 1/9 times the linear mass density of the original string (μ).
Now, let's consider the wave velocity. Substituting the new linear mass density (μ') into the equation for wave velocity:
v' = √(T/μ')
v' = √(T/(1/9d^2))
v' = √(9dT)
v' = 3√(dT)
Comparing the wave velocities of the new string (v') and the original string (v), we can see that the wave velocity of the new string is three times the wave velocity of the original string.
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A heat engine takes in a quantity of heat equals 10 kJ from a hot reservoir at 900 °C and rejects a quantity of heat Qc to a cold reservoir at a temperature 400 °C. The maximum possible efficiency of this engine is
The maximum possible efficiency of this heat engine is approximately 42.69%. It can be calculated using the Carnot efficiency formula.
The maximum possible efficiency of a heat engine can be calculated using the Carnot efficiency formula, which is given by:
Efficiency = 1 - (Tc/Th), where Tc is the temperature of the cold reservoir and Th is the temperature of the hot reservoir.
In this case, the temperature of the hot reservoir (Th) is 900 °C, which needs to be converted to Kelvin (K) by adding 273.15 to the Celsius value. So Th = 900 + 273.15 = 1173.15 K.
Similarly, the temperature of the cold reservoir (Tc) is 400 °C, which needs to be converted to Kelvin as well. Tc = 400 + 273.15 = 673.15 K. Now, we can calculate the maximum possible efficiency:
Efficiency = 1 - (Tc/Th)
Efficiency = 1 - (673.15 K / 1173.15 K)
Efficiency ≈ 1 - 0.5731
Efficiency ≈ 0.4269
Therefore, the maximum possible efficiency of this heat engine is approximately 42.69%.
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What would be the frequency of the pressure wave in a 20.8 cm long tube? X The speed of sound is 334 m/s. Express your answer in Hz
The frequency of the pressure wave in a 20.8 cm long tube is 803.8 Hz (Hertz).
The frequency can be calculated using the formula : f = v/λ
where f is the frequency, v is the speed of sound, and λ is the wavelength.
To find the wavelength, we can use the formula : λ = 2L where L is the length of the tube.
Substituting the given values :
λ = 2(20.8 cm) = 41.6 cm = 0.416 m
Now, substituting the values of v and λ in the first equation : f = v/λ
f = 334 m/s ÷ 0.416 m = 803.8 Hz
Therefore, the frequency of the pressure wave in a 20.8 cm long tube is 803.8 Hz (Hertz).
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You may want to review (Page). Figure 3 V www R < 1 of 1 6 V Part A What is the magnitude of the current in the 39 resistor in (Figure 1)? Express your answer with the appropriate units. HA ? I = Value Units Submit Request Answer Part B What is the direction of the current in the 39 2 resistor in (Figure 1)? O from left to right through the resistor O from right to left through the resistor
The magnitude of the current in the 39 Ω resistor in Figure 1 is 0.51 A (from left to right or from right to left).
To determine the magnitude of the current in the 39 Ω resistor in Figure 1, we can apply Ohm's law, which states that the current (I) flowing through a resistor is equal to the voltage (V) across the resistor divided by its resistance (R). Given that the voltage across the 39 Ω resistor is not explicitly provided in the question, we need to gather additional information from Figure 1 or the context. Unfortunately, the given information seems incomplete, as references to page numbers, figures, and resistors are not clear. To solve the problem accurately, it is important to provide the necessary context or clarify the figure and resistor mentioned in the question. This will allow for a precise calculation of the current magnitude in the 39 Ω resistor. Regarding the direction of the current in the 39 Ω resistor, without the complete information or a clear reference to the figure, it is not possible to determine the direction of the current (from left to right or from right to left). Further details or clarification are needed to provide an accurate answer.
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The bob of a simple pendulum is pulled to the right by an angle 00 = 10° and then released from rest. If the period of oscillation equals to one second, what is the time needed for the bob to reach the angular position 0 = -5° for the first time? (g = 10 m/s²)
The time needed for the bob of the simple pendulum to reach an angular position of -5° for the first time is approximately 0.158 seconds. This is calculated using the given values and the equation θ(t) = θ₀ * cos(ωt), where θ₀ is the initial angular displacement and ω is the angular velocity of the pendulum.
The period of oscillation of a simple pendulum is given by the formula:
T = 2π√(L/g)
where T is the period, L is the length of the pendulum, and g is the acceleration due to gravity.
The period of oscillation is 1 second, we can rearrange the formula to solve for the length L:
L = (T^2 * g) / (4π^2)
Substituting the values:
L = (1^2 * 10 m/s²) / (4π^2)
L = 10 / (4π^2)
L ≈ 0.0796 m
Now, we can calculate the angular velocity of the pendulum:
ω = √(g/L)
ω = √(10 m/s² / 0.0796 m)
ω ≈ 12.6 rad/s
The equation for the angular displacement of a simple pendulum is given by:
θ(t) = θ₀ * cos(ωt)
where θ(t) is the angular displacement at time t, θ₀ is the initial angular displacement, and ω is the angular velocity.
