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stepladder [879]
3 years ago
6

Two parallel disks of diameter D 5 0.6 m separated by L 5 0.4 m are located directly on top of each other. Both disks are black

and are maintained at a temperature of 450 K. The back sides of the disks are insulated, and the environment that the disks are in can be considered to be a blackbody at 300 K. Determine the net rate of radiation heat transfer from the disks to the environment.

Physics
1 answer:
oksian1 [2.3K]3 years ago
5 0

To solve this problem it is necessary to apply the concepts related to the Stefan-Boltzmann law which establishes that a black body emits thermal radiation with a total hemispheric emissive power (W / m²) proportional to the fourth power of its temperature.

Heat flow is obtained as follows:

Q = FA\sigma\Delta T^4

Where,

F =View Factor

A = Cross sectional Area

\sigma = Stefan-Boltzmann constant

T= Temperature

Our values are given as

D = 0.6m

L = 0.4m\\T_1 = 450K\\T_2 = 450K\\T_3 = 300K

The view factor between two coaxial parallel disks would be

\frac{L}{r_1} = \frac{0.4}{0.3}= 1.33

\frac{r_2}{L} = \frac{0.3}{0.4} = 0.75

Then the view factor between base to top surface of the cylinder becomes F_{12} = 0.26. From the summation rule

F_{13} = 1-0.26

F_{13} = 0.74

Then the net rate of radiation heat transfer from the disks to the environment is calculated as

\dot{Q_3} = \dot{Q_{13}}+\dot{Q_{23}}

\dot{Q_3} = 2\dot{Q_{13}}

\dot{Q_3} = 2F_{13}A_1 \sigma (T_1^4-T_3^4)

\dot{Q_3} = 2(0.74)(\pi*0.3^2)(5.67*10^{-8})(450^4-300^4)

\dot{Q_3} = 780.76W

Therefore the rate heat radiation is 780.76W

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Neko [114]

Answer:

d = 40 m

Explanation:

Given that,

Force, F = 4000 N

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Initial velocity, u = 0 (at rest)

Final velocity, v = 20 m/s

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F = ma

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a is the acceleration of the car.

a=\dfrac{F}{m}\\\\a=\dfrac{4000}{800}\\\\a=5\ m/s^2

Let it has traveled d distance. Using third equation of motion.

v^2-u^2=2ad\\\\d=\dfrac{v^2-u^2}{2a}\\\\d=\dfrac{(20)^2-(0)^2}{2\times 5}\\\\d=40\ m

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Aloiza [94]

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6 0
3 years ago
If the radius of silver is 0.144 nm, what is the PD of the (100) plane for silver in m-2?
Brrunno [24]

Before going to solve this question first we have to understand planar density of a crystal lattice.

Planar density of a plane is given defined-

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Where N is number of atoms centred in the plane and A is the area of the plane.

As per the question we have been given silver.

We know that silver is a face centered cubic crystal. i.e FCC

The radius of silver [r] is given as 0.144 nm.

1 nm=10^{-9} m.

Hence radius r =0.144*10^{-9} m

We have to calculate the PD of [100] plane of silver.

The area of [100] FCC is 8r^2 where r is the radius silver.

The number of atoms centered on [100] plane is 2.It is so because four atoms will be shared by four corners of the cube and there will be one central atom.Hence there will be only two atoms in one unit cell of [100] plane of silver.

Now we have to calculate the planar density PD.We know that-

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                                                               =\frac{2}{8r^2}

                                                               =\frac{2}{8*[0.144*10^{-9}]^2 }

                                                               =12.05632716*10^{18} m^{-2}  [ans]

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\Delta U_{g} = m\cdot g\cdot (z_{f}-z_{o}) (1)

Where:

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g - Gravitational acceleration, measured in meters per square second.

z_{o}, z_{f} - Initial and final height with respect to zero reference, measured in meters.

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The change in potential energy of a 3.0 kilograms backpack carried up the stairs.

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\Delta U_{g} = (650\,N)\cdot (0\,m-4.1\,m)

\Delta U_{g} = -2665\,J

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