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Question: Given, \[1g\] of water (volume \[1c{{m}^{3}}\]) becomes \[1671c{{m}^{3}}\] of steam when boiled at a...

Given, 1g1g of water (volume 1cm31c{{m}^{3}}) becomes 1671cm31671c{{m}^{3}} of steam when boiled at a pressure of 1atm1atm. The latent heat of vaporization is 540cal/g540cal/g, then the external work done is :
( 1atm=1.013×105N/m21atm=1.013\times {{10}^{5}}N/{{m}^{2}})
A. 499.9 J499.9\text{ }J
B. 40.3 J40.3\text{ }J
C. 169.2 J169.2\text{ }J
D. 128.57 J128.57\text{ }J

Explanation

Solution

We can solve this using the first law of thermodynamics. It states that the energy given to a system will be used to change the internal energy and work done. This work is found by change in volume.

Formula used: ΔU=ΔQΔW\Delta U=\Delta Q-\Delta W
ΔW=PΔV\Delta W=P\Delta V

Complete answer: In a thermodynamic system with volume change, The amount of external work done is given by the product of pressure and change in volume.
Now, we have the formula for work done as,
ΔW=PΔV\Delta W=P\Delta V
Here,ΔW\Delta Wis the work done,PP is pressure and ΔV\Delta V is change in volume
In the question the volume of water and steam is given. So the change in volume ΔV\Delta V can be found as,
ΔV=VSteamVWater\Delta V={{V}_{Steam}}-{{V}_{Water}}
Vsteam=1671cm3 Vwater=1cm3 \begin{aligned} & {{V}_{steam}}=1671c{{m}^{3}} \\\ & {{V}_{water}}=1c{{m}^{3}} \\\ \end{aligned}
ΔV=(16711)cm3=1670cm3=1670×106m3\Rightarrow \Delta V=(1671-1)c{{m}^{3}}=1670c{{m}^{3}}=1670\times {{10}^{-6}}{{m}^{3}} (here, cm3c{{m}^{3}}is converted tom3{{m}^{3}})
Now, to findΔW\Delta W, pressure is given as1atm=1.013×105N/m21atm=1.013\times {{10}^{5}}N/{{m}^{2}}
ΔW=PΔV ΔW=1.013×105ΔV \begin{aligned} & \Delta W=P\Delta V \\\ & \Rightarrow \Delta W=1.013\times {{10}^{5}}\Delta V \\\ \end{aligned}
ΔW=1.013×105×1670×106 ΔW=1.013×167 ΔW=169.17J169.2J \begin{aligned} & \Delta W=1.013\times {{10}^{5}}\times 1670\times {{10}^{-6}} \\\ & \Delta W=1.013\times 167 \\\ & \Delta W=169.17J\approx 169.2J \\\ \end{aligned}
The latent heat doesn’t take part in the external work done.it only take part in increase in internal energy which can be shown by,
ΔU=ΔQΔW\Delta U=\Delta Q-\Delta W
Here,ΔU\Delta U is a change in internal energy and ΔQ\Delta Q is given energy which could be found as mLmL where LL is latent heat.
ΔU=mLΔW\Rightarrow \Delta U=mL-\Delta W (1 kcal = 4180j1\text{ }kcal\text{ }=\text{ }4180j)
ΔU=1×540(169.2÷4.18) ΔU=54040.47 ΔU500cal \begin{aligned} & \Delta U=1\times 540-(169.2\div 4.18) \\\ & \Delta U=540-40.47 \\\ & \Delta U\approx 500cal \\\ \end{aligned}
Increase in internal energy is 500cal500cal.
So the correct answer is option c

Note: This question may seem a little bit confusing as they have given latent heat in question but asked only about external work done. So we must be aware that the constituents in the first law of thermodynamics must be able to distinguish between them.