E'=phi

The specific heat at constant pressure and at constant volume for an ideal gas are C_(p) and C_(v) and its adiabatic and isothermal eleasticities are E_(phi) and E_(theta) respectively. The ratio of E_(phi) to E_(theta) is

If E_(1),E_(2), are two events with E_(1)nn E_(2)=phi then P(bar(E)_(1)nnbar(E)_(2))=

If and phi(x)=(1)/(1+e^(-x))S=phi(5)+phi(4)+phi(3)+...+phi(-3)+phi(-4)+phi(-5) then the value of S is

If phi(x)=1/(1+e^(-x)) S=phi(5) +phi(4) +phi(3) + ..+phi(-3) + phi (-4) + phi(-5) then the value of S is

if int (e^(6logx) - e^(4logx))/(e^(3logx)-e^(2logx)) dx = phi(x), then phi'(1) is

Let inte^(x){f(x)-f'(x)}dx=phi(x) . Then inte^(x)*f(x)dx is a) phi(x)+e^(x)f(x) b) phi(x)-e^(x)f(x) c) 1/2{phi(x)+e^(x)f(x)} d) 1/2{phi(x)+e^(x)f'(x)}

Fig. shows a surface XY separating two transparent media, medium 1 and medium 2. Lines ab and cd represent wavefronts of a light wave travelling in medium 1 and incident on XY. Line ef and gh represent wavefront of the light wave in medium 2 after rafraciton. The phase of the ligth wave at c, d, e, and f are phi_(c) , phi_(d), phi_(e) and phi_(f) , respectively. It is given that phi_(c ) != phi_(f) . Then

Fig. shows a surface XY separating two transparent media, medium 1 and medium 2. Lines ab and cd represent wavefronts of a light wave travelling in medium 1 and incident on XY. Line ef and gh represent wavefront of the light wave in medium 2 after rafraciton. The phase of the ligth wave at c, d, e, and f are phi_(c) , phi_(d), phi_(e) and phi_(f) , respectively. It is given that phi_(c ) != phi_(f) . Then

If E_1 and E_2=phi are any two events associated with an experiment and lambdaP(E_1capE_2)=P(E_1//E_2) , then write down the value of lambda .