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valentina_108 [34]
3 years ago
9

A work element in a manual assembly task consists of the following MTM-1 elements: (1) R16C, (2) G4A, (3) M10B5, (4) RL1, (5) R1

4B, (6) G1B, (7) M8C3, (8) P1NSE, and (9) RL1.
(a) Determine the normal times in TMUs for these motion elements.
(b) What is the total time for this work element in sec
Engineering
1 answer:
ella [17]3 years ago
7 0

Answer:

a)

1) R16C ; Tn = 17 TMU

2) G4A ; Tn = 7.3 TMU

3) M10B5 ; Tn = 15.1 TMU

4) RL1 ; Tn = 2 TMU

5) R14B ; Tn = 14.4 TMU

6) G1B ; Tn = 3.5 TMU

7) M8C3 ; Tn = 14.7 TMU

8) P1NSE ; Tn = 10.4 TMU

9) RL1 ; Tn = 2 TMU

b) 3.1 secs

Explanation:

a) Determine the normal times in TMUs for these motion elements

1) R16C ; Tn = 17 TMU

2) G4A ; Tn = 7.3 TMU

3) M10B5 ; Tn = 15.1 TMU

4) RL1 ; Tn = 2 TMU

5) R14B ; Tn = 14.4 TMU

6) G1B ; Tn = 3.5 TMU

7) M8C3 ; Tn = 14.7 TMU

8) P1NSE ; Tn = 10.4 TMU

9) RL1 ; Tn = 2 TMU

b ) Determine the total time for this work element in seconds

first we have to determine the total TMU = ∑ TMU = 86.4 TMU

note ; 1 TMU = 0.036 seconds

hence the total time for the work in seconds = 86.4 * 0.036 = 3.1 seconds

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mihalych1998 [28]

Answer:

2.279 bar

Explanation:

I will be using R = 8.314*10^{-2} \frac{l*bar}{K*mol} here.

Also, you should know that 1 l*bar = 0.1 kJ

Lastly, the definition of work for <em>any</em> thermodynamics process:

W=-\int P \, dV                                                           eq1        

So, getting started. We will first find the work for the first process

  • The first step, we have a constant volume process, therefore, there is no work done (W = 0) You can see it from this integral

-\int\limits^{V_2} _{V_1} {P} \, dV

There is no volume change, so no work can be done

  • In the second step We now have a constant pressure process. Don't worry, our eq1 still works here. Take in mind now that P is now a function of T. And since we are assuming that air is an ideal gas, we can use Ideal gas law PV = nRT here. So:

T = \frac{PV}{nR}

But there is no T in this integral!

W=-\int P \, dV

This is where we will do a little calculus trick.

In differential form:

dT=d\frac{PV}{R}

Note that P and R is constant So...

dT=\frac{P}{R}dV

Now we can substitute dV in the integral with dT

-\int\limits^{T_2} _{T_1} {\frac{PR}{P}} \, dT

And we get

W = -\int\limits^{T_2} _{T_1} {\frac{PR}{P}} \, dT

W = -3.741\ kJ

So, in total, the work <em>done</em><em> </em>by this process is 3.741 kJ. Make sure you do not confuse the sign of your answer. It is always good to state <em>prior</em> to your calculation which sign, + or - , will be assigned to work done <em>by </em>your system or work done <em>to</em> your system.

Now for the second process

  • We have an isothermal process, which means that T is constant during the process. So, similar to part 2 of the first process, by using ideal gas law:

P=\frac{RT}{V}

Which we will substitute into our ever reliable eq1

W=-\int\limits^{V_2} _{V_1} {\frac{RT}{V}} \, dV

Solving this integral, we get

W= -RT(ln(V_2)-ln(V_1))=-RTln(\frac{V_2}{V_1})                            eq2

Now, since we don't know V but we know P, We can simply use Ideal gas law(again)

V=\frac{RT}{P}

And substitute it in eq2, so:

W= -RTln(\frac{P_1}{P_2}=-RT(ln(P_1)-ln(P_2))

In kJ unit

W=-0.1*800*0.08314*(ln(4)-ln(P_2))

  • Finally, we find P_2 of process 2 that would make that work done by both process equal. So, we equate the work done by both process

W=-3.741 =-0.1*800*0.08314(ln(4)-ln(P_2))

Solve this equation for P_{2} and we get

P_{2}=2.279\ bar

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A ball of 0.900 kg slides horizontally over a frictionless surface and bumps into a heavy stone at a speed of 20.0 m / s. The ba
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Answer:

33.06 Kgm/s

Explanation:

Given information

Initial velocity= 20 m/s

mass, m=0.9 Kg

0.5\times 0.9\times v^{2}=0.5\times 0.7\times 0.9 Kg\times 20^{2}

v^{2}=280

v=\sqrt {280}=16.7332 m/s

Here, v is -16.7332 m/s in opposite direction

Change in momentum

\triangle p= m(v-u)=0.9(-16.7332-20)=-33.0599 Kgm/s\approx -33.06 Kgm/s

Therefore, the magnitude of change in momentum is 33.06 Kgm/s

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Answer:

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Explanation:

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Answer:

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ηth = 1 - (300/Tc)

We can assume a value for TH to be 400°C

Then,

ηth = 1 - (300/400) = 1 - 0.75 = 0.25

Explanation:

Thermal efficiency, ηth, of an heat engine is define as the ratio of the work it does, W, to the heat input at the high temperature, QH.

The thermal efficiency is expressed mathematically as:

ηth= QH/W

OR

Thermal efficiency(ηth) = 1 - (TH/Tc).

In other words, the fraction of heat that is converted to work is the thermal efficiency. That is, the measure of performance of engines that uses heat energy in their operation. It has no dimension.

Examples of such engines are:

Steam turbine;

Any internal combustion engine;

A refrigerator.

In operation of a refrigeration or heat pumps, thermal efficiency indicates the extent to which the energy added by work is converted to net heat output. Since it is dimensionless number, we must always express W, QH, and QC in the same units

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