A popular quotation states, “There are hundreds of miracles within a single machine; a mechanical engineer calmly explains them with mathematical formulae”. Mechanical engineering is a unique specialization in engineering streams. Modern day mechanical engineering finds its roots from the necessity of designing and fabrication of everything from micro, miniature components to large systems used in daily life (Shingley 1989).

Mechanical engineers should be proficient enough in understanding and applying the concepts of kinematics and thermal engineering in real time engineering requirements. Mechanical engineering can be considered the widest engineering stream, encompassing a range of engineering applications. Mechanical engineering applications include but are not limited to automotive, aerospace applications, MEMS, thermal systems, bio-medical applications, renewable energy applications, energy conservation and conversion, manufacturing, and automation.

Typical mechanical engineers require analysis of materials, mechanics, thermal principles, nano mechanics, vibrations, etc. in their pursuit for design and fabrication of better and more efficient engineering components. Research in classical mechanical engineering requires aptitude and skills in application of advanced mathematical skills and understanding of fundamental mechanical engineering concepts. Computer applications of mechanical engineering include drafting with software, manufacturing through automation, modelling and simulation using computer software, and thermal and mechanical engineering analysis of components using engineering software.

The American Society of Heating, Refrigeration and Air-conditioning Engineers (ASHRAE), The American Society of Mechanical Engineers (ASME), The Society of Automotive Engineers (SAE), and The Institution of Mechanical Engineers(IMechE) are some of the several active professional societies in mechanical engineering. The Major credit for recent developments in Biomechanics viz, design and development of prosthetic limbs, artificial human organs, etc. goes to the advancements in research in mechanical engineering (Mow & Huiskes, 2005). Finite Element Methods and Computational fluid mechanics (Anderson, & Wendt, 1995) is a breakthrough of mechanical engineering in the simulation and modelling part of engineering (ASME n d).

At present, for mechanical engineers with conceptual knowledge, creativity and problem solving skills, there are limitless opportunities for professional excellence.

**References:**

Anderson, J.D. and Wendt, J., 1995. *Computational fluid dynamics* (Vol. 206). New York: McGraw-Hill.

Shigley, J.E., Mischke, C.R., Budynas, R.G., Liu, X. and Gao, Z., 1989.*Mechanical engineering design* (Vol. 89). New York: McGraw-Hill.

Mow, V.C. and Huiskes, R. eds., 2005. *Basic orthopaedic biomechanics & mechano-biology*. Lippincott Williams & Wilkins.

K.Hollerbarch n d. 3-d finite element model development for bio-mechanics – A software demonstration. [July 2012].

ASME n d., Mechanical engineering today and beyond. [12 Aug,2008].

**Question 1:**

Since a refrigeration system operates more efficiently when the condensing temperature is low, evaluate the possibility of cooling the condenser cooling water of the refrigeration system with another refrigeration system. Will the combined performance of the two systems be better, the same, or worse than one individual system? Explain why.

The answer is the combined performance will be worse than one individual system. The following is proof.

Consider the two systems as described above:

where Q_{L} and Q_{H} refer to the heat removed from cooled space and rejected to warm space, respectively. Note that in the combined system, Q_{L2} = Q_{H1 }because the heat rejected from REF1 (Q_{H1}) is received as the cooling load for REF2 (Q_{L2}).

The efficiency of refrigerator is normally defined through the coefficient of performance (COP):

So, we can write the COP for the single system as:

(1)

The COP for the combined system is:

(2)

Note that we have the same desired output as single system Q_{L1. }But Q_{L2} = Q_{H1}, substitute into 2:

(3)

We see that because:

Q_{H2} = Q_{H1} + Q_{W2}

And so:

Q_{H2}> Q_{H1}

By comparing equations 1 and 3, we derrive that** COP _{2} < COP_{1}**

**REFERENCES**

Rajput, R.K., 2000. *Thermal Engineering.* S.Chand Publishers.

**Question 2:**

A two-stage ammonia system using flash-gas removal and intercooling operates on the cycle shown below. The condensing temperature is 35 degrees C. The saturation temperature of the intermediate-temperature evaporator is 0 degrees C, and its capacity is 150KW. The saturation temperature of the low-temperature evaporator is -40 degrees C, and its capacity is 250KW. What is the rate of refrigerant compressed by the high-stage compressor?

Add an adiabatic/isentropic efficiency of the compressors of 85% and THEN solve the problem. Should your answer be higher or lower than the one given in the book?

** **

**Given:**

`T`_{5} = 35^{o}C

`T`_{3} = 0^{o}C

`T`_{1} = -40^{o}C

`Q`_{1} = 150 kW

`Q`_{2} = 250 kW

` = 85% = 0.85`

**Solution:**

Find specific enthalpies at all points shown on the above diagram, using saturated and superheated ammonia vapor tables.