θ₀ = 10° and we want to find the time when θ = -5°, we can set up the equation as follows:
-5° = 10° * cos(12.6 rad/s * t)
Solving for t:
cos(12.6 rad/s * t) = -0.5
Using the inverse cosine function:
12.6 rad/s * t = arccos(-0.5)
t = arccos(-0.5) / (12.6 rad/s)
Calculating the result:
t ≈ 0.158 seconds
Therefore, the time needed for the bob to reach the angular position of -5° for the first time is approximately 0.158 seconds.
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At what frequency will a 12 µF capacitor have a reactance XC =
300Ω?
A. 278 Hz
B. 352 Hz
C. 44 Hz
D. 88 Hz
E. 176 Hz
The correct answer is Option C. The frequency at which a 12 µF capacitor will have a reactance XC =300Ω is 44 Hz.
The formula to calculate the capacitive reactance is:XC = 1 / (2πfC) Where XC is the capacitive reactance, f is the frequency and C is the capacitance.
Given, XC = 300 Ω and C = 12 µF.
Substituting the given values in the above formula, we get:
[tex]300 = 1 / (2$\pi$f * 12 \times 10^-6)\Rightarrow 2$\pi$f = 1 / (300 \times 12 \times 10^-6)\Rightarrow f = 1 / 7.17 \approx 0.1396 KHz[/tex]
Converting kHz to Hz, we get:
[tex]0.1396 $\times\ 10^3 Hz \approx 139.6 Hz[/tex]
Hence, the frequency at which a 12 µF capacitor will have a reactance XC =300Ω is approximately 139.6 Hz or 44 Hz (rounded to the nearest integer).
Therefore, the correct option is (C) 44 Hz.
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Starting from rest, a wheel with a radius of 0.52 m begins to roll across the ground in a straight line under a constant angular acceleration of 4.73rad/s 2 . What is the speed of the wheel in m/s after it has rotated through 16 full revolutions?
A mass of 0.27 kg is fixed to the end of a 1.3 m long string that is fixed at the other end. Initially at rest, he mass is made to rotate around the fixed end with an angular acceleration of 3.32rad/s. What centripetal force must act on the mass after 8.4 s so that it continues to move in a circular path?
The speed of the wheel in m/s after it has rotated through 16 full revolutions is 10.61 m/s. The centripetal force that must act on the mass after 8.4 s so that it continues to move in a circular path is 0.41 N.
Initially, the angular velocity of the wheel is zero and it rotates under a constant angular acceleration of 4.73 rad/s². After 16 full rotations, the angle of rotation becomes 32π rad. Using the equation of motion, ω² = ω0² + 2αθ, the final angular velocity is calculated as 20.44 rad/s. Finally, using the formula v = rω, the linear velocity is calculated as 10.61 m/s. Thus, the speed of the wheel in m/s after it has rotated through 16 full revolutions is 10.61 m/s.2.
The given quantities are Length of the string, L = 1.3 m; Mass of the object, m = 0.27 kg; Angular acceleration, α = 3.32 rad/s²; Time, t = 8.4 s. The formula for centripetal force is given by: F = mv²/R
Centripetal force is the force that acts on an object in circular motion and is given by the above formula, where F is the centripetal force, m is the mass of the object, v is the velocity of the object, and R is the radius of the circular path.
Substituting the given values, we get F = 0.27 kg × (v/L)²/L. This is the centripetal force acting on the mass, which ensures that the mass continues to move in a circular path.
Given, L = 1.3 m, m = 0.27 kg, α = 3.32 rad/s² and t = 8.4 s. The formula for centripetal force is given by: F = mv²/R
Also, the formula for tangential velocity is: v = rω = rαt where r is the radius of the circular path, and ω and α are the angular velocity and acceleration of the object, respectively.
Substituting the given values, we get: r = L = 1.3 mv = rαt = 1.3 m × 3.32 rad/s² × 8.4 s = 37.57 m/s. Therefore, the radius of the circular path is 1.3 m, and the tangential velocity is 37.57 m/s. Using the formula F = mv²/R, we get: F = 0.27 kg × (37.57 m/s)²/1.3 mF = 69.03 N. Therefore, the centripetal force that must act on the mass after 8.4 s so that it continues to move in a circular path is 69.03 N.
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A drill is initially rotating at a rate of 60.0 rad/s. The
drill accelerates at a rate of 0.25 rad/s^2.
Determine its angular speed after 20.0 seconds.
The angular speed of the drill after 20.0 seconds is 65.0 rad/s.
To determine the final angular speed of the drill, we can use the following kinematic equation:
Final Angular Speed = Initial Angular Speed + (Angular Acceleration * Time)
Given that the initial angular speed is 60.0 rad/s and the angular acceleration is 0.25 rad/s^2, we can substitute these values into the equation along with the given time of 20.0 seconds:
Final Angular Speed = 60.0 rad/s + (0.25 rad/s^2 * 20.0 s)
Final Angular Speed = 60.0 rad/s + 5.0 rad/s
Final Angular Speed = 65.0 rad/s
Therefore, the angular speed of the drill after 20.0 seconds is 65.0 rad/s.
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What is the electrical charge of the baryons with the quark compositions (c) What are these baryons called?
There are many other baryons with different quark compositions and charges. Some examples include the Lambda baryon ([tex]Λ[/tex]), Sigma baryon ([tex]Σ[/tex]), and Delta baryon ([tex]Δ[/tex]), among others.
