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photoshop1234 [79]
3 years ago
8

Cos square there + cos square theta multiply cot square theta = cot square theta​

Engineering
1 answer:
Ivahew [28]3 years ago
8 0

Explanation:

We need to prove that : \cos^2\theta+\cos^2\theta {\cdot} \cot^2\theta=\cot^2\theta

Taking LHS : \cos^2\theta+\cos^2\theta {\cdot} \cot^2\theta

Taking \cos^2\theta common as follows :

\cos^2\theta(1+ \cot^2\theta) ...(1)

We know that :

cosec^2\theta-\cot^2\theta=1\\\\cosec^2\theta=1+\cos^2\theta ....(2)

Use equation (2) in equation (1) as follows :

\cos^2\theta{\cdot} cosec^2\theta

We know that : cosec\theta=\dfrac{1}{\sin\theta}

So,

\cos^2\theta{\cdot} \dfrac{1}{\sin^2\theta}\\\\=\cot^2\theta

=RHS

Hence, LHS = RHS

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Answer:

a) The operation of a heat pump involves the extraction of energy in the form of heat Q₁ from a cold source

b) The modifications required to convert a plant operating on an ideal Carnot cycle to a plant operating on a Rankine cycle involves

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ii) Heating of the pumped, pressurized water to the boiler pressure

Explanation:

a) 1 - 2. Wet vapor enters compressor where it undergoes isentropic compression to state 2 by work W₁₂  

2 - 3. The vapor enters the condenser at state 2 where it undergoes isobaric and isothermal condensation to a liquid with the evolution of heat  Q₂

3 - 4. The condensed liquid is expanded isentropically with the work done equal to W₃₋₄

4 - 1. At the state 4, with reduced pressure from the previous expansion, the liquid makes its way to the evaporator where it absorbs heat, Q₁, from the body to be cooled.

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ii) Heating of the pumped, pressurized water to the boiler pressure

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3 years ago
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