**Point 5.** Here the ammonia is saturated liquid. From saturated vapor table at 35^{o}C we get the enthalpy, and pressure, respectively:

`h`_{5} = h_{f} = 346.8 kJ/kg

`P`

_{5} = 1350.4 kPa

**Point 6. **The throttle valve is isenthalpic, so the enthalpy is

`h`

_{6} = h_{5}= 346.8 kJ/kg

**Point 3. **Here the ammonia is saturated gas. From saturated vapor table at 0^{o}C we get the enthalpy, entropy, and pressure respectively:

`h`

_{3} = h_{g} = 1442.2 kJ/kg

`s`

_{3} = s_{g} = 5.3309 kJ/(kg*K)

`P`

_{3} = 429.6 kPa

**Point 7. **Here the ammonia is saturated liquid. From saturated vapor table at 0^{o}C we get the enthalpy

`h`

_{7} = h_{f} = 180.36 kJ/kg

**Point 8. **The throttle valve is isenthalpic, so the enthalpy is

`h`

_{8} = h_{7} = 180.36 kJ/kg

**Point 1. **Here the ammonia is saturated gas. From saturated vapor table at -40^{o}C we get the enthalpy and entropy, respectively:

`h`

_{1} = h_{g} = 1388.8 kJ/kg

`s`

_{1} = s_{g} = 5.9569 kJ/(kg*K)

**Point 2. **The high-stage compressor is isentropic so the entropy at point 2 is

`s`

_{2} = s_{1} = 5.9569 kJ/(kg*K)

The pressure at point 2 is

`P`

_{2} = P_{3} = 429.6 kPa

Now, from the superheated vapor table and using linear interpolation between pressures 400 kPa and 500 kPa we get for pressure 429.6 kPa near entropy 5.9569 kJ/(kg*K):

`h = 1636.7+(1633.1-1636.7)*(429.6-400)/(500-400) = 1635.6 kJ/kg`

at

`s = 5.9907+(5.8744-5.9907)*(429.6-400)/(500-400) = 5.9563 kJ/(kg*K)`

and

`h = 1682.8+(1679.8-1682.8)*(429.6-400)/(500-400) = 1681.9 kJ/kg`

at

`s = 6.1179+(6.0031-6.1179)*(429.6-400)/(500-400) = 6.0839 kJ/(kg*K)`

Now using linear interpolation, we find enthalpy at point 2 for an ideal low-stage compressor

`h`

_{2} = 1635.6+(1681.9-1635.6)*(5.9569-5.9563)/(6.0839-5.9563) = 1635.8 kJ/kg

Let `h`

be the specific enthalpy at point 2 for real low-stage compressor. Then its isentropic efficiency is given by_{2rfeal}

`= (h`

_{2real} - h_{1})/(h_{2} - h_{1})

From which we get

`h`

_{2real} = h_{1} + *(h_{2} - h_{1})

Which is

`h`

_{2real} = 1388.8+0.85*(1635.8-1388.8) = 1598.8 kJ/kg

**Point 4. **The low-stage compressor is isentropic so the entropy at point 4 is

`s`

_{4} = s_{3} = 5.3309 kJ/(kg*K)

The pressure at point 4 is

`P`

_{4} = P_{5} = 1350.4 kPa = 1.3504 MPa

Now from the superheated vapor table using a linear interpolation between pressures 1.2 MPa and 1.4 MPa we get for pressure 1.3504 MPa near entropy 5.3309 kJ/(kg*K):

`h = 1606.8+(1598.8-1606.8)*(1.3504-1.2)/(1.4-1.2) = 1600.8 kJ/kg`

at

`s = 5.3916+(5.2994-5.3916)*(1.3504-1.2)/(1.4-1.2) = 5.3223 kJ/(kg*K)`

and

`h = 1658.0+(1651.4-1658.0)*(1.3504-1.2)/(1.4-1.2) = 1653.0 kJ/kg`

at

`s = 5.5325+(5.4443-5.5325)*(1.3504-1.2)/(1.4-1.2) = 5.4662 kJ/(kg*K)`

Now, using linear interpolation, we find enthalpy at point 4 for an ideal high-stage compressor

`h`

_{4} = 1600.8+(1653.0-1600.8)*(5.3309-5.3223)/(5.4662-5.3223) = 1603.9 kJ/kg

Similarly to point 2, we get the enthalpy at point 4 for real high-stage compressor

`h`

_{4real} = h_{3} + *(h_{4} - h_{3})

Which is

`h`

_{4real} = 1442.2+0.85*(1603.9-1442.2) = 1579.64 kJ/kg

To find the mass flow rates of refrigerant through intermediate-temperature and low-temperature evaporators, respectively:

`m`

_{1} = Q_{1}/(h_{3} - h_{6}) = 150/(1442.2-346.8) = 0.13693 kg/s

`m`

_{2} = Q_{2}/(h_{1} - h_{8}) = 250/(1388.8-180.36) = 0.20688 kg/s

Letting m_{h} be mass flow rate of refrigerant through the high-stage compressors. Then the steady flow energy equation for the intercooler and flash tank is

`m`

_{2}*h_{2real} + (m_{h} - m_{1})*h_{6} = m_{2}*h_{7} + (m_{h} - m_{1})*h_{3}

Solving for m_{h} gives the answer

`m`

_{h} = m_{1} + m_{2}*(h_{2real} - h_{7})/(h_{3} - h_{6})

Which is

`m`

_{h} = 0.13693+0.20688*(1598.8-180.36)/(1442.2-346.8) = 0.4048 kg/s

This is lower than the former value 0.4118 kg/s for ideal compressors

**REFERENCES**

Rajput, R.K., 2000. *Thermal Engineering.* S.Chand Publishers.

