Answer: required tensile stress is 0.889 MPa
Explanation:
Given that;
tensile load is oriented along the [1 1 1] direction
shear stress is 0.242 MPa along [1 0 1] in the (1 1 -1) plane
first we determine
λ which is Angle between [1 1 1] and [1 0 1]
so
cosλ = [ 1(1) + 1(0) + 1(1) ] / [ √(1² + 1² + 1²) √(1² + 0² + 1²)]
= 2 / √3√2 = 2/√6
Next, we determine ∅ which is angle between [1 1 1] and [1 1 -1]
so,
cos∅ = [ 1(1) + 1(1) + 1(-1) ] / [ √(1² + 1² + 1²) √(1² + 1² + (-1)²)]
cos∅ = [ 2-1] / [√3√3 ]
cos∅ = 1/3
Now, we know that;
σ = T_stress/cosλcosθ
so we substitute
σ = 0.242 / ( 2/√6 × 1/3 )
σ = 0.242 / 0.2721
σ = 0.889 MPa
Therefore, required tensile stress is 0.889 MPa
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Answer:
The volume percentage of graphite is 10.197 per cent.
Explanation:
The volume percent of graphite is the ratio of the volume occupied by the graphite phase to the volume occupied by the graphite and ferrite phases. The weight percent in the cast iron is 3.2 wt% (graphite) and 96.8 wt% (ferrite). The volume percentage of graphite is:
![\%V_{gr} = \frac{V_{gr}}{V_{gr}+V_{fe}} \times 100\,\%](https://tex.z-dn.net/?f=%5C%25V_%7Bgr%7D%20%3D%20%5Cfrac%7BV_%7Bgr%7D%7D%7BV_%7Bgr%7D%2BV_%7Bfe%7D%7D%20%5Ctimes%20100%5C%2C%5C%25)
Where:
- Volume occupied by the graphite phase, measured in cubic centimeters.
- Volume occupied by the graphite phase, measured in cubic centimeters.
The expression is expanded by using the definition of density and subsequently simplified:
![\%V_{gr} = \frac{\frac{m_{gr}}{\rho_{gr}} }{\frac{m_{gr}}{\rho_{gr}}+\frac{m_{fe}}{\rho_{fe}}}\times 100\,\%](https://tex.z-dn.net/?f=%5C%25V_%7Bgr%7D%20%3D%20%5Cfrac%7B%5Cfrac%7Bm_%7Bgr%7D%7D%7B%5Crho_%7Bgr%7D%7D%20%7D%7B%5Cfrac%7Bm_%7Bgr%7D%7D%7B%5Crho_%7Bgr%7D%7D%2B%5Cfrac%7Bm_%7Bfe%7D%7D%7B%5Crho_%7Bfe%7D%7D%7D%5Ctimes%20100%5C%2C%5C%25)
Where:
,
- Masses of the ferrite and graphite phases, measured in grams.
- Densities of the ferrite and graphite phases, measured in grams per cubic centimeter.
![\%V_{gr} = \frac{1}{1+\frac{\frac{m_{fe}}{\rho_{fe}} }{\frac{m_{gr}}{\rho_{gr}} } }\times 100\,\%](https://tex.z-dn.net/?f=%5C%25V_%7Bgr%7D%20%3D%20%5Cfrac%7B1%7D%7B1%2B%5Cfrac%7B%5Cfrac%7Bm_%7Bfe%7D%7D%7B%5Crho_%7Bfe%7D%7D%20%7D%7B%5Cfrac%7Bm_%7Bgr%7D%7D%7B%5Crho_%7Bgr%7D%7D%20%7D%20%7D%5Ctimes%20100%5C%2C%5C%25)
![\%V_{gr} = \frac{1}{1 + \left(\frac{\rho_{gr}}{\rho_{fe}} \right)\cdot\left(\frac{m_{fe}}{m_{gr}} \right)} \times 100\,\%](https://tex.z-dn.net/?f=%5C%25V_%7Bgr%7D%20%3D%20%5Cfrac%7B1%7D%7B1%20%2B%20%5Cleft%28%5Cfrac%7B%5Crho_%7Bgr%7D%7D%7B%5Crho_%7Bfe%7D%7D%20%5Cright%29%5Ccdot%5Cleft%28%5Cfrac%7Bm_%7Bfe%7D%7D%7Bm_%7Bgr%7D%7D%20%5Cright%29%7D%20%5Ctimes%20100%5C%2C%5C%25)
If
,
,
and
, the volume percentage of graphite is:
![\%V_{gr} = \frac{1}{1+\left(\frac{2.3\,\frac{g}{cm^{3}} }{7.9\,\frac{g}{cm^{3}} } \right)\cdot \left(\frac{96.8\,g}{3.2\,g} \right)} \times 100\,\%](https://tex.z-dn.net/?f=%5C%25V_%7Bgr%7D%20%3D%20%5Cfrac%7B1%7D%7B1%2B%5Cleft%28%5Cfrac%7B2.3%5C%2C%5Cfrac%7Bg%7D%7Bcm%5E%7B3%7D%7D%20%7D%7B7.9%5C%2C%5Cfrac%7Bg%7D%7Bcm%5E%7B3%7D%7D%20%7D%20%5Cright%29%5Ccdot%20%5Cleft%28%5Cfrac%7B96.8%5C%2Cg%7D%7B3.2%5C%2Cg%7D%20%5Cright%29%7D%20%5Ctimes%20100%5C%2C%5C%25)
![\%V_{gr} = 10.197\,\%V](https://tex.z-dn.net/?f=%5C%25V_%7Bgr%7D%20%3D%2010.197%5C%2C%5C%25V)
The volume percentage of graphite is 10.197 per cent.
Answer:
The pressure drop across the pipe also reduces by half of its initial value if the viscosity of the fluid reduces by half of its original value.
Explanation:
For a fully developed laminar flow in a circular pipe, the flowrate (volumetric) is given by the Hagen-Poiseulle's equation.
Q = π(ΔPR⁴/8μL)
where Q = volumetric flowrate
ΔP = Pressure drop across the pipe
μ = fluid viscosity
L = pipe length
If all the other parameters are kept constant, the pressure drop across the circular pipe is directly proportional to the viscosity of the fluid flowing in the pipe
ΔP = μ(8QL/πR⁴)
ΔP = Kμ
K = (8QL/πR⁴) = constant (for this question)
ΔP = Kμ
K = (ΔP/μ)
So, if the viscosity is halved, the new viscosity (μ₁) will be half of the original viscosity (μ).
μ₁ = (μ/2)
The new pressure drop (ΔP₁) is then
ΔP₁ = Kμ₁ = K(μ/2)
Recall,
K = (ΔP/μ)
ΔP₁ = K(μ/2) = (ΔP/μ) × (μ/2) = (ΔP/2)
Hence, the pressure drop across the pipe also reduces by half of its initial value if the viscosity of the fluid reduces by half of its value.
Hope this Helps!!!