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Kobotan [32]
3 years ago
10

1 point

Physics
1 answer:
Darya [45]3 years ago
7 0

Given that,

Mass of object, m = 55 kg

Mechanical energy of the object, M = 4306 J    

Potential energy, P = 2940 J

We know that the mechanical energy is the sum of kinetic and potential energy such that,

Mechanical energy = kinetic energy + potential energy

K=M-P\\\\K=4306-2940\\\\K=1366\ J

Kinetic energy is given by :

K=\dfrac{1}{2}mv^2v is velocity of object

v=\sqrt{\dfrac{2K}{m}} \\\\v=\sqrt{\dfrac{2\times 1366}{55}} \\\\v=7.04\ m/s

So, the velocity of object is 7.04 m/s.            

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The x vector component of a displacement vector has a magnitude of 86.2 m and points along the negative x axis. The y vector com
Flauer [41]

Answer:

(a) Magnitude of Vector = 207.73 m

(b) Direction = 65.48°

Explanation:

(a)

The formula to find out the magnitude of a resultant vector with the help of its x and y components is given as follows:

Magnitude\ of\ Vector = \sqrt{d_{x}^{2} + d_{y}^{2}} = \sqrt{(86.2\ m)^{2} + (189\ m)^{2}}\\\\

<u>Magnitude of Vector = 207.73 m</u>

(b)

For the direction of the vector we have the formula:

Direction = tan^{-1}(\frac{y}{x})\\\\Direction = tan^{-1}(\frac{189\ m}{86.2\ m})\\\\

<u>Direction = 65.48°</u>

4 0
3 years ago
An ideal Otto cycle has a compression ratio of 8. At the beginning of the compression process, air is at 95 kPa and 27°C, and 75
katen-ka-za [31]

Answer:

Part A) 3899 kPa  

Part B) 392.33 kJ/kg  

Part C) 0.523

Part D) 495 kPa

Explanation:

Part A

First from the temperature at state 1 the relative specific volume and the internal energy at that state are determined from:

u_{1} = 214.07 kJ/kg  

\alphar_{1} = 621.2  

The relative specific volume at state 2 is obtained from the compression ratio:  

\alphar_{2} = \frac{\alpha r_{1}  }{r}

     =621.2/ 8

    = 77.65  

From this the temperature and internal energy at state 2 can be determined using interpolation with data from A-17(table):  

T_{2} = 673 K

u_{2} = 491.2 kJ/kg  

The pressure at state 2 can be determined by manipulating the ideal gas relations at state 1 and 2:  

P_{2} =  P_{1} r\frac{T_{2} }{T_{1} }

       = 95*8*673/300

      = 1705 kPa  

Now from the energy balance for stage 2-3 the internal energy at state 3 can be obtained:  

deltau_{2-3} =q_{in}\\ u_{3} -u_{2} =q_{in}\\u_{3}=u_{2}+q_{in}

     = 1241.2 kJ/kg

From this the temperature and relative specific volume at state 3 can be determined by interpolation with data from A-17(table):  

T_{3} = 1539 K  

\alpha r_{3} = 6.588  

The pressure at state 3 can be obtained by manipulating the ideal gas relations for state 2 and 3:  

P_{3} =P_{2} \frac{T_{3} }{T_{2} }

     = 3899 kPa  

<u>Part B</u>

The relative specific volume at state 4 is obtained from the compression ratio:  

\alpha r_{4}= r\alpha r_{3}

      = 52.7

From this the temperature and internal energy at state 4 can be determined by interpolation with data from A-17:  

T_{4}=775 K

u_{4}= 571.74 kJ/kg  

The net work output is the difference of the heat input and heat rejection where the heat rejection is determined from the decrease in internal energy in stage 4-1:  

w=q_{in}-q_{out}\\q_{in}-(u_{4} -u_{1} )\\=392.33 kJ/kg

<u>Part C  </u>

The thermal efficiency is obtained from the work and the heat input:  

η=\frac{w}{q_{in} }

=0.523

<u>Part D  </u>

The mean effective pressure is determined from its standard relation:  

MEP=\frac{w}{\alpha_{1}- \alpha_{2} }

      =\frac{w}{\alpha_{1}(1- \frac{1}{r}  }

      =\frac{rwP_{1} }{RT_{1} (r-1) }

      =495 kPa

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