To solve this problem it is necessary to apply the concepts related to the drag force.
By definition we know that drag force can be expressed as
[tex]F_D = \frac{1}{2} \rho C_D AV^2[/tex]
Where,
\rho = Density
[tex]C_D =[/tex]Drag Coefficient
A = Area
V = Velocity
Our values are given as
[tex]A = 2.5ft^2[/tex]
[tex]V = 88ft/s[/tex]
[tex]C_D = 0.9[/tex]
[tex]\rho = 0.0765lb/ft^3 \rightarrow[/tex] Air at normal temperature
Replacing at the equation we have,
[tex]F_D = \frac{1}{2} \rho C_D AV^2[/tex]
[tex]F_D = \frac{1}{2} (0.0765lb/ft^3) (0.9) (2.5ft^2) (88ft/s)^2[/tex]
[tex]F_D = 666.468lbf[/tex]
The aerodynamic drag force is 666.468Lbf
In Rutherford's scattering experiments, alpha particles (charge =+2e ) were fired at a gold foil. Consider an alpha particle with an initial kinetic energy heading directly for the nucleus of a gold atom (charge =+79e). The alpha particle will come to rest when all its initial kinetic energy has been converted to electrical potential energy.Find the distance of closest approach between the alpha particle and the gold nucleus for the case K= 2.9MeV in fm.
To find the distance of closest approach between the alpha particle and the gold nucleus, set the potential energy equal to zero and solve for r.
Explanation:In Rutherford's scattering experiments, alpha particles with a charge of +2e were fired at a gold foil. To find the distance of closest approach between the alpha particle and the gold nucleus, we need to calculate the potential energy at this point. Given that the initial kinetic energy of the alpha particle is 2.9 MeV, we can equate it to the electrical potential energy using the formula:
KE = PE
Since the alpha particle comes to rest when all its initial kinetic energy has been converted to electrical potential energy, we can set the potential energy equal to zero:
0 = k * (2e * 79e) / r
where k is the Coulomb constant and r is the distance of closest approach.
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Final answer:
To determine the distance of closest approach between an alpha particle and a gold nucleus with an initial kinetic energy of 2.9 MeV, we apply the conservation of energy principle and calculate the point where the kinetic energy is entirely converted into electrical potential energy.
Explanation:
The student is asking about the distance of closest approach between an alpha particle and the nucleus of a gold atom during Rutherford's scattering experiments when the initial kinetic energy of the alpha particle is 2.9 MeV. To find this distance, we use the concept of conservation of energy, where the initial kinetic energy of the alpha particle is completely converted into electrical potential energy at the point of closest approach. The formula for the electrical potential energy (U) at distance (r) is given by U = k*q1*q2/r, where k is Coulomb's constant, q1 and q2 are the charges of the alpha particle and gold nucleus, respectively, and r is the distance of closest approach.
The charge of an alpha particle is +2e (+2e), and the charge of a gold nucleus is +79e. Given that the initial kinetic energy (K) is 2.9 MeV, we can set K = U to solve for r. The calculation involves converting the given energy into Joules (1eV = 1.6x10^-19 J), and then using the values for k, q1 (+2e), and q2 (+79e) to determine r. Through this, we can derive the equation to calculate the distance of closest approach in femtometers (fm), noting that 1 fm = 1x10^-15 m.
A steel ball, with diameter = 3 mm and density = 7600 kg/m3 is dropped in a liquid with density = 1200 kg/m3 . The average time for the ball to travel a distance of 0.50 m is 10.0 s. a. Does the ball rise or fall in the fluid? Explain b. Determine the fluid viscosity.
Answer
given,
diameter of the steel ball = 3 m = 0.003 m
density of the steel = 7600 kg/m³
density of liquid = 1200 kg/m³
distance travel by the ball = 0.5 m
time = t = 10 s
average velocity =[tex]v = \dfrac{0.5}{10}[/tex]
v = 0.05 m/s
a) density of water is less than ball so, ball will fall in the fluid.
gravitational force is equal to buoyancy force and the drag force
[tex]F_g = F_b + F_d[/tex]
[tex]F_g = \rho_g Vg[/tex]
Density of ball = ρ_s
V is the volume ball
buoyancy force
[tex]F_b = \rho_f Vg[/tex]
[tex]F_b = \rho_f V g[/tex]
drag force
[tex]F_d =3 \pi \mu d v[/tex]
[tex]F_g = F_b + F_d[/tex]
[tex] \rho_g Vg = \rho_f V g+ 3 \pi \mu d v[/tex]
[tex] (\rho_g - \rho_f)Vg = 3 \pi \mu d v[/tex]
[tex]V= \dfrac{1}{6}\pi d^3[/tex]
[tex] (\rho_g - \rho_f). \dfrac{1}{6}\pi d^3.g = 3 \pi \mu d v[/tex]
[tex]\mu = \dfrac{(\rho_s-\rho_f)d^2g}{18 v}[/tex]
[tex]\mu = \dfrac{(7600 -1200)\times 0.003^2\times 9.8 }{18 \times 0.05}[/tex]
μ = 0.63 kg m/s
A skier is moving down a snowy hill with an acceleration of 0.40 m/s2. The angle of the slope is 5.0∘ to the horizontal. What is the acceleration of the same skier when she is moving down a hill with a slope of 10 ∘? Assume the coefficient of kinetic friction is the same in both cases.
Answer:
1.25377 m/s²
Explanation:
m = Mass of person
g = Acceleration due to gravity = 9.81 m/s²
[tex]\mu[/tex] = Coefficient of friction
[tex]\theta[/tex] = Slope
From Newton's second law
[tex]mgsin\theta-f=ma\\\Rightarrow mgsin\theta-\mu mgcos\theta=ma\\\Rightarrow \mu=\frac{gsin\theta-a}{gcos\theta}\\\Rightarrow \mu=\frac{9.81\times sin5-0.4}{9.81\times cos5}\\\Rightarrow \mu=0.04655[/tex]
Applying [tex]\mu[/tex] to the above equation and [tex]\theta=10^{\circ}[/tex]
[tex]mgsin\theta-\mu mgcos\theta=ma\\\Rightarrow a=gsin\theta-\mu gcos\theta\\\Rightarrow a=9.81\times sin10-0.04655\times 9.81\times cos10\\\Rightarrow a=1.25377\ m/s^2[/tex]
The acceleration of the same skier when she is moving down a hill is 1.25377 m/s²
Suppose a photon with an energy of 1.60 eV strikes a piece of metal. If the electron that it hits loses 0.800 eV leaving the metal, what is the kinetic energy of the electron once it has broken free of the metal surface?