**Question 3:**

A R22 flash-gas removal system has a capacity of 180KW at an evaporating temperature of -30 degrees C when the condensing pressure is 1500KPa. Compute the power requirement for a system with a single compressor. Compute the total power required by the two compressors in the system where there is no intercooling but there is flash-gas removal at 600KPa.

Add an adiabatic/isentropic efficiency of the compressors of 85% and THEN solve the problem. Should your answer be higher or lower than the one given in the book?

**(b) Given:**

`Q`

_{in} = 180 kW

`t`

_{1} = -30^{o}C

`P`

_{2} = P_{4} = P_{5} = 1500 kPa

`P`

_{3} = P_{6} = P_{7} = 600 kPa

` = 85% = 0.85`

**Solution:**

Find the specific enthalpies at all points on the Figure 16-17.

From saturated table we have for saturated liquid near 1500 kPa

** P h _{f}**

Now using linear interpolation find the specific enthalpy at point 5

`h`

_{5} = h_{f }= 248.361+(249.686-248.361)*(1500-1496.5)/(1533.5-1496.5) = 248.486 kJ/kg

The throttle valve at point 6 is isenthalpic, so the specific enthalpy at point 6 is

`h`

_{6} = h_{5} = 248.486 kJ/kg

From saturated table at -30^{o}C we get the specific enthalpy and entropy at point 1 for saturated vapor

`h`

_{1 }= h_{g }= 393.138 kJ/kg

`s`

_{1} = s_{g} = 1.80329 kJ/(kgK)

The saturated table gives near 600 kPa

Using linear interpolation we get for 600 kPa:

`t = 5+(6-5)*(600-583.78)/(602.28-583.78) = 5.87675`

^{o}C

`h`

_{g} = 407.143+(407.489-407.143)*(600-583.78)/(602.28-583.78) = 407.446 kJ/kg

`h`

_{f} = 205.899+(207.089-205.899)*(600-583.78)/(602.28-583.78) = 206.942 kJ/kg

`s`

_{g }= 1.74463+(1.74324-1.74463)*(600-583.78)/(602.28-583.78) = 1.74341 J(kgK)

_{ }

Now we get he enthalpy and entropy at point 3, and enthalpy at point 7:

`h`

_{3} = h_{g} = 407.446 kJ/kg

`s`

_{3} = s_{g} = 1.74341 J(kgK)

`h`

_{7} = h_{f} = 206.942 kJ/kg

The throttle valve at point 8 is isenthalpic, so the specific enthalpy at point 8 is

`h`

_{8} = h_{7} = 206.942 kJ/kg

The flash-gas compressor is isentropic, so the specific entropy at point 4 is

`s`

_{4 }= s_{3} = 1.74341 kJ/(kgK)

From saturated table at pressure 1500 kPa we find the saturation temperature 39^{o}C. Now from superheated table using columns with saturation temperatures 38^{o}C and 40^{o}C find the enthalpies and entropies at column with saturated temperature 39^{o}C near the entropy 1.74341 kJ/(kgK):

`h = (427.155+425.871)/2 = 426.513 at s = (1.7365+1.7287)/2 = 1.73260`

`h = (431.568+430.374)/2 = 430.971 at s = (1.7501+1.7426)/2 = 1.74635`

Now using liner interpolation find the specific enthalpy at point 4 for ideal flash-gas compressor

`h`

_{4} = 426.513+(430.971-426.513)*(1.74341-1.73260)/(1.74635-1.73260) = 430.018 kJ/kg

Let h_{4rfeal} be specific enthalpy at point 4 for real flash-gas compressor. Then its isentropic efficiency is given by

`= (h`

_{4real} - h_{3})/(h_{4} - h_{3})

From which we get

`h`

which is_{4real} = h_{3} + *(h_{4} - h_{3}),

`h`

_{4real} = 407.446+0.85*(430.018-407.446) = 426.63 kJ/kg

The evaporator compressor is isentropic, so the specific entropy at point 2 is

`s`

_{2 }= s_{1} = 1.80329 kJ/(kgK)

Similarly to the above from the superheated table we get near the entropy 1.80329 kJ/(kgK):

`h = (448.703+447.771)/2 = 448.237 at s = (1.8008+1.7940)/2 = 1.7974`

`h = (452.901+452.019)/2 = 452.46 at s = (1.8127+1.8061)/2 = 1.8094`

Now we can get the enthalpy at point 2 for an ideal evaporator compressor

`h`

_{2} = 448.237+(452.46-448.237)*(1.80329-1.7974)/(1.8094-1.7974) = 450.301 kJ/kg

The specific enthalpy at point 2 for a real evaporator compressor is given by

`h`

which is_{2real} = h_{1} + *(h_{2} - h_{1})

`h`

_{2real} = 393.138+ 0.85*(450.301-393.138) = 441.73 kJ/kg

Let m_{1} and m_{2} be mass flow through evaporator and flash-gas compressors, respectively. The mass flow m_{1} is given by

`m`

_{1} = Q_{in}/(h_{1} - h_{8}) = 180/(393.138-206.942) = 0.96672 kg/s

The steady flow energy equation for points 3-6-7 gives

`(m`

_{1} + m_{2})*h_{6} = m_{1}*h_{7} + m_{2}*h_{3}

From which we get m_{2}

`m`

which is_{2} = m_{1}*(h_{6}-h_{7})/(h_{3}-h_{6})

`m`

_{2} = 0.96672*(248.486-206.942)/(407.446-248.486) = 0.25265 kg/s

The power required by the evaporator and flash-gas compressors are given by, respectively:

`W`

_{1} = m_{1}*(h_{2real} - h_{1})

`W`

_{2} = m_{2}*(h_{4real} - h_{3})

Now we can find the total power required by two compressors

`W = W`

_{1} + W_{2} = m_{1}*(h_{2real} - h_{1}) + m_{2}*(h_{4real} - h_{3})

which is

`W = 0.96672*(441.73-393.138)+0.25265*(426.63-407.446) = 51.82 kW`

This is lower than the former value 60.96 kW for ideal compressors.