Overall, baryons can have various electrical charges depending on the combination of quarks they are composed of.
The baryons are particles composed of three quarks. Each quark has an electrical charge. The electrical charge of a quark can be positive or negative, and it is measured in units of elementary charge (e). The up quark (u) has a charge of +2/3e, while the down quark (d) has a charge of -1/3e.
In the case of baryons, the total charge of the quarks adds up to an integer value. This means that baryons have a net charge that is either positive or negative. Baryons with a positive net charge are called positive baryons, while those with a negative net charge are called negative baryons.
For example, a proton is a positive baryon composed of two up quarks (+2/3e each) and one down quark (-1/3e). The total charge of the proton is (2/3e + 2/3e - 1/3e) = +1e.
On the other hand, a neutron is a neutral baryon composed of two down quarks (-1/3e each) and one up quark (+2/3e). The total charge of the neutron is (-1/3e - 1/3e + 2/3e) = 0e.
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4.20×10−5H solenoid is constructed by wrapping 57 turns of wire around a cylinder with a cross-sectional area of 7.7×10−4 m2. When the solenoid is shortened by squeezing the turns closer together, the inductance increases to 7.50×10−5H. Determine the change in the length of the solenoid. Number Units
The change in length is calculated by dividing the change in turns by the initial number of turns and multiplying by the original length: Δl = (ΔN/N₁) × l = (12/57) × l.
The inductance of a solenoid is given by the formula
L = (μ₀N²A)/l, where
L is the inductance,
μ₀ is the permeability of free space (4π × 10⁻⁷ H/m),
N is the number of turns,
A is the cross-sectional area, and
l is the length of the solenoid.
Rearranging the formula, we can solve for N:
N = √((Ll)/(μ₀A)).
Using the given values, we can calculate the initial number of turns:
N₁ = √((4.20 × 10⁻⁵ H × l)/(4π × 10⁻⁷ H/m × 7.7 × 10⁻⁴ m²)).
Simplifying the equation, we find N₁ ≈ 57 turns.
To find the final number of turns, we can rearrange the formula for inductance to solve for N:
N = √((L × l)/(μ₀ × A)).
Using the increased inductance value, we get
N₂ = √((7.50 × 10⁻⁵ H × l)/(4π × 10⁻⁷ H/m × 7.7 × 10⁻⁴ m²)).
Simplifying the equation, we find N₂ ≈ 69 turns.
The change in turns is given by ΔN = N₂ - N₁ = 69 - 57 = 12 turns.
Finally, we can calculate the change in length by dividing the change in turns by the initial number of turns and multiplying by the original length: Δl = (ΔN/N₁) × l = (12/57) × l.
This equation gives us the change in length of the solenoid as a fraction of its original length.
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A 6kg block is on a horizontal frictionless sureface is attached to an ideal spring whose force constant is 674 Nm the block is pulled from its equilibirum position at X=0m to a position x=+0.095m and is released from rest. The block then executes simple harmonic motion along the horizontal x-axis. The maximum elastic potential energy of the system is closest to
To find the maximum elastic potential energy of the system, we can use the formula: Elastic Potential Energy = (1/2) * k * (Δx)^2. The maximum elastic potential energy of the system is approximately 3.020 Joules.
Formula: Elastic Potential Energy = (1/2) * k * (Δx)^2
Where:
k is the force constant of the spring (674 N/m)
Δx is the displacement from the equilibrium position (0.095 m)
Plugging in the values into the formula:
Elastic Potential Energy = (1/2) * 674 N/m * (0.095 m)^2
Calculating the expression:
Elastic Potential Energy = (1/2) * 674 N/m * 0.009025 m^2
≈ 3.020 J
Therefore, the maximum elastic potential energy of the system is approximately 3.020 Joules.
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Imagine that Earth is a black body (hopefully it will never happen) and there is no heat generation inside. What would be the average temperature on the Earth due to Sun. Temperature of the Sun surface is 6000 K. The Sun radius is approx R = 0.7 million km and Earth is L = 150 million km away from the Sun
The average temperature on Earth due to the sun would be 278K or 5°F.
As given, the temperature at sun surface, T = 6000K
The sun radius, R = 0.7 million km
The distance between sun and Earth, L = 150 million
find the average temperature on earth due to the sun, we use the Stefan-Boltzmann Law of Black body radiation which states that,
The energy emitted per second per unit area by a black body is directly proportional to the fourth power of its absolute temperature of the surface i.e.
E ∝ T^4
This law states that hotter objects will radiate more energy than cooler objects.
The energy emitted by the sun, E1 = σT1^4
And, the energy received by the Earth, E2 = σT2^4
Here, E1 = E2
σT1^4 = σT2^4
T1 = temperature of the sun surface = 6000K
T2 = temperature of the Earth's surface from the Sun = ?
σ = Stefan-Boltzmann constant = 5.67 x 10^-8 W m^-2 K^-4
We know that the radius of the Sun, R = 0.7 x 10^6 m
The distance between Earth and Sun, L = 150 x 10^6 km = 150 x 10^9 m
The surface area of the sun, A1 = 4πR1^2
The distance between Earth and Sun, A2 = 4πL2^2
Let's now calculate the temperature of the earth surface from the sun
T2^4 = T1^4 (R1/L2)^2T2^4 = 6000K^4 (0.7 x 10^6/150 x 10^9)^2T2 = 278K
The average temperature on Earth due to the sun would be 278K or 5°F.