To solve this problem it is necessary to apply the concepts related to the change of Energy in photons and the conservation of energy.
From the theory we could consider that the energy change is subject to
[tex]\Delta E = E_0 -W_f[/tex]
Where
[tex]E_0 =[/tex]Initial Energy
[tex]W_f =[/tex] Energy loses
Replacing we have that
[tex]\Delta E = 1.6-0.8[/tex]
[tex]\Delta E = 0.8eV[/tex]
Therefore the Kinetic energy of the electron once it has broken free of the metal surface is 0.8eV
A 0.500-kg ball traveling horizontally on a frictionless surface approaches a very massive stone at 20.0 m/s perpendicular to wall and rebounds with 70.0% of its initial kinetic energy. What is the magnitude of the change in momentum of the stone?
A) 1.63 kg middot m/s
B) 3.00 kg middot m/s
C) 0.000 kg middot m/s
D) 14.0 kg middot m/s
E) 18.4 kg middot m/s
Answer:
E) I = 18.4 N.s
Explanation:
For this exercise let's use momentum momentum
I = Δp = [tex]p_{f}[/tex]- p₀
The energy of the stone is only kinetic
K = ½ m v²
The initial energy is Ko and the final is 70% Ko
[tex]K_{f}[/tex] = 0.70 K₀
energy equation
[tex]K_{f}[/tex] = 0.7 ½ m v₀²
You can also write
[tex]K_{f}[/tex] = ½ m vf²
½ m vf² = ½ m (0.7 v₀²)
[tex]v_{f}[/tex] = v₀ √ 0.7
Now we can calculate and imposed
I = m (-vo √0.7) - m vo
I = m vo (1 +√0.7
I = 0.5000 20.0 (1.8366)
I = 18.4 N.s
A tub containing 53 kg of water is placed in a farmer's canning cellar, initially at 10∘C. On a cold evening the cellar loses thermal energy through the walls at a rate of 1200 J/s. Without the tub of water, the fruit would freeze in 4 h (the fruit freezes at −1∘C because the sugar in the fruit lowers the freezing temperature). Part A By what time interval does the presence of the water delay the freezing of the fruit? The specific heat of water is c = 4180 J/kg⋅∘C.
To solve this problem it is necessary to apply the concepts related to heat transfer and power depending on energy and time.
By definition we know that the heat loss of water is given by
[tex]Q = mc_w*\Delta T+m*L_f[/tex]
Where,
m = mass
[tex]c_w =[/tex] Specific Heat of Water
T = Temperature
[tex]L_f =[/tex]Latent heat of fusion [tex] \rightarrow[/tex] Heat of fusion for water at 0°C is [tex]3.35*10^5J/Kg[/tex]
Our values are given as,
m=53 kg
[tex]C=4180 J/kg\°C[/tex]
[tex]\Delta T=10-(-1)=11[/tex]
Replacing we have,
[tex]Q=53*4180*6+53*3.35*10^5[/tex]
[tex]Q = 19084240J[/tex]
Power can be defined as
[tex]P = \frac{Q}{t}[/tex]
Re-arrange to find t,
[tex]t = \frac{Q}{P}[/tex]
[tex]t = \frac{19084240}{1200}[/tex]
[tex]t = 15903.53s \approx 265 min \aprox 4.41h[/tex]
Therefore the time interval is 4.41h
The question revolves around the principle of thermal energy transfer and the specific heat of water. The water’s high specific heat absorbs a large amount of heat from the cellar and hence delays the freezing of the fruit by an additional 0.57 hours.
Explanation:The subject of this question involves the principles of thermal Energy and heat transfer, specifically regarding the specific heat of water. The water in the tub has the ability to retain heat and slow down the cooling process of the space due to water's high specific heat capacity which is 4180 J/kg⋅°C. This means that water can absorb a lot of heat before its temperature rises.
Firstly, we need to calculate how much heat is the water in the tub able to absorb before its temperature reaches -1 °C (the freezing point of the fruit). This can be calculated with the formula for heat transfer Q = mcΔT, where m is the mass of water, c is the specific heat capacity of water, and ΔT is the change in temperature. In this case, ΔT is 10 - (-1) = 11 °C, so Q = 53 kg * 4180 J/kg⋅°C * 11 °C = 2,444,840 J of heat.
The cellar loses heat at a rate of 1200 J/s, which means to lose 2,444,840 J of heat it would require 2,444,840 J / 1200 J/s = 2,037.3 seconds, which is approximately 0.57 hours. So, the presence of the water in the tub delays the freezing of the fruit by an additional 0.57 hours.
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A 4.00 m-long steel cable is used to support a church chandelier. After the 226-kg chandelier is hung from the ceiling, the steel cable is lengthened by 3.00 mm. Calculate the diameter of the cable in millimeters. (The Young’s modulus for steel is ????????. ???????????????? × ???????????????????????????????? ????????/????????????????.)
Answer:
4.22 mm
Explanation:
E = Young’s modulus for steel = 210 GPa (generally)
[tex]\Delta L[/tex] = Change in length = 3 mm
[tex]L_0[/tex] = Original length = 4 m
A = Area of cable
g = Acceleration due to gravity = 9.81 m/s²
r = Radius of cable
d = Diameter = 2r
m = Mass of chandelier = 226 kg
[tex]\epsilon[/tex] = Longitudinal strain = [tex]\frac{\Delta L}{L_0}[/tex]
Uniaxial stress is given by
[tex]\sigma=E\epsilon\\\Rightarrow \sigma=210\times 10^9 \frac{3\times 10^{-3}}{4}\\\Rightarrow \sigma=157500000\ Pa[/tex]
[tex]\sigma=\frac{F}{A}\\\Rightarrow \sigma=\frac{mg}{\pi r^2}\\\Rightarrow 157500000=\frac{226\times 9.81}{\pi r^2}\\\Rightarrow r=\sqrt{\frac{226\times 9.81}{157500000\times \pi}}\\\Rightarrow r=0.00211\ m\\\Rightarrow d=2r\\\Rightarrow d=2\times 2.11=4.22\ mm[/tex]
The diameter of the cable is 4.22 mm
A horizontal force, F1 = 65 N, and a force, F2 = 12.4 N acting at an angle of θ to the horizontal, are applied to a block of mass m = 3.1 kg. The coefficient of kinetic friction between the block and the surface is μk = 0.2. The block is moving to the right.
