A flask is filled with mercury at temperature `28^(@)C` . If the flask and the contents are heated to `48^(@)C` , the volume of mercury above the mark will be `(alpha_(glass=9xx10^(-6)//^(@)C` , `gamma_(Hg)=180xx10^(-6)//^(@)C)`

A one litre flask contains some mercury. It is found that at different temperatures the volume of air inside the flask remains the same. The volume of mercury in the flask is (alpha_(glass)=9xx10^(-6)//^(@)C,gamma_(Hg)=180xx10^(-6)//^(@)C)

A galss flask is filled up to a mark with 50 cc of mercury at 18^@C . If the flask and contents are heated to 38^@C , how mech mercury will be above the mark ( alpha for glass is 9xx10^(-6)//^@C and coeffiecient of real expansion of mercury is 180xx10^(-6)//^@C )?

A glass flask is filled up to a mark with 50 cc of mercury at 18^@C . If the flask and contents are heated to 38^@C , how much mercury will be above the mark ( alpha for glass is 9xx10^(-6)//^@C and coeffiecient of real expansion of mercury is 180xx10^(-6)//^@C )?

A two litre glass flask contains some mercury. It is found that at all temperatures the volume of the air inside the flask remains the same. The volume of the mercury inside the flask is ( alpha for glass =9xx10^-6//^@C,gamma for mercury 1.8xx10^-4//^@C)

A two litre glass flask contains some mercury. It is found that at all temperatures the volume of the air inside the flow remains the same. The volume of the mercury inside the flask is (alpha for glass = 9 xx 10^-6/^@C, gamma for mercury 1.8 xx 10^-4/^@C)

The fraction of the volume of a glass flask must be filled with mercury so that the volume of the empty space may be the same at all temperature is (alpha_("glass") = 9 xx 10^(-6)//^(0)C, gamma_(Hg) = 18.9 xx 10^(-5) // ^(0)C)