Answer: LED have the lowest cost of operation.
Explanation:
If we ignore the initial procurement cost of the items the operational cost of any device consuming electricity is given by
![Cost=Energy\times cost/unit](https://tex.z-dn.net/?f=Cost%3DEnergy%5Ctimes%20cost%2Funit)
Among the three item's LED consumes the lowest power to give the same level of brightness as compared to the other 2 item's thus LED's shall have the lowest operational cost.
Answer:
The difference of head in the level of reservoir is 0.23 m.
Explanation:
For pipe 1
![d_1=50 mm,f_1=0.0048](https://tex.z-dn.net/?f=d_1%3D50%20mm%2Cf_1%3D0.0048)
For pipe 2
![d_2=75 mm,f_2=0.0058](https://tex.z-dn.net/?f=d_2%3D75%20mm%2Cf_2%3D0.0058)
Q=2.8 l/s
![Q=2.8\times 10^{-3]](https://tex.z-dn.net/?f=Q%3D2.8%5Ctimes%2010%5E%7B-3%5D)
We know that Q=AV
![Q=A_1V_1=A_2V_2](https://tex.z-dn.net/?f=Q%3DA_1V_1%3DA_2V_2)
![A_1=1.95\times 10^{-3}m^2](https://tex.z-dn.net/?f=A_1%3D1.95%5Ctimes%2010%5E%7B-3%7Dm%5E2)
![A_2=4.38\times 10^{-3} m^2](https://tex.z-dn.net/?f=A_2%3D4.38%5Ctimes%2010%5E%7B-3%7D%20m%5E2)
![So V_2=0.63 m/s,V_1=1.43 m/s](https://tex.z-dn.net/?f=So%20V_2%3D0.63%20m%2Fs%2CV_1%3D1.43%20m%2Fs)
head loss (h)
![h=\dfrac{f_1L_1V_1^2}{2gd_1}+\dfrac{f_2L_2V_2^2}{2gd_2}+0.5\dfrac{V_1^2}{2g}](https://tex.z-dn.net/?f=h%3D%5Cdfrac%7Bf_1L_1V_1%5E2%7D%7B2gd_1%7D%2B%5Cdfrac%7Bf_2L_2V_2%5E2%7D%7B2gd_2%7D%2B0.5%5Cdfrac%7BV_1%5E2%7D%7B2g%7D)
Now putting the all values
![h=\dfrac{0.0048\times 15\times 1.43^2}{2\times 9.81\times 0.05}+\dfrac{0.0058\times 24\times 0.63^2}{2\times 9.81\times 0.075}+0.5\dfrac{1.43^2}{2\times 9.81}](https://tex.z-dn.net/?f=h%3D%5Cdfrac%7B0.0048%5Ctimes%2015%5Ctimes%201.43%5E2%7D%7B2%5Ctimes%209.81%5Ctimes%200.05%7D%2B%5Cdfrac%7B0.0058%5Ctimes%2024%5Ctimes%200.63%5E2%7D%7B2%5Ctimes%209.81%5Ctimes%200.075%7D%2B0.5%5Cdfrac%7B1.43%5E2%7D%7B2%5Ctimes%209.81%7D)
So h=0.23 m
So the difference of head in the level of reservoir is 0.23 m.
Answer:
At the point when the quantity of bit strings is not exactly the quantity of processors, at that point a portion of the processors would stay inert since the scheduler maps just part strings to processors and not client level strings to processors. At the point when the quantity of part strings is actually equivalent to the quantity of processors, at that point it is conceivable that the entirety of the processors may be used all the while. Be that as it may, when a part string obstructs inside the portion (because of a page flaw or while summoning framework calls), the comparing processor would stay inert. When there are more portion strings than processors, a blocked piece string could be swapped out for another bit string that is prepared to execute, in this way expanding the use of the multiprocessor system.When the quantity of part strings is not exactly the quantity of processors, at that point a portion of the processors would stay inert since the scheduler maps just bit strings to processors and not client level strings to processors. At the point when the quantity of bit strings is actually equivalent to the quantity of processors, at that point it is conceivable that the entirety of the processors may be used at the same time. Be that as it may, when a part string hinders inside the piece (because of a page flaw or while summoning framework calls), the relating processor would stay inert. When there are more portion strings than processors, a blocked piece string could be swapped out for another bit string that is prepared to execute, along these lines expanding the usage of the multiprocessor framework.