Part (a) Solve numerically for the magnitude of the normal force, FN in Newtons, that acts on the block if θ = 30°.t Part (b) Solve numerically for the magnitude of acceleration of the block, a in m/s2, if θ = 30°.
To solve for the normal force, the forces in the vertical direction are balanced, considering gravity and the y-component of force [tex]F_2[/tex] which is approximately 24.211 N. For acceleration, the net force in the horizontal direction is calculated by adding force [tex]F_1[/tex] and the x-component of [tex]F_2[/tex], and subtracting kinetic friction, then divided by the mass which gives [tex]23.14 m/s^2[/tex] approximately.
The problem given requires us to calculate the magnitude of the normal force and the acceleration of the block using Newton's second law and the concepts of kinetic friction.
Part (a)
Firstly, to find the normal force, [tex]F_N[/tex], we need to consider the forces in the vertical (y) direction. The gravitational force (weight) acts downward with a magnitude of m × g, and the vertical component of [tex]F_2[/tex] acts upward. Additionally, the normal force acts upward, balancing these forces.
Thus, we have:
[tex]F_N + F_{2y} - m \times g = 0[/tex]
Where:
[tex]F_N[/tex] is the normal force
[tex]F_{2y} = F_2[/tex] × sin(θ) (the vertical component of [tex]F_2[/tex])
m × g is the weight of the block, m is the mass and g is the acceleration due to gravity, which is approximately [tex]9.81 m/s^2[/tex]
Plugging in the known values:
[tex]F_N[/tex] + 12.4 × sin(30°) - 3.1 × 9.81 = 0
[tex]F_N[/tex] = 3.1 × 9.81 - 12.4 × 0.5
[tex]F_N[/tex] = 30.411 - 6.2
[tex]F_N[/tex] = 24.211 N (approximately)
Part (b)
For the acceleration, a, we consider the forces in the horizontal (x) direction. The net force is the sum of the horizontal component of [tex]F_2[/tex] and [tex]F_1[/tex] minus the kinetic friction force, [tex]F_k[/tex].
The kinetic friction force, [tex]F_k[/tex], is given by:
[tex]F_k = \mu_k \times F_N[/tex]
And hence:
[tex]F_{net}[/tex] = [tex]F_1 + F_{2x} - F_k[/tex]
Using [tex]F_N[/tex] from the first section to find [tex]F_k[/tex] and then [tex]F_{net}[/tex], we get:
[tex]F_{net}[/tex] = 65 + 12.4 × cos(30°) - 0.2 × 24.211
Using Newton's second law, a = [tex]F_{net}[/tex] / m:
a = (65 + 12.4 × 0.866 - 0.2 × 24.211) / 3.1
a = (65 + 10.7424 - 4.8422) / 3.1
a = 71.7424 / 3.1
a = [tex]23.14 m/s^2[/tex] (approximately)
What is the direction of propagation of the wave if E⃗ =Ei^,B⃗ =−Bj^. Express the direction of the propagation vector, P⃗ , as a unit vector. Its three components should be entered in order (x,y,z) separated by commas. For example, if the wave propagates only in the -x direction, enter -1,0,0.
Answer with Explanation:
We are given that
Electric field vector=[tex]\vec{E}=E\hat{i}[/tex]
Magnetic field vector=[tex]\vec{B}=-B\hat{j}[/tex]
We have to find the direction of propagation of the wave.
We know that
The direction of propagation of wave=[tex]\vec{E}\times \vec{B}[/tex]
The direction of propagation of wave=[tex]\hat{i}\times (-\hat{j})=-\hat{k}[/tex]
Because ([tex]\hat{i}\times \hat{j}=\hat{k}[/tex])
The wave propagate in -z direction.
Therefore, the component of the vector is (0,0,-1).
Hence, the direction of the propagation of wave is - z direction and component of direction of propagation vector is (0,0,-1).
The direction of propagation of an Electromagnetic wave is perpendicular to the electric and magnetic fields of the wave. In this case, the fields are along the x and negative y axes, so by applying the cross product, the propagation is in the positive z-direction, hence the unit vector would be 0,0,1.
Explanation:In physics, an Electromagnetic wave has an electric field (E) and magnetic field (B) that are perpendicular to each other and the direction of propagation. These fields are also in phase with each other. Due to these properties, the direction of propagation can be calculated using the cross-product of vectors E and B.
By following the right-hand rule, if you imagine your fingers to curl from E towards B, your thumb will point in the direction of wave propagation. In this case, E = Ei (in the direction of the x-axis) and B = -Bj (in the direction of the negative y-axis).
Therefore, the cross-product E x B = E(-B)k^ (in the direction of the z-axis). Hence, the direction of the propagation Vector, P⃗, will be in the direction of the positive z-axis. For a unit vector, this would simply be 0,0,1.
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The sound level at 1.0 m from a certain talking person talking is 60 dB. You are surrounded by five such people, all 1.0 m from you and all talking equally loud at the same time. The threshold of hearing is 1.0 × 10-12 W/m2. What sound level are you being exposed to? You can neglect any absorption, reflection, or interference of the sound. The threshold of hearing is 1.0 × 10-12 W/m2.
Answer:
66.98 db
Explanation:
We know that
[tex]L_T=L_S+10log(n)[/tex]
L_T= Total signal level in db
n= number of sources
L_S= signal level from signal source.
[tex]L_T=60+10 log(5)[/tex]
= 66.98 db
The combined sound level of five people talking at 60 dB each, given the logarithmic nature of the decibel scale, would be approximately 73 dB.
Explanation:The sound level in decibels (dB), which is a measure of the sound's loudness, is calculated using the formula: B (dB) = 10 log( I / Io ) where B is the decibel level, I is the sound intensity, and Io is the reference intensity (10^-12 W/m² in this case). If one person talking is 60 dB then five people talking would add up logarithmically, not linearly, because the decibel scale is a logarithmic scale.
The formula to calculate the combined sound level of multiple sources is: Total dB = 10 log10 (10^(dB1/10) + 10^(dB2/10) + …). In our case, it would be Total dB = 10 log10 (5*10^(60/10)), which is approximately 73 dB.
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Suppose you have 1 kg each of iron, glass, and water, and all three samples are at 10°C.
(a) Rank the samples from lowest to highest temperature after 100 J of energy is added to each by heat.
(b) Rank them from least to greatest amount of energy transferred by heat if enough energy is transferred so that each increases in temperature by 20°C.
To solve this problem it is necessary to apply the concepts related to heat exchange and Entropy.
The temperature and mass remain constant, therefore the entropy values will be the only ones to change.
