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OLga [1]
3 years ago
10

Does an electronic clock use electrical energy?​

Engineering
2 answers:
kati45 [8]3 years ago
5 0
Yes it does because it's using the flow of energy from a conductor to power the clock :)
prohojiy [21]3 years ago
3 0

Answer:

Yes

Explanation:

It uses electrical energy because it is using the flow of energy from a conductor to power the clock.

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Consider a refrigerator that consumes 320 W of electric power when it is running. If the refrigerator runs only one quarter of t
Semenov [28]

Answer:

B. $5.18

Explanation:

Cost of electricity per kWh = $0.09

Power consumption of refrigerator = 320W = 320/1000 = 0.32kW

In a month (30 days) the refrigerator works 1/4 × 30 days = 7.5 days = 7.5 × 24 hours = 180 hours

Energy consumed in 180 hours = 0.32kW × 180h = 57.6kWh

Cost of electricity of 57.6kWh energy consumed by the refrigerator = 57.6 × $0.09 = $5.18

3 0
4 years ago
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Could a volcanic eruption suddenly bury a city and its inhabitants? (Plz explain to me)
andrezito [222]
Yes a volcanic eruption can suddenly bury a city ! if you look up some stuff on pompeii you can learn more
7 0
3 years ago
How much extra water does a 21.5 ft, 175-lb concrete canoe displace compared to an ultra-lightweight 38-lb Kevlar canoe of the s
pantera1 [17]

Answer:

The volume of the extra water is 2.195 ft^{3}

Solution:

As per the question:

Mass of the canoe, m_{c} = 175 lb + w

Height of the canoe, h = 21.5 ft

Mass of the kevlar canoe, m_{Kc} = 38 lb + w

Now, we know that, bouyant force equals the weight of the fluid displaced:

Now,

V\rho g = mg

V = \frac{m}{\rho}                                  (1)

where

V = volume

\rho = 62.41 lb/ft^{3} = density

m = mass

Now, for the canoe,

Using eqn (1):

V_{c} = \frac{m_{c} + w}{\rho}

V_{c} = \frac{175 + w}{62.41}

Similarly, for Kevlar canoe:

V_{Kc} = \frac{38 + w}{62.41}

Now, for the excess volume:

V = V_{c} - V_{Kc}

V = \frac{175 + w}{62.41} - \frac{38 + w}{62.41} = 2.195 ft^{3}

8 0
3 years ago
Refrigerant-134a enters an adiabatic compressor as saturated vapor at -24°C and leaves at 0.8 MPa and 60°C. The mass flow rate o
Leni [432]

Answer:

(a) The power input to the compressor: \dot{W}=73.07 kJ/s = 73.07 kW

(b) The volume flow rate of the refrigerant at the compressor inlet: \dot{v}=0.209 m^{3}/s

Explanation:

(a)

We need to check the values of enthalpy (as we have an open system) for both states, being the inlet, state 1 and the outlet, state 2. We will know these values by checking the vapor charts of R134a, I used the ones found in Thermodynamics of Cengel, 7th edition.

Then, our values are:

h_{1}=235.92kJ/kg\\h_{2}=296.81kJkg

Now we proceed to know the work with the following expression:

\dot{W}=\dot{m}(h_{2}-h_{1})

Now we replace values and our result is:

\dot{W}=73.07 kJ/s = 73.07 kW

(b)

To know the volume rate at the compressor inlet, we need to know the specific volume in that phase, as we have that is saturated and at -24°C, we can read our table:

\nu=0.1739m^{3}/kg

With our specific volume and the mass rate, we can calculate the volume rate:

\dot{v}=\nu * \dot{m}\\\dot{v}=0.209 m^{3}/s

6 0
3 years ago
Refrigerant R-12 is used in a Carnot refrigerator
Sphinxa [80]

Answer:

Heat transferred from  the refrigerated space = 95.93 kJ/kg

Work required = 18.45 kJ/kg

Coefficient  of performance = 3.61

Quality at the beginning of the heat  addition cycle = 0.37

Explanation:

From figure  

Q_H is heat rejection process

Q_L is heat transferred from the refrigerated space

T_H is high temperature = 50 °C + 273 = 323 K

T_L is low temperature = -20 °C + 273 = 253 K  

W_{net} is net work of the cycle (the difference between compressor's work and turbine's work)

 

Coefficient of performance of a Carnot refrigerator (COP_{ref}) is calculated as

COP_{ref} = \frac{T_L}{T_H - T_L}

COP_{ref} = \frac{253 K}{323 K - 253 K}

COP_{ref} = 3.61

From figure it can be seen that heat rejection is latent heat of vaporisation of R-12 at 50 °C. From table

Q_H = 122.5 kJ/kg

From coefficient of performance definition

COP_{ref} = \frac{Q_L}{Q_H - Q_L}

Q_H \times COP_{ref} = (COP_{ref} + 1) \times Q_L

Q_L = \frac{Q_H \times COP_{ref}}{(COP_{ref} + 1)}

Q_L = \frac{122.5 kJ/kg \times 3.61}{(3.61 + 1)}

Q_L = 95.93 kJ/kg

Energy balance gives

W_{net} = Q_H - Q_L

W_{net} = 122.5 kJ/kg - 95.93 kJ/kg

W_{net} = 26.57 kJ/kg

Vapor quality at the beginning of the heat addition cycle is calculated as (f and g refer to saturated liquid and saturated gas respectively)

x = \frac{s_1 - s_f}{s_g - s_f}

From figure

s_1 = s_4 = 1.165 kJ/(K kg)

Replacing with table values

x = \frac{1.165 kJ/(K \, kg) - 0.9305 kJ/(K \, kg)}{1.571 kJ/(K \, kg) - 0.9305 kJ/(K \, kg)}

x = 0.37

Quality can be computed by other properties, for example, specific enthalpy. Rearrenging quality equation we get

h_1 = h_f + x \times (h_g - h_f)

h_1 = 181.6 kJ/kg + 0.37 \times 162.1 kJ/kg

h_1 = 241.58 kJ/kg

By energy balance, W_{t} turbine's work is

W_{t} = |h_1 - h_4|

W_{t} = |241.58 kJ/kg - 249.7 kJ/kg|

W_{t} = 8.12 kJ/kg

Finally, W_{c} compressor's work is

W_{c} = W_{net} + W_{t}

W_{c} = 26.57 kJ/kg + 8.12 kJ/kg

W_{c} = 34.69 kJ/kg

6 0
3 years ago
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