**REFERENCES**

Rajput, R.K., 2000. *Thermal Engineering.* S.Chand Publishers.

**Question 4:**

In a R22 refrigeration system the capacity is 180KW at a temperature of -30 deg C. The vapour from the evaporator is pumped by one compressor to the condensing pressure of 1500KPa. Later the system is revised to two-stage compression operating on a cycle with intercooling but no removal of flash gas at 600KPa. Calculate the power required from a single compressor in the original system? Calculate the power required from two compressors in the revised system?

** **

**(a) Given:**

Q_{in} = 180 kW

t_{1} = -30^{o}C

P_{2} = 1500 kPa

**Solution:**

Find the specific enthalpies at all points in the above original one evaporator - one compressor refrigeration system, using Table A-6 for saturated and Table A-7 for superheated Refrigerant 22

From the saturated table we have for saturated liquid near 1500 kPa

** P h _{f}**

_{}

Using linear interpolation find the specific enthalpy at point 3:

`h`

_{3} = h_{f }= 248.361+(249.686-248.361)*(1500-1496.5)/(1533.5-1496.5) = 248.486 kJ/kg

The throttle valve is isenthalpic, so the specific enthalpy at point 4 is

`h`

_{4} = h_{3} = 248.486 kJ/kg

From saturated table at -30^{o}C we get the specific enthalpy and entropy at point 1 for saturated vapor

`h`

_{1 }= h_{g }= 393.138 kJ/kg

`s`

_{1} = s_{g} = 1.80329 kJ/(kgK)

The compressor is isentropic, so the specific entropy at point 2 is

`s`

_{2 }= s_{1} = 1.80329 kJ/(kgK)

From the saturated table at pressure 1500 kPa we find the saturation temperature 39^{o}C. Now from the superheated table using columns with saturation temperatures 38^{o}C and 40^{o}C find the enthalpies and entropies at column with saturated temperature 39^{o}C near the entropy 1.80329 kJ/(kgK):

`h = (448.703+447.771)/2 = 448.237 for s = (1.8008+1.7940)/2 = 1.7974`

`h = (452.901+452.019)/2 = 452.460 for s = (1.8127+1.8061)/2 = 1.8094`

Now using liner interpolation find the specific enthalpy at point 2

`h`

_{2} = 448.237+(452.460-448.237)*(1.80329-1.7974)/(1.8094-1.7974) = 450.310 kJ/kg

Find the mass flow rate of refrigerant

`m = Q`

_{in}/(h_{1} - h_{4}) = 180/(393.138-248.486) = 1.24437 kg/s

Now we can find the power of the compressor required

`W = m*(h`

_{2} - h_{1}) = 1.24437*(450.310- 393.138) = 71.1 kW

**(b) Given:**

`Q`

_{in} = 180 kW

`t`

_{1} = -30^{o}C

`P`

_{4} = 1500 kPa

`P`

_{2} = P_{3} = P_{6} = 600 kPa

Now find the specific enthalpies at all points in the above figure.

From the saturated table we have for saturated liquid near 1500 kPa

** P h _{f}**

Now using linear interpolation find the specific enthalpy at point 5

`h`

_{5} = h_{f }= 248.361+(249.686-248.361)*(1500-1496.5)/(1533.5-1496.5) = 248.486 kJ/kg

The throttle valve is isenthalpic, so the specific enthalpy at points 6 and 7 is

`h`

_{6} = h_{7} = h_{5} = 248.486 kJ/kg

From saturated table at -30^{o}C we get the specific enthalpy and entropy at point 1 for saturated vapor

`h`

_{1 }= h_{g }= 393.138 kJ/kg

`s`

_{1} = s_{g} = 1.80329 kJ/(kgK)

The low-stage compressor is isentropic, so the specific entropy at point 2 is

`s`

_{2 }= s_{1} = 1.80329 kJ/(kgK)

The saturated table gives near 600 kPa

Using linear interpolation we get for 600 kPa:

`t = 5+(6-5)*(600-583.78)/(602.28-583.78) = 5.87675`

^{o}C

`h`

_{g} = 407.143+(407.489-407.143)*(600-583.78)/(602.28-583.78) = 407.446 kJ/kg

`s`

_{g }= 1.74463+(1.74324-1.74463)*(600-583.78)/(602.28-583.78) = 1.74341 J(kgK)

_{ }

Now we get he enthalpy and entropy at point 3:

`h`

_{3} = h_{g} = 407.446 kJ/kg

`s`

_{3} = s_{g} = 1.74341 J(kgK)

_{ }

From the superheated table using columns with saturation temperatures 5^{o}C and 10^{o}C find the enthalpies and entropies at column with saturated temperature 5.87675^{o}C near the entropy 1.80329 kJ/(kgK):