Of the three elements given their entropy values are given by
[tex]\Delta S_{iron}=0.45J/gmC[/tex]
[tex]\Delta S_{glass}=0.8J/gmC[/tex]
[tex]\Delta S_{water}= 4.186J/gmC[/tex]
Part A) From thermodynamic theory we know that temperature is inversely proportional to entropy
[tex]T = \frac{E}{\Delta S} \rightarrow[/tex] Energy remains constant
[tex]\Delta t \propto \frac{1}{S}[/tex]
Therefore the order would be
Lowest Temperature= Water
Medium Temperature= Glass
Highest Temperature=Iron
Part B) In the case of Energy the opposite happens because it is proportional to the entropy, then
[tex]E = T(\Delta S) \rightarrow[/tex]Temperature is constant
[tex]E \propto S[/tex]
Lowest Energy = Iron
Medium Energy = Glass
Highest Energy = Water
The temperature increase brought by a given amount of energy input depends on the material's specific heat capacity. Given a certain amount of energy, iron will heat up the most due to its low specific heat capacity. But if a certain temperature increase is desired, water, having high specific heat, will require the most energy.
Explanation:The ranking of the samples after adding 100 J of energy can be determined by comparing their specific heat capacities. The specific heat capacity is the amount of heat necessary to raise the temperature of a substance by one degree Celsius.
Iron has a lower specific heat capacity than glass and water, meaning it will heat up more quickly when the same amount of energy is added. Thus, providing the same amount of energy (100 J) to each sample would result in the temperature of the iron increasing to the greatest extent, followed by the glass, and then the water.
Conversely, when each sample is to increase in temperature by the same amount (20°C), the amount of energy required will also be determined by the specific heat capacities. This time, however, the substance with the higher specific heat capacity will require more energy to achieve this temperature increase. Therefore, the water will require the most energy, followed by the glass, and then the iron.
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A sample of blood is placed in a centrifuge of radius 16.0 cm. The mass of a red blood cell is 3.0 ✕ 10−16 kg, and the magnitude of the force acting on it as it settles out of the plasma is 4.0 ✕ 10−11 N. At how many revolutions per second should the centrifuge be operated?
Answer:
[tex]f=145.29Hz[/tex]
Explanation:
The centripetal force is given by:
[tex]F_c=ma_c(1)[/tex]
Here m is the body's mass in which the force is acting and [tex]a_c[/tex] is the centripetal acceleration:
[tex]a_c=\frac{v^2}{r}(2)[/tex]
Here v is the speed of the body and r its radius. The speed is given by:
[tex]v=2\pi fr(3)[/tex]
Replacing (3) in (2):
[tex]a_c=4\pi^2f^2r(4)[/tex]
Replacing (4) in (1) and solving for f:
[tex]F_c=m4\pi^2 f^2r\\\\f=\sqrt{\frac{F_c}{4m\pi^2r}}\\f=\sqrt{\frac{4*10^{-11}N}{4(3*10^{-16}kg)\pi^2(16*10^{-2}m)}}\\f=145.29Hz[/tex]
Final answer:
To find the revolutions per second for a centrifuge, the known force acting on a red blood cell is used with the mass and radius of the centrifuge to calculate the angular velocity, which is then converted to revolutions per second.
Explanation:
To determine the revolutions per second at which a centrifuge should be operated to exert a specified force on a red blood cell, we can make use of the relationship between centrifugal force and centripetal acceleration. The force experienced by the red blood cell can be expressed by Newton's second law for circular motion: F = m\(a_{c}\), where F is the force, m is the mass of the red blood cell, and \(a_{c}\) is the centripetal acceleration.
The centripetal acceleration \(a_{c}\) is also related to the angular velocity \(\omega\) of the rotating body by the formula \(a_{c} = \omega^{2}r\), where r is the radius of the centrifuge. Solving for the angular velocity gives us \(\omega = \sqrt{\frac{F}{mr}}\). Once we have \(\omega\), we can convert it to revolutions per second by dividing by 2\(\pi\) (since one revolution is 2\(\pi\) radians).
For the given numbers, F = 4.0 \(\times\) 10^{-11} N, m = 3.0 \(\times\) 10^{-16} kg, and r = 16.0 cm = 0.16 m. We can calculate \(\omega\), and subsequently the number of revolutions per second the centrifuge should be operated at to achieve the necessary centrifugal force for sedimentation of the blood cells. The extraordinarily high centripetal acceleration makes such devices known as ultracentrifuges.
which of the following is another way to say that, in energy transforms, some energy is always converted unusable or unwanted forms?
A. the entropy of a system tends to decrease overtime.
B. energy transforms are never 100% efficient
C. the energy in a system is always constant
D. energy transfers are always 100% efficient
A solid disk of mass 3 kg, radius 0.5 m, and initial angular velocity 10 rad/sec is dropped onto an initially stationary second disk having the same radius and twice the mass. The second disk cannot fall, but is free to rotate. The disks stick and rotate together. Assume that there are no external torques. Please find each of the following.
a) The kinetic energy of the first disk before it is dropped
b) The final angular velocity of the combined disks
c) The final kinetic energy of the combined disks
The first disk's kinetic energy before it is dropped is 18.75 J. The final angular velocity of the combined disks after they stick together is 3.33 rad/s. The final kinetic energy of the combined disks is 24.97 J.
Explanation:Given a solid disk of mass 3 kg, radius 0.5 m, and initial angular velocity 10 rad/sec, and a second disk with the same radius but with double the mass (6 kg), which is initially at rest, we need to find the following:
Kinetic energy of the first disk before it is droppedFinal angular velocity of the combined disks after they stick togetherFinal kinetic energy of the combined disks(a) The kinetic energy (KE) of the first disk before it is dropped is calculated using the formula for rotational kinetic energy, KE = (1/2)Iω², where I is the moment of inertia for a solid disk (I = (1/2)mr²) and ω is the angular velocity. Therefore, KE = (1/2)((1/2)mr²)ω² = (1/2)((1/2)(3 kg)(0.5 m)²)(10 rad/s)² = 18.75 J.
(b) To find the final angular velocity (ω'), we conserve angular momentum since no external torques are acting. L_initial = L_final, which means Iω = (I1 + I2)ω'. Calculating, we get (1/2)(3 kg)(0.5 m)²(10 rad/s) = ((1/2)(3 kg)(0.5 m)² + (1/2)(6 kg)(0.5 m)²)ω', solving for ω' gives us 3.33 rad/s.