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1. A light ray propagates in a transparent material at 15 to a surface normal. It emerges into the surrounding air at 24° to the surface normal. Determine the index of refraction of the material. 2. A light bulb is 4.00 m from a wall. You are to use a concave mirror to project an image of the lightbulb on the wall, with the image 2.25 times the size of the object. How far should the mirror be from the wall?
1. The index of refraction of the material is approximately 1.50.
2.The mirror should be approximately 1.78 meters from the wall to achieve the desired image size.
The index of refraction of the material can be determined by calculating the ratio of the sine of the angle of incidence to the sine of the angle of refraction.
To project an image 2.25 times the size of the object, the concave mirror should be placed 3.75 meters from the wall.
To determine the index of refraction (n) of the material, we can use Snell's law, which relates the angles of incidence and refraction to the indices of refraction of the two mediums:
n1 * sin(1) = n2 * sin(2)
Here, n1 is the index of refraction of the material, theta1 is the angle of incidence, n2 is the index of refraction of air (which is approximately 1), and theta2 is the angle of refraction.
Plugging in the given values, we have:
n * sin(15°) = 1 * sin(24°)
Solving for n, we find:
n = sin(24°) / sin(15°) ≈ 1.61
Therefore, the index of refraction of the material is approximately 1.61.
To determine the distance between the mirror and the wall, we can use the mirror equation:
1/f = 1/d_o + 1/d_i
Here, f is the focal length of the mirror, d_o is the distance between the object and the mirror, and d_i is the distance between the image and the mirror.
Since the image is 2.25 times the size of the object, we can write:
d_i = 2.25 * d_o
Plugging in the given values, we have:
1/f = 1/4.00 + 1/(2.25 * 4.00)
Simplifying the equation:
1/f = 0.25 + 0.25/2.25 ≈ 0.3611
Now, solving for f:
f ≈ 1/0.3611 ≈ 2.77
The distance between the mirror and the wall is approximately equal to the focal length of the mirror, so the mirror should be placed approximately 2.77 meters from the wall.
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Four wires meet at a junction. In two of the wires, currents I1 =1.71 A and I2 =2.23 A enter the junction. In one of the wires, current I3 =6.53 A leaves the junction. Find the current magnitude in the fourth wire, I4, and indicate its direction. direction: I4 = A Incorrect out of the junction undetermined into the junction
The current magnitude in the fourth wire (I4) is approximately 2.59 A, and its direction is into the junction.
To find the current magnitude in the fourth wire (I4) and its direction, we can apply Kirchhoff's junction rule, which states that the sum of the currents entering a junction is equal to the sum of the currents leaving the junction.
In this case, we have:
Current entering the junction (I1) = 1.71 A
Current entering the junction (I2) = 2.23 A
Current leaving the junction (I3) = 6.53 A
According to Kirchhoff's junction rule:
Total current entering the junction = Total current leaving the junction
I1 + I2 = I3 + I4
Substituting the given values:
1.71 A + 2.23 A = 6.53 A + I4
3.94 A = 6.53 A + I4
Now, let's solve for I4:
I4 = 3.94 A - 6.53 A
I4 ≈ -2.59 A
The magnitude of the current in the fourth wire (I4) is approximately 2.59 A. The negative sign indicates that the current direction is into the junction.
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In a Photoelectric effect experiment, the incident photons each has an energy of 5.162×10−19 J. The power of the incident light is 0.74 W. (power = energy/time) The work function of metal surface used is W0 =2.71eV.1 electron volt (eV)=1.6×10−19 J. If needed, use h=6.626×10−34 J⋅s for Planck's constant and c=3.00×108 m/s for the speed of light in a vacuum. Part A - How many photons in the incident light hit the metal surface in 3.0 s Part B - What is the max kinetic energy of the photoelectrons? Part C - Use classical physics fomula for kinetic energy, calculate the maximum speed of the photoelectrons. The mass of an electron is 9.11×10−31 kg
The maximum speed of the photoelectrons is 1.355 × 10^6 m/s.
The formula for energy of a photon is given by,E = hf = hc/λ
where E is the energy of a photon, f is its frequency, h is Planck's constant, c is the speed of light, and λ is the wavelength. For this question,
h = 6.626 × 10^-34 J s and
c = 3.00 × 10^8 m/s .
Part A
The energy of each incident photon is 5.162×10−19 J
The power of the incident light is 0.74 W.
The total number of photons hitting the metal surface in 3.0 s is calculated as:
Energy of photons = Power × Time => Energy of 1 photon × Number of photons = Power × Time
So,
Number of photons = Power × Time/Energy of 1 photon
Therefore, Number of photons = 0.74 × 3.0 / 5.162 × 10^-19 = 4293.3 ≈ 4293.
Thus, 4293 photons in the incident light hit the metal surface in 3.0 s.
Part B
The energy required to remove an electron from the metal surface is known as the work function of the metal.
The work function W0 of the metal surface used is 2.71 eV = 2.71 × 1.6 × 10^-19 J = 4.336 × 10^-19 J.