`h = 425.562+(423.974-425.562)*(5.87675-5)/(10-5) = 425.284`

`for s = 1.8080+(1.7894-1.8080)*(5.87675-5)/(10-5) = 1.80474`

and

`h = 429.229+(427.724-429.229)*(5.87675-5)/(10-5) = 428.965`

`for s = 1.8200+(1.8017-1.8200)*(5.87675-5)/(10-5) = 1.81679`

Now using liner interpolation find the specific enthalpy at point 2

`h`

_{2 }= 425.284+(428.965-425.284)*(1.80329-1.80474)/(1.81679-1.80474) = 424.841 kJ/kg

The high-stage compressor is isentropic, so the specific entropy at point 4 is

`s`

_{4 }= s_{3} = 1.74341 J(kgK)

From the saturated table at pressure 1500 kPa we find the saturation temperature 39^{o}C. Now from the superheated table using columns with saturation temperatures 38^{o}C and 40^{o}C find the enthalpies and entropies at column with saturated temperature 39^{o}C near the entropy 1.74341 kJ/(kgK):

`h = (427.155+425.871)/2 = 426.513 at s = (1.7365+1.7287)/2 = 1.73260`

`h = (431.568+430.374)/2 = 430.971 at s = (1.7501+1.7426)/2 = 1.74635`

Now using liner interpolation find the specific enthalpy at point 4

`h`

_{4} = 426.513+(430.971-426.513)*(1.74341-1.73260)/(1.74635-1.73260) = 430.018 kJ/kg

Let m_{1} and m_{2} be mass flow through low-stage and high-stage compressors, respectively.

The mass flow m_{1} is given by

`m`

_{1} = Q_{in}/(h_{1} - h_{7}) = 180/(393.138-248.486) = 1.24437 kg/s

The steady flow energy equation for intercooler gives

`(m`

_{2} - m_{1})*h_{6} + m_{1}*h_{2} = m_{2}*h_{3}

From which we get m_{2}

`m`

_{2} = m_{1}*(h_{2}-h_{5})/(h_{3}-h_{5})

Which is

`m`

_{2} = 1.24437*(424.841-248.486)/(407.446-248.486) = 1.38054 kg/s

The powers required by low-stage and high-stage compressors are given by, respectively:

`W`

_{1} = m_{1}*(h_{2} - h_{1})

`W`

_{2} = m_{2}*(h_{4} - h_{3})

Now we can find the total power required by two compressors

`W = W`

_{1} + W_{2} = m_{1}*(h_{2} - h_{1}) + m_{2}*(h_{4} - h_{3})

Which is

`W = 1.24437*(424.841-393.138) + 1.38054*(430.018-407.446) = 70.6 kW`

**Question 5:**

A refrigeration system using R22 is to have a refrigerating capacity of 80KW. The cycle is standard vapour-compression cycle in which the evaporating temperature is -8 deg C and the condensing temperature is 42 deg C.

Determine the volume flow of refrigerant measured in cubic meters per second at the inlet to the compressor.

Calculate the power required by the compressor.

At the entrance to the evaporator what is the fraction of vapour in the mixture expressed both on a mass basis and a volume basis?

**Given:**

`Q`

_{in} = 40 kW

`T`

_{1} = -8^{o}C

`T`

_{3} = 42^{o}C

**Solution:**

Refer to above diagram of the refrigeration system, and find the specific enthalpies at all points.

From the saturated vapor table at 42^{o}C find the specific enthalpy at point 3 for saturated liquid

`h`

_{3} = h_{f }= 252.352 kJ/kg

The throttle valve is isenthalpic, so the same specific enthalpy is at point 4

`h`

_{4} = h_{3} = 252.352 kJ/kg

From the saturated vapor table at -8^{o}C we get the specific enthalpy, specific entropy, specific volume, and pressure at point 1 for saturated vapor, respectively:

`h`

_{1 }= h_{g }= 402.341 kJ/kg

`s`

_{1} = s_{g} = 1.76394 kJ/(kgK)

`v`

_{1} = v_{g} = 61.0958 L/kg = 0.0610958 m^{3}/kg

`P`

_{1} = 380.06 kPa

The compressor is isentropic, so the specific entropy at point 2 is

`s`

_{2 }= s_{1} = 1.76394 kJ/(kgK)

From the superheated vapor table at saturation temperature 42^{o}C we have the enthalpy and entropy near the entropy 1.76394 kJ/(kgK):

** h s**

Using linear interpolation we get the specific enthalpy at point 2

`h`

_{2} = 438.062+(442.449-438.062)*(1.76394-1.7618)/(1.7747-1.7618) = 438.790 kJ/kg

Now we get:

(a) The specific heat received by evaporator is given by

`q`

_{in} = h_{1} - h_{4} = 402.341-252.352 = 149.989 kJ/kg

So the mass flow of refrigerant is

`M = Q`

_{in}/q_{in} = 40/149.989 = 0.266686 kg/s

Now we can get the volume flow rate at the inlet of compressor

`V = m*v`

_{1} = 0.266686*0.0610958 = 0.0162934 or 0.0163 m^{3}/s

(b) Find specific power of the compressor

`w = w = h`

_{2} - h_{1 }= 438.790-402.341 = 36.4490 kJ/kg

Now we can find power of the compressor

`W = w*M = 36.4490*0.266686 = 9.72044 9.72 kW`

(c) The pressure at point 4 is

`P`

_{4} = P_{1} = 380.06 kPa

From the saturated vapor table at 380.06 kPa we get the specific enthalpies and specific volumes for saturated liquid and vapor, respectively:

`h`

_{f} = 190.718 kJ/kg

`h`

_{g} = 402.341 kJ/kg

`v`

_{f} = 0.76253 L/kg

`v`

_{g} = 61.0958 L/kg

The fraction of vapor in the mixture at the entrance of the evaporator, at point 4, expressed on a mass basis is given by:

`x`

_{4m} = (h_{4} - h_{f})/(h_{g} - h_{f}) = (252.352-190.718)/(402.341-190.718) = 0.29124 or 0.291

(d) Find specific volume at point 4

`v`

_{4} = (1 - x_{4m})*v_{f} + x_{4m}*v_{g} = (1-0.29124)*0.76253+0.29124*61.0958 = 18.3340 L/kg

The fraction of vapor in the mixture at the entrance of the evaporator expressed on a volume basis is given by:

`x`

_{4v} = (1/v_{4}-1/v_{f})/(1/_{g}-1/v_{f}) = (1/8.3340-1/0.76253)/(1/61.0958-1/0.76253) = 0.971

**Question 6:**

If in a standard vapor compression cycle using R22 refrigerant the evaporating temperature is -5 deg C and the condensing temperature is 30 deg C, sketch the cycle on pressure-enthalpy coordinates and calculate the work of compression, the refrigerating effect, and the heat rejected in the condenser in KJ/Kg and the corresponding COP as well.

**Given:**

`T`

_{1} = -5^{o}C

`T`

_{3} = 30^{o}C

**Solution:**

The diagram of the vapor-compression cycle is shown above, where: P_{1}=P_{4}; P_{2}=P_{3}

The corresponding cycle on pressure-enthalpy coordinates is drawn below

Find enthalpies at all points using Table A-6 for saturated Refrigerant 22 and Table A-7 for superheated Refrigerant 22

From the saturated vapor table at 30^{o}C we get the specific enthalpy and pressure, respectively, at point 3 for saturated liquid:

`h`

_{3} = h_{f }= 236.664 kJ/kg

`P`

_{3} = 1191.9 kPa

Since the throttle valve is isenthalpic the specific enthalpy at point 4 is

`h`

_{4} = h_{3} = 236.664 kJ/kg

From saturated vapor table at -5^{o}C we get the specific enthalpy and entropy at point 1 for saturated vapor:

`h`

_{1 }= h_{g }= 403.496 kJ/kg

`s`

_{1} = s_{g} = 1.75928 kJ/(kgK)

Since the compressor is isentropic the specific entropy at point 2 is

`s`

_{2 }= s_{1} = 1.75928 kJ/(kgK)

The pressure at point 2 is

P_{2} = P_{3} = 1191.9 kPa

From superheated vapor table at saturation temperature 30^{o}C we have the enthalpy and entropy near entropy 1.75928 kJ/(kgK):

h s

Using linear interpolation we get the specific enthalpy at point 2

`h`

_{2} = 427.378+(431.549-427.378)*(1.75928-1.7534)/(1.7664-1.7534) = 429.265 kJ/kg

Now we get:

(a) The work of compression is given by

`w = h`

_{2} - h_{1}

which is

`w = 429.265-403.496 = 25.769 25.8 kJ/kg`

(b) The refrigerating effect is given by

`q`

_{in} = h_{1} - h_{4}

which is

`q`

_{in} = 403.496-236.664 = 166.832 167 kJ/kg

(c) The heat rejected in the condenser is given by

`q`

_{out} = h_{2} - h_{3}

which is

`q`

_{out} = 429.265-236.664 = 192.601 193 kJ/kg

(d) The coefficient of performance is given by

`COP = q`

_{in}/w

Which is

`COP = 166.832/25.769 = 6.47`

**REFERENCES**

Rajput, R.K., 2000. *Thermal Engineering.* S.Chand Publishers.

**Question 1:**

Derive the response of viscously damped SDOF system to the force F(t) by means of the convolution integral and plot the response for the system.

Solution

The equation of motion of a single degree of freedom system is

Natural frequency:

Damping ratio:

The impulse response function when

Given force ,

The response of the system is

Thus,

The response of the system with given force is

**Question 2**

Plot the response of a viscously damped force free system.

(a) Given:

x(0) = 2 cm

x'(0) = 0

ω_{n} = 5 rad/s = frequency of undamped oscillation

ς = 0.1

Solution:

We have the differential equation for oscillations

x'' + 2ςω_{n}x' + ω_{n}^{2}x = 0 (1)

The general solution is given by

*x*(t) = X_{o} exp(-ςω_{n}t) cos(ω_{n}√(1- ς^{2})^{ }t + φ) (2)

Differentiating gives

x'(t) = -X_{o}ω_{n} exp(ςω_{n}-t) [ς cos(ω_{n}√(1- ς^{2})^{ }t + φ) + √(1- ς^{2}) sin(ω_{n }√(1- ς^{2}) t + φ)]