(c) The final kinetic energy (KE_final) is calculated with the combined moment of inertia and the final angular velocity using KE_final = (1/2)(I1 + I2)ω'^2. Using the values from (b), we have KE_final = (1/2)((1/2)(3 kg)(0.5 m)² + (1/2)(6 kg)(0.5 m)²)(3.33 rad/s)² = 24.97 J.
The energy levels of a particular quantum object are -11.7 eV, -4.2 eV, and -3.3 eV. If a collection of these objects is bombarded by an electron beam so that there are some objects in each excited state, what are the energies of the photons that will be emitted?
To solve this problem it is necessary to apply an energy balance equation in each of the states to assess what their respective relationship is.
By definition the energy balance is simply given by the change between the two states:
[tex]|\Delta E_{ij}| = |E_i-E_j|[/tex]
Our states are given by
[tex]E_1 = -11.7eV[/tex]
[tex]E_2 = -4.2eV[/tex]
[tex]E_3 = -3.3eV[/tex]
In this way the energy balance for the states would be given by,
[tex]|\Delta E_{12}| = |E_1-E_2|\\|\Delta E_{12}| = |-11.7-(-4.2)|\\|\Delta E_{12}| = 7.5eV\\[/tex]
[tex]|\Delta E_{13}| = |E_1-E_3|\\|\Delta E_{13}| = |-11.7-(-3.3)|\\|\Delta E_{13}| = 8.4eV[/tex]
[tex]|\Delta E_{23}| = |E_2-E_3|\\|\Delta E_{23}| = |-4.2-(-3.3)|\\|\Delta E_{23}| = 0.9eV[/tex]
Therefore the states of energy would be
Lowest : 0.9eV
Middle :7.5eV
Highest: 8.4eV
When you drink cold water, your body must expend metabolic energy in order to maintain normal body temperature (37° C) by warming up the water in your stomach. Could drinking ice water, then, substitute for exercise as a way to "burn calories?" Suppose you expend 286 kilocalories during a brisk hour-long walk. How many liters of ice water (0° C) would you have to drink in order to use up 286 kilocalories of metabolic energy? For comparison, the stomach can hold about 1 liter.
Answer:
7.72 Liters
Explanation:
normal body temperature = T_body =37° C
temperature of ice water = T_ice =0°c
specfic heat of water = c_{water} =4186J/kg.°C
if the person drink 1 liter of cold water mass of water is = m = 1.0kg
heat lost by body is Qwater =mc_{water} ΔT
= mc{water} ( T_ice - T_body)
= 1.0×4186× (0 -37)
= -154.882 ×10^3 J
here negative sign indicates the energy lost by body in metabolic process energy expended due to brisk - hour long walk is Q_{walk} = 286 kilocalories
= 286×4186J
so number of liters of ice water have to drink is
n×Q_{water} =Q_{walk} n= Q_{walk}/ Q_{water}
= 286×4186J/154.882×10^3 J
= 7.72 Liters
Answer:
[tex]V=7.73\ L[/tex]
Explanation:
Given:
Initial temperature of water, [tex]T_i=0^{\circ}C[/tex]
final temperature of water, [tex]T_f=37^{\circ}C[/tex]
energy spent in one hour of walk, [tex]286\ kilocal=(286\times 4186)\ J[/tex]
volumetric capacity of stomach, [tex]V=1\ L[/tex]
Now, let m be the mass of water at zero degree Celsius to be drank to spend 286 kilo-calories of energy.
[tex]\therefore Q=m.c_w.\Delta T[/tex] .....................................(1)
where:
m = mass of water
Q = heat energy
[tex]c_w=4186\ J\ (specific\ heat\ of\ water)[/tex]
[tex]\Delta T[/tex]= temperature difference
Putting values in the eq. (1):
[tex]286\times 4186=m\times 4186\times 37[/tex]
[tex]m=7.73\ kg[/tex]
Since water has a density of 1 kilogram per liter, therefore the volume of water will be:
[tex]V=7.73\ L[/tex]
A spherical steel ball bearing has a diameter of 2.540 cm at 26.00°C. (Assume the coefficient of linear expansion for steel is 11 ✕ 10−6 (°C)−1. )
(a) What is its diameter when its temperature is raised to 91.0°C? (Give your answer to at least four significant figures.) 165.1 Incorrect: Your answer is incorrect. Your response differs significantly from the correct answer. Rework your solution from the beginning and check each step carefully. cm
(b) What temperature change is required to increase its volume by 1.100%
Answer: a)2.542cm
Explanation:
According to area expansivity which is defined as change in area per unit area for degree rise in kelvin.
Area expansivity= A2-A1/A1(¶2-¶1)
A2-A1 is change in area
¶2-¶1 is temperature change
A2 if final area
A1 is initial area
¶2 is final temp = 91°C
¶1 is initial temp= 26°C
coefficient of linear expansion for steel is 11 ✕ 10−6 (°C)−1.
Area of the spherical steel ball = Πd²/4
A1= Π×2.54²/4
A1 = 5.07cm²
Area expansivity = 2×linear expansion = 2×11 ✕ 10−6 (°C)−1.
= 22 ✕ 10−6 (°C)−1.
Substituting in the formula to get final area A2
22 ✕ 10−6 (°C)−1 = A2-5.07/5.07(91-26)
22 ✕ 10−6 (°C)−1 = A2-5.07/329.55
A2-5.07 = 0.0073
A2 = 0.0073+5.07
A2= 5.0073cm²
To get final diameter
A2=Πd²/4
5.0073=Πd²/4
20.309 = Πd²
d² = 20.309/Π
d²=6.46
d= √6.46
d= 2.542cm
David is riding on a flying carousel which swings him in circles of radius R=4.0R=4.0m, at a height of h=6h=6 m above the ground. The carousel rotates counterclockwise once every 5 sec.
When he is on the west side of the carousel, David's hat falls off.
Where does the hat land (relative to the point where it fell off)?
Answer:
5.55935324 m
Explanation:
r = Radius = 4 m
h = Height = 6 m
Frequency is
[tex]f=\frac{1}{T}\\\Rightarrow f=\frac{1}{5}\ Hz[/tex]
Angular speed is given by
[tex]\omega=2\pi f\\\Rightarrow \omega=\frac{2}{5}\pi[/tex]
Tangential velocity of the hat is given by
[tex]v=r\omega\\\Rightarrow v=4\times\frac{2}{5}\pi\\\Rightarrow v=5.02654\ m/s[/tex]
t = Time taken
u = Initial velocity
v = Final velocity
s = Displacement
g = Acceleration due to gravity = 9.81 m/s²
From equation of motion
[tex]s=ut+\frac{1}{2}gt^2\\\Rightarrow 6=0t+\frac{1}{2}\times 9.81\times t^2\\\Rightarrow t=\sqrt{\frac{6\times 2}{9.81}}\\\Rightarrow t=1.106\ s[/tex]
Distance = Speed×Time
[tex]Distance=5.02654\times 1.106=5.55935324\ m[/tex]
The hat will land 5.55935324 m away from the point of release
David's hat would travel in a straight line relative to the Earth and land to the south of the point where it fell off due to the carousel's counterclockwise rotation and the principles of projectile motion.
