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Question: A large weather balloon whose mass is \(226{\text{kg}}\) filled with helium gas until its volume is ...

A large weather balloon whose mass is 226kg226{\text{kg}} filled with helium gas until its volume is 325m3325{{\text{m}}^3}. Assume the density of air is 1.2kgm31.2{\text{kg}}{{\text{m}}^{ - 3}} and the density of helium is 0.179kgm30.179{\text{kg}}{{\text{m}}^{ - 3}}. What additional mass can the balloon support in equilibrium?

Explanation

Solution

To solve such problems we need to draw a free body diagram to know all the components of force acting on the body so that we do not miss out any and as we have to find the additional mass in equilibrium, therefore, we need to balance all the force acting on it.

Complete step by step solution:
The given values in the question are
Mass =226kg = 226{\text{kg}}, let this be Mb{M_b}
Volume =325m3 = 325{{\text{m}}^3}, let this be VV
The density of air =1.2kgm3 = 1.2{\text{kg}}{{\text{m}}^{ - 3}} , let this be ρair{\rho _{air}}
The density of helium =0.179kgm3 = 0.179{\text{kg}}{{\text{m}}^{ - 3}} , let this be ρh{\rho _h}
And gg be the acceleration due to gravity
Now let us draw the free body diagram of the balloon and denote the force acting on it

Where, FB{F_B} is Buoyant force, Wh{W_h} is the weight of helium, Wb{W_b} is the weight of the balloon and Fg{F_g} is the gravitational force.
So the total force along the Y-axis (ΣFy)(\Sigma {F_y}) will be zero as the system is in equilibrium.
ΣFy=FBWhWbFg=0\Rightarrow \Sigma {F_y} = {F_B} - {W_h} - {W_b} - {F_g} = 0
ΣFy=ΣFNFg=0\Rightarrow \Sigma {F_y} = \Sigma {F_N} - {F_g} = 0
Where, ΣFN\Sigma {F_N} is the net force which will be,
ΣFN=FBWhWb(1)\Rightarrow \Sigma {F_N} = {F_B} - {W_h} - {W_b} - - - - (1)
Now we know, FB=ρa×V×g{F_B} = {\rho _a} \times V \times g
Substituting the values we get,
FB=1.2×325×9.8\Rightarrow {F_B} = 1.2 \times 325 \times 9.8
FB=3822N(2)\Rightarrow {F_B} = 3822{\text{N}} - - - (2)
And Wh=ρh×V×g{W_h} = {\rho _h} \times V \times g
Substituting the values we get,
Wh=0.179×325×9.8\Rightarrow {W_h} = 0.179 \times 325 \times 9.8
Wh=570N(3)\Rightarrow {W_h} = 570{\text{N}} - - - (3)
And Wb=Mb×g{W_b} = {M_b} \times g
Substituting the values we get,
Wb=226×9.8\Rightarrow {W_b} = 226 \times 9.8
Wb=2214.8N(4)\Rightarrow {W_b} = 2214.8{\text{N}} - - - (4)
Now putting the values from equations (2),(3) and (4) in (1), we get
ΣFN=38225702214.8\Rightarrow \Sigma {F_N} = 3822 - 570 - 2214.8
ΣFN=1.037×103N\Rightarrow \Sigma {F_N} = 1.037 \times {10^3}{\text{N}}
Therefore using the above value in the total force along with the Y-axis equation, we get
ΣFy=1037Fg=0\Rightarrow \Sigma {F_y} = 1037 - {F_g} = 0
Fg=1037\Rightarrow {F_g} = 1037
Now we know Fg=M×g{F_g} = M \times g
Where MM is the additional mass in equilibrium that we need to find out
M=1037g\Rightarrow M = \dfrac{{1037}}{g}
Substituting the value of acceleration due to gravity g=9.8m/s2g = 9.8 m/s^2 we get,
M=105kg\therefore M = 105{\text{kg}}
Therefore the mass 105.8kg105.8{\text{kg}} can be supported by the balloon in equilibrium.

Note: Buoyant force accounts for the air buoyancy created by the displaced air similar to the displacement of liquid in case of submerged body underwater and it acts downwards. Note the calculation of the weight of helium and the balloon which is equal to the mass multiplied by the acceleration due to gravity.