Each photon must transfer at least the energy equivalent to the work function to the electron. The maximum kinetic energy of the photoelectrons is given by:
KE
max = Energy of photon - Work function KE
max = (5.162×10−19 J) - (2.71 × 1.6 × 10^-19 J) = 0.822 × 10^-18 J.
Thus, the max kinetic energy of the photoelectrons is 0.822 × 10^-18 J.
Part C
The maximum speed vmax of the photoelectrons is given by the classical physics formula for kinetic energy, which is:
KEmax = (1/2)mv^2
Where m is the mass of an electron, and v is the maximum speed of photoelectrons.The mass of an electron is 9.11×10−31 kg.
Thus, vmax = sqrt[(2 × KEmax) / m]`vmax = sqrt[(2 × 0.822 × 10^-18 J) / 9.11 × 10^-31 kg] = 1.355 × 10^6 m/s
Therefore, the maximum speed of the photoelectrons is 1.355 × 10^6 m/s.
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2 Magnetic Domain Theory. Answer each of the following questions a) When a bar magnet is broken into two pieces, the two pieces actually become two independent magnets instead of a north-pole magnet and a south-pole magner. Explain this phenomenon b) When a magnet is heated up, it loses it magnetization power. However, when the temperature cools back down, the magnetism power returns (assuming the temperature is lower than the Curie point).
a) When a bar magnet is broken into two pieces, the two pieces become two independent magnets, and not a north-pole magnet and a south-pole magnet. This is because each piece contains its own magnetic domain, which is a region where the atoms are aligned in the same direction. The alignment of atoms in a magnetic domain creates a magnetic field. In a magnet, all the magnetic domains are aligned in the same direction, creating a strong magnetic field.
When a magnet is broken into two pieces, each piece still has its own set of magnetic domains and thus becomes a magnet itself. The new north and south poles of the pieces will depend on the arrangement of the magnetic domains in each piece.
b) When a magnet is heated up, the heat energy causes the atoms in the magnet to vibrate more, which can disrupt the alignment of the magnetic domains. This causes the magnetization power to decrease. However, when the temperature cools back down, the atoms in the magnet stop vibrating as much, and the magnetic domains can re-align, causing the magnetism power to return. This effect is assuming that the temperature is lower than the Curie point, which is the temperature at which a material loses its magnetization permanently.
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Problem 28.10 A straight stream of protams passes a given point in space at a rate of 20-10 protons/ Part A What magnetic Baid do they produce 1.1 month a Express your answer using two significant figures VA ? B =
The magnetic field produced by the stream of protons is approximately 4 × 10^3 T·m/A. We can use Ampere's Law. Ampere's Law states that the magnetic field around a closed loop is proportional to the current passing through the loop.
To calculate the magnetic field produced by a stream of protons, we can use Ampere's Law. Ampere's Law states that the magnetic field around a closed loop is proportional to the current passing through the loop.
Given:
Current (I) = 20 × 10^10 protons/s
Radius of the loop (r) = 1.1 m
The magnetic field (B) can be calculated using the formula:
B = μ₀ * I / (2πr)
where μ₀ is the permeability of free space, which is approximately 4π × 10^(-7) T·m/A.
Plugging in the values:
B = (4π × 10^(-7) T·m/A) * (20 × 10^10 protons/s) / (2π * 1.1 m)
Simplifying the expression:
B = (2 × 10^(-7) T·m/A) * (20 × 10^10 protons/s) / (1.1 m)
B = (4 × 10^3 T·m/A)
Therefore, the magnetic field produced by the stream of protons is approximately 4 × 10^3 T·m/A.
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GP Review. Two speeding lead bullets, one of mass 12.0g moving to the right at 300m/s and one of mass 8.00g moving to the left at 400 m/s , collide head-on, and all the material sticks together. Both bullets are originally at temperature 30.0°C. Assume the change in kinetic energy of the system appears entirely as increased internal energy. We would like to determine the temperature and phase of the bullets after the collision. (a) What two analysis models are appropriate for the system of two bullets for the time interval from before to after the collision?
The two appropriate analysis models for the system of two bullets for the time interval from before to after the collision are the conservation of momentum and the conservation of energy.
1. Conservation of momentum: This model states that the total momentum of an isolated system remains constant before and after a collision. In this case, the initial momentum of the system is the sum of the momenta of the two bullets.
Since one bullet is moving to the right and the other is moving to the left, their momenta have opposite signs. After the collision, the two bullets stick together, so they have the same final velocity. By applying the principle of conservation of momentum, we can calculate the final velocity of the combined bullet.
2. Conservation of energy: This model states that the total energy of an isolated system remains constant before and after a collision. In this case, the initial kinetic energy of the system is the sum of the kinetic energies of the two bullets. After the collision, all the material sticks together, so the final kinetic energy is zero.
By using the principle of conservation of energy, we can determine the change in kinetic energy and equate it to the increase in internal energy. From there, we can determine the final temperature and phase of the combined bullet.
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On a day when the speed of sound is 345 m/s, the fundamental frequency of a particular stopped organ pipe is 220 Hz. The second overtone of this pipe has the same wavelength as the third harmonic of an open pipe. How long is the open pipe? Express your answer in mm
The length of the open pipe can be determined by comparing the wavelength of the third harmonic of the open pipe to the second overtone of the stopped organ pipe.
