( a ) 2 ( b ) 4 ( c ) 8 ( d ) 16
A black body is
a theoretical object that absorbs all radiation that incident on its surface. As there is no reflection of light at room temperature the body is appears black ( that’s why it is called as black body ). Interestingly, when heated a ‘black body’ can radiate depending upon the temperature to which it is heated. This is known as ‘black body radiation’.
According to Stefan the power radiated from the blackbody can be determine by the formula
Where
P = Power radiated from the black body in W ( J / s )
σ = Stefan's Constant 5.67 x 10 - 8 W m - 2 K - 4 .
A = Surface area of black body ( m ² )
T = Temperature of body ( in Kelvin Scale [ K ] )
In other words we can say that the power radiated by the body is varies linearly with the forth power of its absolute temperature ( T 4 ) . Therefore the total energy increases so much for a relatively small increase in temperature.
Problem:
If the temperature of black body is increased by a factor of 2, the amount of energy and volume radiated increases by a factor of
Let us consider that the P1 be the power radiated from the black body in W ( J / s ) at initial temperature T1 ( K ). ‘ A ’ be the Surface area of black body and P2 be the power radiated from the black body in W ( J / s ) at final temperature T2 ( K ) .
At initial temperature T1 the Stefan’s law can be written as
Similarly at final temperature T2 the Stefan’s law can be written as
Taking ratio of above equations, we get
But,
Therefore,
Therefore we can say that if If the temperature of black body is increased by a factor of 2, the amount of energy and volume radiated increases by a factor of 16 (Answer : d)
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