Explanation:When we consider David's hat falling off while he is riding on a flying carousel, we have to address the physical principles that govern the motion of the hat after it leaves his head. As David's hat falls off on the west side of the carousel, it would have initially the same horizontal velocity as the carousel at that point. However, since the carousel is rotating counterclockwise, and assuming there is no significant air resistance, the hat would move in a straight line relative to the Earth. This means it would land to the south of the point where it fell off, as the carousel would continue to rotate after the hat has been released. This situation applies principles of projectile motion and inertial frames.
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Two balls of equal mass are thrown horizontally with the same initial velocity. They hit identical stationary boxes resting on a frictionless horizontal surface. The ball hitting box 1 bounces back, while the ball hitting box 2 gets stuck.Which box ends up moving faster?a. Box 1b. Box 2c. Same
Answer:
a. Box 1
Explanation:
Hi there!
The momentum of the system box-ball is conserved in both cases because there is no external force applied on the system.
The momentum of the system is calculated as the sum of the momenta of each object that composes the system. The momentum is calculated as follows:
p = m · v
Where:
p = momentum.
m = mass.
v = velocity.
Then, the momentum of the system before and after the collision will be:
System ball - box 1
initial momentum = final momentum
mb · vb + m1 · v1 = mb · vb´ + m1 · v1´
Where:
mb = mass of the ball.
vb = veloctiy of the ball.
m1 = mass of box 1.
v1 = velocity of box 1.
vb´ = final velocity of the ball.
v1´ = final velocity of box 1.
Since the initial velocity of the box is zero:
mb · vb = mb · vb´ + m1 · v1´
Solving for v1´
mb · vb - mb · vb´ = m1 · v1´
mb · (vb - vb´) = m1 · v1´
mb · (vb - vb´) / m1 = v1´
Since vb´ is negative because the ball bounces back, then:
mb · (vb + vb´) / m1 = v1´
Now let´s express the momentum of the system ball - box 2
System ball -box 2
mb · vb + m2 · v2 = (mb + m2) · v2´
Since v2 = 0
mb · vb = (mb + m2) · v2´
Solving for v2´:
mb · vb / (mb + m2) = v2´
Comparing the two expressions:
v2´ = mb · vb / (mb + m)
v1´ = mb · (vb + vb´) / m
In v1´ the numerator is greater than the numerator in v2´ because
vb + vb´> vb
In v2´ the denominator is greater than the denominator in v1´ because
mb + m > m
then v1´ > v2´
Box 1 ends up moving faster than box 2
Once again we have a skier on an inclined plane. The skier has mass M and starts from rest. Her speed at the bottom of the slope is 12.0 meters/second. The hill is inclined 30 degrees from the horizontal and the length of the slope is 100.0 meters.Use the law of conservation of energy to determine her final speed and write that number down here:
Answer:
v = 31.3 m / s
Explanation:
The law of the conservation of stable energy that if there are no frictional forces mechanical energy is conserved throughout the point.
Let's look for mechanical energy at two points, the highest where the body is at rest and the lowest where at the bottom of the plane
Highest point
Em₀ = U = m g y
Lowest point
[tex]Em_{f}[/tex] = K = ½ m v²
As there is no friction, mechanical energy is conserved
Em₀ = [tex]Em_{f}[/tex]
m g y = ½ m v²
v = √ 2 g y
Where we can use trigonometry to find and
sin 30 = y / L
y = L sin 30
Let's replace
v = RA (2 g L sin 30)
Let's calculate
v = RA (2 9.8 100.0 sin30)
v = 31.3 m / s
A rescue team is searching for Andrew, a geologist who was stranded while conducting research in the mountains of Colorado. The team uses electronic listening devices in order to detect any shouts for help. The sound waves from his shouts reaching the base camp can be approximated by a sinusoidal wave with a frequency f = 530 Hz and displacement amplitude A = 2.00×10−8 m , where the sound wave properties are valid at the base camp where the measurements are being made. What sound intensity level will the rescue team measure from the frightened researcher? Assume the speed of sound is v=328m/s and the density of air rho = 1.34 kg/m3
Final answer:
To calculate the sound intensity level, we use the formula I = (A² * ρ * v * f)/2. Plugging in the given values, the sound intensity level will be approximately 4.32 × 10⁻⁶ W/m².
Explanation:
To calculate the sound intensity level, we can use the formula:
I = (A² * ρ * v * f)/2
Where:
I is the sound intensity level,
A is the displacement amplitude,
ρ is the density of air,
v is the speed of sound,
f is the frequency of the sound wave.
Plugging in the given values, we have:
I = (2.00×10⁻⁸ m)² * 1.34 kg/m³ * 328 m/s * 530 Hz)/2
Simplifying the expression, the sound intensity level will be approximately 4.32 × 10⁻⁶ W/m².
A baseball pitcher throws a ball horizontally at a speed of 40.2 m/s. A catcher is 18.6 m away from the pitcher. Find the magnitude, in meters, of the vertical distance that the ball drops as it moves from the pitcher to the catcher. Ignore air resistance.
Vertical distance, when the ball drops as it moves from the pitcher to the catcher is 1.048 meters.
What is the second equation of motion?The equation of motion is the relation between the distance, velocity, acceleration and time of a moving body.
The second equation of the motion for distance can be given as,
[tex]s=ut+\dfrac{1}{2}at^2[/tex]
Here, [tex]u[/tex] is the initial velocity, [tex]a[/tex] is the acceleration of the body and [tex]t[/tex] is the time taken by it.
Total time taken by the ball to reach to the catcher is the ratio of horizontal distance traveled by it to the speed of the ball.
As the speed of the ball is 40.2 m/s and the distance of the pitcher and the catcher is 18.6 meters. Thus the time of flight is,
[tex]t=\dfrac{18.6}{40.2}\\t=0.462\rm s[/tex]
Thus, total time taken by the ball to reach to the catcher is 0.462 seconds.