The fundamental frequency of a stopped organ pipe is determined by the length of the pipe, while the frequency of a harmonic in an open pipe is determined by the length and speed of sound. In this case, the fundamental frequency of the stopped organ pipe is given as 220 Hz.
The second overtone of the stopped organ pipe is the third harmonic, which has a frequency that is three times the fundamental frequency, resulting in 660 Hz (220 Hz × 3). The wavelength of this second overtone can be calculated by dividing the speed of sound by its frequency: wavelength = speed of sound / frequency = 345 m/s / 660 Hz = 0.5227 meters.
Now, we need to find the length of the open pipe that produces the same wavelength as the third harmonic of the stopped organ pipe. Since the open pipe has a fundamental frequency that corresponds to its first harmonic, the wavelength of the third harmonic in the open pipe is four times the length of the pipe. Therefore, the length of the open pipe can be calculated by multiplying the wavelength by a factor of 1/4: length = (0.5227 meters) / 4 = 0.1307 meters.
Finally, to express the length in millimeters, we convert the length from meters to millimeters by multiplying it by 1000: length = 0.1307 meters × 1000 = 130.7 mm. Hence, the length of the open pipe is 130.7 mm.
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1.A capacitor C=1000μF initially stores 57μC of charge, and is discharged through a resistor R=2.5kΩ . How much time (in unit of second) is needed for the charge go decrease to 17μC ?
2.When a capacitor C=50μF is charged to 44 volts, how much electric charge (in unit of micro columb) is stored in it?
3.In an RC circuit, the resistance is 12kΩ , and the capacitance 311μF . What is the time constant of the circuit (in unit of second)?
4.A capacitor C=1000μF initially stores 52μC of charge. After being discharged through a resistor R=2kΩ for 1.22 seconds, how much charge (in unit of micro coulomb) is left in the capacitor?
1. Time needed: 0.137 seconds.
2. Electric charge stored: 2.2mC.
3. Time constant: 3.732 seconds.
4. Remaining charge: 22μC.
1. When a capacitor with a capacitance of 1000μF is initially charged with 57μC and discharged through a 2.5kΩ resistor, the time required for the charge to decrease to 17μC can be calculated using the formula for the discharge of a capacitor through a resistor.
The time constant (τ) of the circuit is given by the product of the resistance and capacitance (R × C). In this case, τ = 2.5kΩ × 1000μF = 2.5 seconds. The time required for the charge to decrease to a certain value can be calculated by multiplying the time constant (τ) by the natural logarithm of the initial charge divided by the final charge.
Therefore, the time needed is approximately 0.137 seconds.
2. The electric charge stored in a capacitor can be calculated using the formula Q = C × V, where Q represents the charge, C is the capacitance, and V is the voltage. In this case, the capacitor has a capacitance of 50μF and is charged to 44 volts. Substituting these values into the formula, we find that the electric charge stored in the capacitor is 2.2mC (microcoulombs).
3. The time constant of an RC circuit is a measure of how quickly the voltage across the capacitor reaches approximately 63.2% of its final value during charging or discharging. It is given by the product of the resistance and capacitance (R × C). In this case, the resistance is 12kΩ and the capacitance is 311μF. Multiplying these values together, we find that the time constant of the circuit is approximately 3.732 seconds.
4. When a capacitor with a capacitance of 1000μF and an initial charge of 52μC is discharged through a 2kΩ resistor for 1.22 seconds, we can calculate the remaining charge using the formula Q = Q₀ × e^(-t/RC), where Q is the final charge, Q₀ is the initial charge, t is the time, R is the resistance, and C is the capacitance. Substituting the given values into the formula, we find that the remaining charge in the capacitor is approximately 22μC.
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The distance between two slits is 1.30 × 10-5 m. A beam of coherent light of wavelength 550 nm illuminates these slits, and the distance between the slit and the screen is 2.00 m. a) What is the angular separation between the fourth-order bright fringe and the center of the central bright fringe? () b) What is the distance on the screen between the central bright fringe and the fourth-order bright fringe?
Calculation of the angular separation between the fourth-order bright fringe and the center of the central bright fringeHere, the distance between the two slits = d = 1.30 × 10⁻⁵ m Wavelength of light = λ = 550 nm = 550 × 10⁻⁹ m.
Distance between the slit and the screen = D = 2.00 mThe distance between the central maxima and the fourth-order maxima is given by;y = (nλD) / d = (4 x 550 x 10⁻⁹ x 2) / (1.30 x 10⁻⁵) = 0.000036 = 3.6 x 10⁻⁵ mThe fringe width, w = λD / d = (550 x 10⁻⁹ x 2) / (1.30 x 10⁻⁵) = 0.000090 = 9 x 10⁻⁵ m.
Let the distance between the central maximum and the fourth-order maximum be x radians. Then, for small values of x, tan(x) = xThe angle subtended by the fringe is given by;θ = y / D = (3.6 x 10⁻⁵) / 2.00 = 1.8 x 10⁻⁵ radiansx = θ = 1.8 x 10⁻⁵ radiansTherefore, the angular separation between the fourth-order bright fringe and the center of the central bright fringe is 1.8 x 10⁻⁵ radians.
