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Question: If a vessel of thermal capacity \( 30 \) calories contains \( 170g \) of water at \( 30^\circ C \) ....

If a vessel of thermal capacity 3030 calories contains 170g170g of water at 30C30^\circ C . If on dropping a solid at 93C93^\circ C into the calorimeter, then the temperature of mixture becomes 33C33^\circ C , find the thermal capacity of the solid.

Explanation

Solution

Hint : In a calorimeter, the object is dropped into water, on doing so it transfers the heat energy present in it to the water, this causes the overall temperature of the water to rise, thus the heat lost by the hot object is equal to heat gained by the cold object. Here the dropped solid is the hot object while water is the cold object.

Formula used:
η×m=ω\Rightarrow \eta \times m = \omega
Where η\eta is the specific heat capacity of a substance, ω\omega is the heat capacity of the body, mm is the mass of the body.

Complete step by step answer
When the solid is dropped into water, all of its heat is transferred to water if it is assumed that heat does not dissipate into the surroundings.
Therefore it can be written as,
Heat lost by the solid = Heat gained by the water
It is given that initial temperature of the hot body Ti=93{T_i} = 93
Final temperature of the hot body Tf=33{T_f} = 33
Let the change in temperature of the hot body be ΔT\Delta T . Then,
ΔT=TfTi\Rightarrow \Delta T = {T_f} - {T_i} of the solid.
ΔTs=3393=60\Rightarrow \Delta {T_s} = 33 - 93 = 60
Let the thermal capacity of the solid be ωs{\omega _s}
Then the heat lost by the solid HL{H_L} is given by-
Q=ωsΔTs\Rightarrow Q = {\omega _s}\Delta {T_s}
Q=ωs×60\Rightarrow Q = {\omega _s} \times 60
For the water and the vessel (or the cold body),
The initial temperature Ti=30{T_i} = 30
The final temperature Tf=33{T_f} = 33
The change in temperature of the water in the vessel is,
ΔT=TfTi\Rightarrow \Delta T = {T_f} - {T_i} of the water.
ΔTw=3330=3\Rightarrow \Delta {T_w} = 33 - 30 = 3
The heat gained by the system of water and the vessel can be calculated by adding the individual heat gains of the water and the vessel.
For the vessel, heat gained is,
Qv=ωvΔTw\Rightarrow {Q_v} = {\omega _v}\Delta {T_w}
Where, ωv{\omega _v} is the heat capacity of the vessel equal to 30cal30cal .
And heat gained by the water is,
Qw=ηw×mw×ΔT\Rightarrow {Q_w} = {\eta _w} \times {m_w} \times \Delta T
ηw{\eta _w} is the specific heat capacity of the water which is equal to 1cal/gC1cal/g^\circ C .
mw{m_w} is the mass of water, which is given as 170g170g
Therefore,
The heat gained by water and vessel is given by-
Qv+Qw=ΔTw(ωv+mwηw)\Rightarrow {Q_v} + {Q_w} = \Delta {T_w}({\omega _v} + {m_w}{\eta _w})
On putting the values,
Qv+Qw=3(30+170×1)\Rightarrow {Q_v} + {Q_w} = 3(30 + 170 \times 1)
Qv+Qw=600\Rightarrow {Q_v} + {Q_w} = 600
Since this is equal to the heat lost by the solid,
Qv+Qw=Qs\Rightarrow {Q_v} + {Q_w} = {Q_s}
600=60ωs\Rightarrow 600 = 60{\omega _s}
ωs=10\therefore {\omega _s} = 10
The thermal capacity of the solid is 10cal/C10cal/^\circ C .

Note
The terms thermal capacity and heat capacity have the same meaning. But the terms heat capacity and specific heat capacity are different. Heat capacity is the heat required to raise the temperature of a body by 1C1^\circ C , while the specific heat capacity is the heat required to raise the temperature of 11 gram of a body by 1C1^\circ C .