00:01
Hello everyone, let us consider s is equals to f of t, v and then ds becomes, differentiation of this becomes del f upon del t of v dt plus ds upon dv of tv for t is a equation number one.
00:27
For system involving tv work then ds is equals to 1 upon t du plus v upon t dv is a equation number two.
00:41
Then u is equals to f of t, v then del u is equals to, du is equals to del of u del t for v dt plus del u or del divided by del v for t dv.
01:09
Therefore ds is equals to 1 upon t, del u becomes, du becomes del u upon del t of v dt plus 1 upon t, t plus del u upon del v for t dv.
01:40
This is the equation number three.
01:42
Therefore, this equation will becomes and cvm of t dt plus 1 upon t, t plus del u upon del v t dv is hence, the equation will becomes del u upon del v for t is equals to t del p upon del t for v minus p that is by thermodynamic equation of state ds is equals to n c, m divided by t dt plus del p upon del t v dv.
03:06
Hence, it is equals to nr c, v divided by t dt plus del nr t divided by v divided by del t dv.
03:27
That is the ideal case p is equals to nr t divided by v.
03:35
Therefore, the equation will also becomes nr 1 upon cpm minus cvm divided by cv, m dt by t plus nr dv upon v because of ideal case we know that becomes cv, m equals to cv sorry minus cv, m equals to r...