Substituting the initial conditions gives:

x'(0) = -X_{o}ω_{n}(ς cos φ + √(1- ς^{2} sin φ) = 0

*x*(0) = X_{o} cos φ = 2

From which we get:

The graph of *x*(t) for damping factor =0.1 is drawn below

(b) Now the formula (2) in part (a) gives the general solution for ς = 1

*x*(t) = (X_{o} cos φ) exp(-ω_{n}t)

Substituting the initial conditions gives the system of equations:

x'(0) = -X_{o} ω_{n }cos φ = 0

*x*(0) = X_{o} cos φ = 2

From the first equation we get

cos φ = 0

Substituting it into the second equation we get that the X_{o} is infinitely large. So the system of equations has no physical solution for the given initial conditions

(c) Now the differential equation (2) in part (a) gives for ς = 2 and ω_{n }= 5

x'' + 20x' + 25*x* = 0

Find the solution in form

*x* = exp(-pt)

Put it into the above equation and get the equation for p

p^{2} - 20p + 25 = 0

Solving for p gives

p = 10± √(10^{2}-25) = 10 ± √75

Thus the general solution is

*x*(t) = X_{1}exp[-(10 + √75)t] + X_{2}exp[-(10 - √75)t]

The initial conditions give the system of equations:

x'(0) = -X_{1}(10 + √75) - X_{2}(10 - √75) = 0

*x*(0) = X_{1} + X_{2} = 2

Solving for X_{1 }and X_{2} gives:

X_{1 }= -0.155

X_{2} = 2.15

Thus the equation is

*x*(t) = -0.155exp[-(10 + √75)t] + 2.15exp[-(10 - √75)t]

The graph is drawn below

n

References

Meirovitch, L., 2010, *Fundamentals of Vibrations,* Waveland Pr Inc

Traditionally mechanical engineering is considered to be made of three mainstream engineering aspects: manufacturing engineering, thermal engineering and design engineering. To excel in the domain a thorough knowledge of all of these is essential. A practicing mechanical engineer must solve many problems every day in all these subdomains.

** **

**Shaper cutting time**

*Consider a shaper machine is working to smooth a surface plate of length 400mm. Assume the feed of the shaper tool is 2mm/stroke and it is working at a speed of 50 strokes per minute. Determine the time it takes for the shaper to complete machining of the surface of the shaper machine.*

The length of the travel needed on the job, L_{w} is 400mm

Assuming a reasonable approach (A) and overrun (O) as 2 mm each, the length of cut required for shaper machine is Lw+A+O = 400 + 2+ 2 = 404 mm.

The feed of the shaper (S_{o}) is 2mm/stroke

The speed of the shaper is (N_{s}) = 50 strokes/minute, hence the time it takes to complete the cutting process = (L_{w}+A+O)/N_{s}*S_{o} = 404/2*50 = 4.04 minutes.

**Milling cutting time calculation**

*Determine the milling time required for milling a rectangular plate of length 100mm, width 50mm by a helical fluted plain HSS milling cutter of diameter 60mm and length 75mm and 6 teeth. *

Assume A = O = 5mm, Vc = 40m/min and So = 0.1mm/teeth.

Cutting time Tc = Length of travel (Lc)/Table Feed (Sm)

Length of travel (Lc) = Length of work piece (Lw) + Approach (A) + Overrun (O) + (1/2 x Diameter of the rod)

Table feed(Sm) = So x Zc x N

So = Feed per teeth

Zc = Number of teeth on the cutter

N = Speed of the cutter

Lc = 100mm + 5mm + 5mm + 30mm = 140mm

Sm = 0.1 x 6 x N

N = (1000 x Vc)/(∏ x Dc) = (1000 x 40)/(∏ x 60) = 212.31rpm or ~213rpm

Sm = 0.1 x 6 x 213 = 127.8mm/min

Hence the Cutting time = Lc/Sm = 140/127.88 = 1.09minutes.

**Casting and metal flow problems**

*Consider the case of a metal mold with a sprue length of 20cm and a cross sectional area at the base of the sprue of 2.5 cm ^{2}. If the sprue feeds a horizontal runner leading into a mold cavity whose volume is 1560 cubic centimeter. Determine *

*a) the velocity of the molten metal at the base of the sprue;**b) volume flow rate of the molten metal; and**c) the time it takes to fill the mold.*

For determining the flow rate of the molten metal at the bottom of the sprue pin, Bernoulli’s principle is required. As per Bernoulli’s principle the pressure at the top of the sprue should be converted to the velocity at the bottom of the sprue, so it will be given by the equation:

V = sqrt (2*g*h), where h is the height of the sprue, V is the velocity of the molten metal at the bottom of the sprue,

So in the given problem

- A) Flow velocity of the molten metal, V = sqrt (2*9.81*100*20) = 198.1 cm/s
- B) The flow rate of the molten metal at the bottom of the sprue pin is given by Q = A * V

Where A is the area of cross section of the sprue pin and V is the velocity of the molten metal,

dQ/dt = 2.5 * 198.1 = 495.25 cubic centimeters/s.