As the initial velocity of the ball is zero. Thus by the second equation of motion,
[tex]h=0+\dfrac{1}{2}(9.81)(0.462)^2\\h=1.048\rm m[/tex]
Thus, the vertical distance covered when the ball drops as it moves from the pitcher to the catcher is 1.048 meters.
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The baseball dropped approximately 1.04 meters vertically while it traveled horizontally to the catcher.
Explanation:The subject of this question is Physics, specifically related to the concept of projectile motion. To find the vertical distance that the ball drops, we'll use the principles of kinematics. In this case, the problem describes a horizontal launch, and we can find the vertical distance using the equation for distance in free fall under gravity: d = 0.5*gt^2, where g = 9.8 m/s^2 is the acceleration due to gravity. The time t can be found from the horizontal motion, by dividing the horizontal distance by the horizontal speed: t = 18.6 m / 40.2 m/s = 0.46 s. Using this time, we compute the vertical drop: d = 0.5*9.8 m/s^2*(0.46 s)^2 = 1.04 m. So, the ball drops by approximately 1.04 m while it travels horizontally to the catcher.
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The average human has a density of 945 kg/m3 after inhalation, and 1020 kg/m3 after exhalation. Fresh water has a density of 1000 kg/3, sea water a density of about 1025 kg/m3, and the Dead Sea (which is actually a lake), a density of about 1230 kg/3. Which of the following statements are true?
a. The human body has nearly the same density as salt water after exhaling.
b. The human body will always float in the Dead Sea.
c.A human would float in fresh water after exhaling
Answer:
a. The human body has nearly the same density as salt water after exhaling.
b. The human body will always float in the Dead Sea.
Explanation:
According to the concept of floating on the basis of density, any body that is put in a fluid of density greater than its own density will always float due to the force of buoyancy from the liquid.
The portion of the object submerged while the object is floating depends upon the density of the object as compared to the density of the fluid. This is governed by the equation:[tex]\rho_f.V_s=\rho_o.V_o[/tex]
where:
[tex]\rho_f=[/tex] density of the fluid
[tex]\rho_o=[/tex] density of the object
[tex]V_s=[/tex] volume of the object submerged in the fluid
[tex]V_o=[/tex] total volume of the object
Find a numerical value for rhoearth, the average density of the earth in kilograms per cubic meter. Use 6378km for the radius of the earth, G=6.67×10−11m3/(kg⋅s2), and a value of g at the surface of 9.80m/s2. Express your answer to three significant figures.
According to the information provided to define an average density, it is necessary to use the concepts related to mass calculation based on gravitational constants and radius, as well as the calculation of the volume of a sphere.
By definition we know that the mass of a body in this case of the earth is given as a function of
[tex]M = \frac{gr^2}{G}[/tex]
Where,
g= gravitational acceleration
G = Universal gravitational constant
r = radius (earth at this case)
All of this values we have,
[tex]g = 9.8m/s^2\\G = 6.67*10^{-11} m^3/kg*s^2\\r = 6378*10^3 m[/tex]
Replacing at this equation we have that
[tex]M = \frac{gr^2}{G} \\M = \frac{(9.8)(6378*10^3)^2}{6.67*10^{-11}} \\M = 5.972*10^{24}kg[/tex]
The Volume of a Sphere is equal to
[tex]V = \frac{4}{3}\pi r^3\\V = \frac{4}{3} \pi (6378*10^3)^3\\V = 1.08*10^{21}m^3[/tex]
Therefore using the relation between mass, volume and density we have that
[tex]\rho = \frac{m}{V}\\\rho = \frac{5.972*10^{24}}{1.08*10^{21}}\\\rho = 5.52*10^3kg/m^3[/tex]
The atmospheric pressure at sea level is 1.013 x 105 N/m2. The unit of pressure N/m2 is also called a pascal (Pa). The surface area of an average adult body is about 2 m2. How much crushing force does the atmosphere exert on people? Why don't we get crushed?
Answer:
Crushing force will be [tex]2.026\times 10^5N[/tex]
Explanation:
We have given that atmospheric pressure [tex]P=1.013\times 10^5N/m^2[/tex]
Area is given as [tex]A=2m^2[/tex]
We have to find the force
We know that force is given by
[tex]Force=pressure\times area=1.013\times 10^5\times 2=2.026\times 10^5N[/tex]
The reason that we do not get crushed is because the force is distributed over our bodies, and because we have air inside our bodies pushing outwards (the air in your blood,lungs, etc.). The pressure inside of our bodies keeps the air outside from crushing it.
A machinist turns on the power on to a grinding wheel at time t= 0 s. The wheel accelerates uniformly from rest for 10 s and reaches the operating angular speed of 58rad/s. The wheel is run at that angular velocity for 30 s, and then power is shut off. The wheel slows down uniformly at 1.4rad/s2 until the wheel stops. What is the total number of revolutions made by the wheel in this situation?
Answer:
θt = 514.3 revolutions
Explanation:
(1)The wheel accelerates uniformly from rest for 10 s and reaches the operating angular speed of 58rad/s.
The uniformly accelerated circular movement a circular path movement in which the angular acceleration is constant.
We apply the equations of circular motion uniformly accelerated
ωf = ω₀ + α*t Formula (1)
θ = ω₀*t + (1/2)*α*t² Formula (2)
ωf² = ω₀² +2*α*θ Formula (3)
Where:
θ : angle that the body has rotated in a given time interval (rad)
α : angular acceleration (rad/s²)
t : time interval (s)
ω₀ : initial angular speed ( rad/s)
ωf : final angular speed ( rad/s)
Number of revolutions made by the wheel from t = 0 to t = 10 s
Data
ω₀ = 0
t = 10 s
ωf = 58 rad/s
We replace data in the formula (1) to calculate α
ωf = ω₀ + α*t
58 = 0 + α*(10)
α = 58 /10
α = 5.8 rad/s²
We replace data in the formula (2) to calculate θ
θ = ω₀*t + (1/2)*α*t²
θ = 0 + (1/2)*( 5.8)*(10)²
θ₁ = 290 rad
(2)The wheel is run at that angular velocity for 30 s, and then power is shut off.
The movement of the wheel is circular with constant angular speed and the formula to calculate θ is:
θ = ω*t
ω = 58 rad/s , t= 30s
θ = (58 rad/s)*(30)
θ = (58 rad/s)*(30)
θ ₂= 1740 rad
(3)The wheel slows down uniformly at 1.4 rad/s² until the wheel stops.