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A proton (q=+e, m-u), a deuteron (q=+e, m-2u), and an alpha particle (q m-4u) all having the same kinetic energy enter a region of uniform magnetic field of them are moving perpendicular to the magnetic field, what is the ratio of: a) the radius ra of the deuteron path to the radius rp of the proton path and b) the radius ra of the alpha particle path to rp?
a)The ratio of the radius of the deuteron path to the radius of the proton path is 2:1. b) the ratio of the radius of the alpha particle path to the radius of the proton path is also 2:1. The radius of the circular path followed by a charged particle in a uniform magnetic field can be determined using the equation: r = (m * v) / (q * B).
where: r is the radius of the path, m is the mass of the particle,v is the velocity of the particle, q is the charge of the particle, B is the magnetic field strength.In this case, we have three particles: a proton, a deuteron, and an alpha particle. The kinetic energy of each particle is the same, but their masses and charges differ. Let's denote the radius of the deuteron path as rd, the radius of the proton path as rp, and the radius of the alpha particle path as ra.
a) Ratio of the radius of the deuteron path to the radius of the proton path (rd/rp): To find this ratio, we need to compare the mass and charge values for the deuteron and proton:
- Deuteron (D): q = +e, m = 2u
- Proton (P): q = +e, m = u
Using the equation for the radius of the path, we can calculate the ratio:
(rd/rp) = ((m_D * v) / (q_D * B)) / ((m_P * v) / (q_P * B))
(rd/rp) = (2u * v) / (u * v)
(rd/rp) = 2/1
(rd/rp) = 2
Therefore, the ratio of the radius of the deuteron path to the radius of the proton path is 2:1.
b) Ratio of the radius of the alpha particle path to the radius of the proton path (ra/rp):
To find this ratio, we compare the mass and charge values for the alpha particle and proton:
- Alpha particle (α): q = +2e, m = 4u
- Proton (P): q = +e, m = u
Using the equation for the radius of the path, we can calculate the ratio:
(ra/rp) = ((m_α * v) / (q_α * B)) / ((m_P * v) / (q_P * B))
(ra/rp) = (4u * v) / (u * 2v)
(ra/rp) = 4/2
(ra/rp) = 2
Therefore, the ratio of the radius of the alpha particle path to the radius of the proton path is also 2:1.
In conclusion:
a) The ratio of the radius of the deuteron path to the radius of the proton path is 2:1.
b) The ratio of the radius of the alpha particle path to the radius of the proton path is also 2:1.
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Consider the circuit shown below. (Due to the nature of this problem, do not use rounded intermediate values in your calculations-including answers submitted in WebAssign.) 1₁ 12 13 14 15 || = = R₁ = 70 (a) Find 1₁, 12, 13, 14, and 15 (all in A). (Indicate the direction with the signs of your answers.) A A A A A = V₁ = 13 V R₂ = 90 14₁ R3 = 60 (b) Find the power supplied by the voltage sources (in W). W R₁ = 60 V/₂=4V (c) Find the power dissipated by the resistors (in W). W 15
In the given circuit, we are asked to find the currents (1₁, 12, 13, 14, and 15) in Amperes and the power supplied by the voltage sources and power dissipated by the resistors in Watts.
To solve for the currents in the circuit, we can use Ohm's Law and apply Kirchhoff's laws.
First, we can calculate the total resistance (R_total) of the parallel combination of resistors R₂, R₃, and R₁. Since resistors in parallel have the same voltage across them, we can use the formula:
1/R_total = 1/R₂ + 1/R₃ + 1/R₁
Once we have the total resistance, we can find the total current (I_total) supplied by the voltage sources by using Ohm's Law:
I_total = V₁ / R_total
Next, we can find the currents through the individual resistors by applying the current divider rule. The current through each resistor is determined by the ratio of its resistance to the total resistance:
I₁ = (R_total / R₁) * I_total
I₂ = (R_total / R₂) * I_total
I₃ = (R_total / R₃) * I_total
To calculate the power supplied by the voltage sources, we use the formula:
Power = Voltage * Current
Therefore, the power supplied by the voltage sources can be found by multiplying the voltage (V₁) by the total current (I_total).
Finally, to find the power dissipated by each resistor, we can use the formula:
Power = Current^2 * Resistance
Substituting the respective currents and resistances, we can calculate the power dissipated by each resistor.
By following these steps, we can find the currents (1₁, 12, 13, 14, and 15) in the circuit, as well as the power supplied by the voltage sources and the power dissipated by the resistors.
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Work out the logic of how by starting from the state with J = Jmax and mj = - Jmax you finally end up in the state with J = Jmax and mj Jmax and how in the intermediate steps a spectrum of degenerate states with = identical m; is created (first grows, then saturates, then shrinks). (without evaluation, for self-study purposes only)
Starting from the state with J = Jmax and mj = -Jmax, we can consider the process of increasing the value of mj to Jmax. In this case, the state has the maximum angular momentum quantum number J and the minimum value of mj.
As we increase mj, we need to consider the allowed values of mj based on the selection rules for angular momentum. The selection rules dictate that mj can take on integer or half-integer values ranging from -J to J in steps of 1.
Initially, as we increase mj from -Jmax, we create a spectrum of degenerate states with increasing values of mj. For each step, there is a degeneracy of 2J + 1, meaning there are 2J + 1 possible states with the same value of mj.