- C) Time it takes to fill the mold = Q’/(dQ/dt) = 1560/495.25 = 3.15 seconds

**Steady flow Energy Equation**** (first law of thermodynamics) and the principle of energy conservation**

*0.5 kg/s of fluid flows in a steady state process. The properties of fluid at the entrance are measured as *

*p _{1} = 1.4bar, and the density of the fluid is 2.5kg/m3. *

*U _{i} = 920kJ/kg while at exit the properties are P_{2 }= 5.6bar, density = 5kg/m3, U_{2} = 720KJ/kg. *

*The velocity at entrance is 200m/s, while at exit it is 180m/s. It rejects 60KW of heat and raises through 60m during the flow process. Determine the change of enthalpy as well as the work done during the process.*

The key to the solution is the fact that the total energy remains constant during the process.

Mass flow rate of fluid in the process = mf = 0.5kg/s

Pressure at the inlet to the process = 1.4bar

Density of the fluid = 2.5kg/m3

Initial internal energy of the fluid = 920KJ/kg

Final pressure of the fluid = 5.6bar

Final density at the exit = 5kg/m3

Final internal energy of the fluid =720kJ/kg

Velocity of the fluid at the entrance = 200m/s

Velocity of the fluid at the exit = 180m/s

The amount of the heat given to the fluid during the process = 60KW

The rise in height of the fluid during the process = 60m

Enthalpy change during the process (h2-h1) = ∆(U2-U1) + ∆PV

Therefore, ∆PV = p2/ρ2 – p1/ρ1.

Specific enthalpy change = (720 - 920) x 10^{3} + (5.6/5 - 1.4/2.5) x 10^{5} = -144KJ/kg

Hence Enthalpy change = ∆H = mf x (h2-h1) = 0.5 x (-144) = -72 KJ/s

The steady flow energy equation (SFEE) can be applied as:

SFEE - Q - WS = mf [(h2 – h1) + ½( V_{2}^{2} –V_{1}^{2}) + g(Z2 –Z1)]

60 x 10^{3 }- Ws = 0.5 x (-144 + 0.5 x (180^{2} -200^{2}) + 9.81 x 60)

Hence Ws = 13605.7W = 136.1KW

**Principle of energy conservation**

*0.25kg/s of water is heated from 30 ^{o}C to 60^{0}C by hot gasses that enter at 180^{0}C and leave at 80^{0}C. Calculate the mass flow rate of gases when its specific heat at constant pressure is 1.08 KJ/kg - K. Find the entropy change of water and of hot gases. Take the specific heat of water as 4.186KJ/kg - K*

The total energy entering the system should be equal to the energy leaving the system. The system is being heated by the hot gases entering and it is being cooled by the water leaving the system.

The temperature of the exhaust gas entering into the system = 180 degree Celsius

The temperature of the exhaust gas leaving the system = 80 degree Celsius.

The specific heat at constant pressure of the exhaust gases = 1.08KJ/kg - K

The specific heat of water = 4.1868KJ/kg - K

Water flow rate = 0.25kg/s

The heat intake from the exhaust gases = mg x Cpg x (Tg1-Tg2)* (1)*

.mg is the mass of the exhaust gases entering into the system

Cpg is the specific heat of the exhaust gases

Tg1 is the temperature of the exhaust gases entering into the system

Tg2 is the temperature of the exhaust gases leaving the system

The heat carried away by water = mw x Cpw x (Tw2 - Tw1) *(2)*

Mw is the mass of water = 0.25kg/s

CPw is the specific heat of water = 4.1868KJ/kg-K

Tw1 = 30^{o}C

Tw2 = 60^{0}C

Equating equations 1 and 2, Mg x 1.08 x (180-80) = 0.25 x 4.1868 x (60 - 30), which yields that the mass flow rate of exhaust gases = 0.291kg/s.

Entropy change of hot water is calculable by: mw x Cpw x ln(Tw2/Tw1) = 0.25 x 4.1868 x ln(273 + 60/273 + 30)

S2 – S1 = 0.25 x 4.186 x ln(Tw2/Tw1) = 0.099KJ/kg-K

Entropy change of Exhaust gases = 0.291 x 1.08 x ln(80+273)/(180+273) = -0.0783KJ/kg-K.

**Machine Design**

*You are required to design a pulley, B, given that the diameter of a pulley A is 300mm and the speed of rotation of pulley A is 250rpm. The belt thickness is 6mm. Determine the diameter of the pulley B, if it is rotating at a speed of 750rpm*

For the belt drive to function the surface velocity of the pulley A should be same as the surface velocity of the pulley B.

The surface velocity of the pulley A = ∏ x 0.3 x 250/60 = 3.925m/s

Considering the surface velocity of the pulley as same, its diameter will be given by ∏ x D x 750/60 = 3.925m/s, where D = 100mm.

*Suppose a shaft is made of a material with shear stress of 50Mpa and if the maximum torque that can act on the shaft is 200N-m, design the shaft diameter considering a factor of safety of 3.*

Let T be the torque of the shaft = 200N-m,

The shear stress of the shaft material (fs) will be given by, T = ∏/16 x fs x d^{3}

In the given scenario diameter d is 2.73cm = 3 cm.

Considering the factor of safety of 3, diameter of the shaft = 3 x 3 = 9cm.

**References:**

Grote, K.H. and Antonsson, E.K., 2009. *Springer handbook of mechanical engineering* (Vol. 10). Springer Science & Business Media.

Kreith, F., 1999. Mechanical engineering handbook.

Jain, R.K., 1995. *Machine design*. Khanna Publishers.

Ballaney, P.L., 1981. *Thermal Engineering*. Khanna.

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