Answer:
![10.8\ \text{lb/ft^2}](https://tex.z-dn.net/?f=10.8%5C%20%5Ctext%7Blb%2Fft%5E2%7D)
![101.96\ \text{lb/ft}^2](https://tex.z-dn.net/?f=101.96%5C%20%5Ctext%7Blb%2Fft%7D%5E2)
Explanation:
= Velocity of car = 65 mph = ![65\times \dfrac{5280}{3600}=95.33\ \text{ft/s}](https://tex.z-dn.net/?f=65%5Ctimes%20%5Cdfrac%7B5280%7D%7B3600%7D%3D95.33%5C%20%5Ctext%7Bft%2Fs%7D)
= Density of air = ![0.00237\ \text{slug/ft}^3](https://tex.z-dn.net/?f=0.00237%5C%20%5Ctext%7Bslug%2Fft%7D%5E3)
![v_2=0](https://tex.z-dn.net/?f=v_2%3D0)
![P_1=0](https://tex.z-dn.net/?f=P_1%3D0)
![h_1=h_2](https://tex.z-dn.net/?f=h_1%3Dh_2)
From Bernoulli's law we have
![P_1+\dfrac{1}{2}\rho v_1^2+h_1=P_2+\dfrac{1}{2}\rho v_2^2+h_2\\\Rightarrow P_2=\dfrac{1}{2}\rho v_1^2\\\Rightarrow P_2=\dfrac{1}{2}\times 0.00237\times 95.33^2\\\Rightarrow P_2=10.8\ \text{lb/ft^2}](https://tex.z-dn.net/?f=P_1%2B%5Cdfrac%7B1%7D%7B2%7D%5Crho%20v_1%5E2%2Bh_1%3DP_2%2B%5Cdfrac%7B1%7D%7B2%7D%5Crho%20v_2%5E2%2Bh_2%5C%5C%5CRightarrow%20P_2%3D%5Cdfrac%7B1%7D%7B2%7D%5Crho%20v_1%5E2%5C%5C%5CRightarrow%20P_2%3D%5Cdfrac%7B1%7D%7B2%7D%5Ctimes%200.00237%5Ctimes%2095.33%5E2%5C%5C%5CRightarrow%20P_2%3D10.8%5C%20%5Ctext%7Blb%2Fft%5E2%7D)
The maximum pressure on the girl's hand is ![10.8\ \text{lb/ft^2}](https://tex.z-dn.net/?f=10.8%5C%20%5Ctext%7Blb%2Fft%5E2%7D)
Now
= 200 mph = ![200\times \dfrac{5280}{3600}=293.33\ \text{ft/s}](https://tex.z-dn.net/?f=200%5Ctimes%20%5Cdfrac%7B5280%7D%7B3600%7D%3D293.33%5C%20%5Ctext%7Bft%2Fs%7D)
![P_2=\dfrac{1}{2}\rho v_1^2\\\Rightarrow P_2=\dfrac{1}{2}\times 0.00237\times 293.33^2\\\Rightarrow P_2=101.96\ \text{lb/ft}^2](https://tex.z-dn.net/?f=P_2%3D%5Cdfrac%7B1%7D%7B2%7D%5Crho%20v_1%5E2%5C%5C%5CRightarrow%20P_2%3D%5Cdfrac%7B1%7D%7B2%7D%5Ctimes%200.00237%5Ctimes%20293.33%5E2%5C%5C%5CRightarrow%20P_2%3D101.96%5C%20%5Ctext%7Blb%2Fft%7D%5E2)
The maximum pressure on the girl's hand is ![101.96\ \text{lb/ft}^2](https://tex.z-dn.net/?f=101.96%5C%20%5Ctext%7Blb%2Fft%7D%5E2)
Answer:
(a)
<em>d</em>Q = m<em>d</em>q
<em>d</em>q =
<em>d</em>T
=
(T₂ - T₁)
From the above equations, the underlying assumption is that
remains constant with change in temperature.
(b)
Given;
V = 2L
T₁ = 300 K
Q₁ = 16.73 KJ , Q₂ = 6.14 KJ
ΔT = 3.10 K , ΔT₂ = 3.10 K for calorimeter
Let
be heat constant of calorimeter
Q₂ =
ΔT
Heat absorbed by n-C₆H₁₄ = Q₁ - Q₂
Q₁ - Q₂ = m
ΔT
number of moles of n-C₆H₁₄, n = m/M
ρ = 650 kg/m³ at 300 K
M = 86.178 g/mol
m = ρv = 650 (2x10⁻³) = 1.3 kg
n = m/M => 1.3 / 0.086178 = 15.085 moles
Q₁ - Q₂ = m
' ΔT
= (16.73 - 6.14) / (15.085 x 3.10)
= 0.22646 KJ mol⁻¹ k⁻¹