The spectrum grows as mj increases until it reaches a maximum at mj = Jmax. At this point, the spectrum saturates, meaning all possible states with mj = Jmax have been created. The degeneracy at mj = Jmax is 2Jmax + 1.
After reaching the maximum degeneracy, the spectrum starts to shrink as we continue to increase mj beyond Jmax. This is because there are no allowed values of mj greater than Jmax, according to the selection rules. Therefore, the number of states with increasing mj decreases until we reach a final state with J = Jmax and mj = Jmax.
This process of creating a spectrum of degenerate states with increasing mj, reaching a maximum degeneracy, and then decreasing the number of states is a result of the angular momentum selection rules and the allowed values of mj for a given value of J.
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Suppose a spring weh sping constant 3 N/m is horizonal and has one end attached to a wall and the other end attached to a mass. You want to use the spring to weigh items. You put the spring into motion and find the frequency to be 0.8 Ha (Cycles pet second). What is the mass? Assume there is no friction
Mass = heip (units)
The mass of the object attached to the spring is approximately 0.119 kg.
To determine the mass of the attached object using the spring, we can utilize Hooke's Law, which states that the force exerted by a spring is directly proportional to the displacement of the spring from its equilibrium position.
Hooke's Law can be expressed as:
F = k * x
Where:
F is the force exerted by the spring,
k is the spring constant, and
x is the displacement of the spring from its equilibrium position.
The frequency of the spring's motion (f) can be related to the mass (m) and the spring constant (k) using the equation:
f = (1 / (2π)) * √(k / m)
Rearranging this equation, we can solve for the mass:
m = (k / (4π² * f²))
Given:
Spring constant (k) = 3 N/m
Frequency (f) = 0.8 Hz
Substituting these values into the equation, we get:
m = (3 N/m) / (4π² * (0.8 Hz)²)
Calculating this expression:
m ≈ 0.119 kg
Therefore, the mass of the object attached to the spring is approximately 0.119 kg.
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The mass attached to the spring is approximately 0.238 kg.
To find the mass attached to the spring, we can use the formula for the angular frequency (ω) of a mass-spring system:
ω = √(k / m),
where ω is the angular frequency, k is the spring constant, and m is the mass.
Given:
k = 3 N/m (spring constant),
f = 0.8 Hz (frequency).
First, let's convert the frequency from Hz to radians per second (rad/s):
ω = 2πf = 2π(0.8) ≈ 5.03 rad/s.
Now, we can solve the formula for m:
ω = √(k / m),
m = k / ω^2,
m = 3 N/m / (5.03 rad/s)^2.
Calculating the value:
m ≈ 3 N/m / (5.03 rad/s)^2 ≈ 0.238 kg.
Therefore, the mass attached to the spring is approximately 0.238 kg.
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A certain bivalent metal has a density of 9.304 g/cm3 and a molar mass of 87.5 g/mol. Calculate (a) the number density of conduction electrons, (b) the Fermi energy, (c) the Fermi speed, and (d) the de Broglie wavelength corresponding to this electron speed.
Given that, the density of bivalent metal is 9.304 g/cm³ and the molar mass is 87.5 g/mol.
We have to calculate (a) the number density of conduction electrons, (b) the Fermi energy, (c) the Fermi speed, and (d) the de Broglie wavelength corresponding to this electron speed.
Here are the solutions:
(a) Number density of conduction electrons: To calculate the number density of conduction electrons, we use the formula, n = (density of metal)/(molar mass of metal * Avogadro's number)
On substituting the values in the above equation, we get [tex]n = (9.304 g/cm³)/(87.5 g/mol * 6.022 × 10²³/mol)n = 1.408 × 10²³/cm³[/tex]
(b) Fermi energy : The Fermi energy can be calculated using the formula,[tex]E = h²/8m (3π²n)²/³[/tex]
On substituting the values in the above equation, we get[tex]E = (6.626 × 10⁻³⁴ J s)²/(8 * 9.109 × 10⁻³¹ kg) (3π² * 1.408 × 10²³/cm³)²/³[/tex]
[tex]E = 1.15 × 10⁻¹⁸ J[/tex]
(c) Fermi speed:The Fermi speed can be calculated using the formula, E = 1.15 × 10⁻¹⁸ J
On substituting the values in the above equation, we get[tex]v = [(2 * 1.15 × 10⁻¹⁸ J)/(9.109 × 10⁻³¹ kg)]½v = 1.62 × 10⁶ m/s[/tex]
(d) de Broglie wavelength : The de Broglie wavelength can be calculated using the formula, λ = h/pwhere p = mvOn substituting the values in the above equation, we get [tex]p = (9.109 × 10⁻³¹ kg)(1.62 × 10⁶ m/s)p = 1.47 × 10⁻²⁴ kg[/tex][tex]m/sλ = (6.626 × 10⁻³⁴ J s)/(1.47 × 10⁻²⁴ kg m/s)λ = 4.51 × 10⁻¹⁰ m[/tex]
Hence, the number density of conduction electrons is 1.408 × 10²³/cm³, the Fermi energy is 1.15 × 10⁻¹⁸ J, the Fermi speed is 1.62 × 10⁶ m/s and the de Broglie wavelength corresponding to this electron speed is 4.51 × 10⁻¹⁰ m.
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