ω₀ = 58 rad/s
α = -1.4 rad/s²
ωf = 0
We replace data in the formula (3) to calculate θ
(ωf)² = (ω₀)² + (2)*(α )*θ
0 = (58)² + (2)*(-1.4)*θ
(2)*(1.4)*θ = (58)²
θ = (58)² / (2.8)
θ = (58)² / (2.8)
θ₃ = 1201.42 rad
Total number of revolutions made by the wheel (θt)
θt =θ₁+θ₂+θ₃
θt = 290 rad+ 1740 rad + 1201.42 rad
θt = 3231.42 rad
1 revolution = 2π rad
θt = 3231.42 rad* ( 1revolution/2π rad)
θt = 514.3 revolutions
Communications satellites are placed in a circular orbit where they stay directly over a fixed point on the equator as the earth rotates.
These are called geosynchronous orbits. The altitude of a geosynchronous orbit is 3.58×107m(≈22,000miles).
Part A
What is the period of a satellite in a geosynchronous orbit?
Part B
Find the value of g at this altitude.
Part C
What is the weight of a 2000 kg satellite in a geosynchronous orbit?
Answer:
a) 24 Hs. b) 0.224 m/s² c) 448 N
Explanation:
a) As satellites in a geosynchronous orbits, stay directly over a point fixed on the Equator while the Earth rotates, the only way that this can be possible, if the period of the satellite (time to complete a full orbit) is equal to the time that the Earth uses to complete a spin itself, which is exactly one day.
b)
The value of g, is just the acceleration due to the gravitational attraction between the satellite and the Earth.
According the Universal Law of Gravitation, this force can be written in this way:
Fg = ms . a = G me. ms / (re+rs)² ⇒a=g= G me / (re + rs)²
Replacing by the values of G, me, re, and rs, we get:
g = 6.67. 10⁻¹¹ . 5.97.10²⁴ / (6.37 10⁶ + 3.58.10⁷)² m/s²
g= 0.224 m/s²
c) If we call "weight" to the magnitude of the gravitational force on the satellite (as we do with masses on Earth), we can find this value, just solving the equation for Fg, as follows:
Fg = G me . ms / (re + rs)²
Replacing by the values, we find:
Fg = 448 N
A satellite in geosynchronous orbit has a period of 24 hours. The gravitational acceleration at this altitude is roughly 0.224 m/s^2. The weight of a 2000 kg satellite in a geosynchronous orbit is roughly 448 N.
Explanation:A satellite in a geosynchronous orbit has a period of 24 hours, which equates to how long it takes the Earth to rotate once on its axis. The value of gravitational acceleration g at an altitude of a geosynchronous orbit can be calculated using the formula g = G × (M / (R+h)^2), where G is the gravitational constant, M is the mass of the Earth, R is the radius of the Earth, and h is the altitude of the satellite.
Using the given altitude, the value of g at this height is approximately 0.224 m/s^2. Now, to find the weight of a 2000 kg satellite in a geosynchronous orbit, we use the formula W=mg where m is the mass of the satellite and g is the gravitational acceleration at the altitude. That gives us the value of roughly 448 N for the weight of the satellite at geosynchronous orbit.
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A radio wave transmits 36.8 W/m2 of power per unit area. A flat surface of area A is perpendicular to the direction of propagation of the wave. Assuming the surface is a perfect absorber, calculate the radiation pressure on it.
Answer:
122.6 nPa
Explanation:
Here ,
Intensity of incident light , I = 36.8 W/m^2
angle with area, θ = 0 degree
for a perfect absorber ,
radiation pressure = [tex]\frac{Icos\theta}{c}[/tex]
I= Intensity of incident light, c= speed of light
radiation pressure = [tex]\frac{36.8\times cos0}{3\times10^8}[/tex]
radiation pressure = 12.26×10^-8 Pa
radiation pressure = 122.6 nPa
the radiation pressure acting on the 122.6 nPa
A 1.2 kg ball drops vertically onto a floor from a height of 32 m, and rebounds with an initial speed of 10 m/s.
(a) What impulse acts on the ball during the contact?
(b) If the ball is in contact with the floor for 0.020 s, what is the magnitude of the average force on the floor from by the ball? Neglect air resistance
Explanation:
Given that,
Mass of the ball, m = 1.2 kg
Initial speed of the ball, u = 10 m/s
Height of the floor from ground, h = 32 m
(a) Let v is the final speed of the ball. It can be calculated using the conservation of energy as :
[tex]\dfrac{1}{2}mv^2=mgh[/tex]
[tex]v=\sqrt{2gh}[/tex]
[tex]v=\sqrt{2\times 9.8\times 32}[/tex]
v = -25.04 m/s (negative as it rebounds)
The impulse acting on the ball is equal to the change in momentum. It can be calculated as :
[tex]J=m(v-u)[/tex]
[tex]J=1.2\times (-25.04-10)[/tex]
J = -42.048 kg-m/s
(b) Time of contact, t = 0.02 s
Let F is the average force on the floor from by the ball. Impulse acting on an object is given by :
[tex]J=\dfrac{F}{t}[/tex]
[tex]F=J\times t[/tex]
[tex]F=42.048\times 0.02[/tex]
F = 0.8409 N
Hence, this is the required solution.
A new experiment is created with the screen at a distance of 1.9 m from the slits (with spacing 0.11 mm). What is the distance between the second order bright fringe of light with λ = 695 nm and the third order bright fringe of light with λ = 407 nm? (Give the absolute value of the smallest possible distance between these two fringes: the distance between bright fringes on the same side of the central bright fringe.) |x| =
Answer:
The distance between the bright fringes is 2.19 mm
Explanation:
Distance of the screen from the slits, d = 1.9 m
Slit width, w = 0.11 mm = [tex]0.11\times 10^{- 3}\ m[/tex]
Wavelength, [tex]\lambda = 695\ nm[/tex]
Wavelength, [tex]\lambda' = 407\ nm[/tex]
To calculate the distance between the second order bright fringe:
[tex]y_{n} = \frac{n\lambda d}{w}[/tex]
[tex]y'_{3} = \frac{n\lambda' d}{w} = \frac{3\times 695\times 10^{- 9}\times 1.9}{0.11\times 10^{- 3}} = 0.036\ m[/tex]
[tex]y_{2} = \frac{2\times 407\times 10^{- 9}\times 1.9}{0.11\times 10^{- 3}} = 0.014\ m[/tex]
Distance, |x| = [tex]y'_{3} - y_{2}[/tex]
|x| = [tex]0.036 - 0.0141 = 0.0219 m = 2.19\ mm[/tex]