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An ideal gas at \(7^{\circ} \mathrm{C}\) is in a spherical flexible container having a radius of \(1.00 \mathrm{~cm}\). The gas is heated at constant pressure to \(88^{\circ} \mathrm{C}\). Determine the radius of the spherical container after the gas is heated. [Volume of a sphere \(\left.=(4 / 3) \pi r^{3} .\right]\)

Short Answer

Expert verified
The radius of the spherical container after the gas is heated is approximately \(1.23 cm\).

Step by step solution

01

Write down the Ideal Gas Law equation

The Ideal Gas Law equation is given by \(PV = nRT\), where P is the pressure, V is the volume, n is the number of moles, R is the universal gas constant, and T is the temperature in Kelvin.
02

Convert the temperatures to Kelvin

We need to convert the given temperatures from degrees Celsius to Kelvin. The formula for the conversion is \(T(K) = T(°C) + 273.15\). Initial temperature, \(T_1 = 7°C + 273.15 = 280.15 K\) Final temperature, \(T_2 = 88°C + 273.15 = 361.15 K\)
03

Calculate the initial volume

The volume of a sphere is given by the formula: \(V = \frac{4}{3} \pi r^3\). Using the initial radius, \(r_1 = 1.00 cm\), we can calculate the initial volume, \(V_1\). \(V_1 = \frac{4}{3} \pi (1.00)^3 = \frac{4}{3} \pi cm^3\)
04

Use the constant pressure property

Since the pressure remains constant during the heating process, we can write the Ideal Gas Law equation for both initial and final states as follows: \(\frac{V_1}{T_1} = \frac{V_2}{T_2}\)
05

Solve for the final volume

Substituting the values of \(V_1, T_1\), and \(T_2\) into the above equation, we can solve for the final volume, \(V_2\): \(\frac{\frac{4}{3} \pi cm^3}{280.15 K} = \frac{V_2}{361.15 K}\) After rearranging the equation, we find that: \(V_2 = \frac{4}{3} \pi cm^3 \times \frac{361.15}{280.15} \approx 1.89 \pi cm^3\)
06

Find the new radius of the container

We can find the final radius \(r_2\) using the formula for the volume of a sphere. Setting \(V_2 = 1.89 \pi cm^3\), we can solve for \(r_2\): \(\frac{4}{3} \pi r_2^3 = 1.89 \pi cm^3\) Dividing both sides by \(\frac{4}{3} \pi\), we get: \(r_2^3 = 1.89 cm^3\) Take the cube root of both sides: \(r_2 \approx 1.23 cm\) The radius of the spherical container after the gas is heated is approximately 1.23 cm.

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Most popular questions from this chapter

One of the chemical controversies of the nineteenth century concerned the element beryllium (Be). Berzelius originally claimed that beryllium was a trivalent element (forming \(\mathrm{Be}^{3+}\) ions) and that it gave an oxide with the formula \(\mathrm{Be}_{2} \mathrm{O}_{3} .\) This resulted in a calculated atomic mass of \(13.5\) for beryllium. In formulating his periodic table, Mendeleev proposed that beryllium was divalent (forming \(\mathrm{Be}^{2+}\) ions) and that it gave an oxide with the formula BeO. This assumption gives an atomic mass of \(9.0 .\) In 1894 , A. Combes (Comptes Rendus 1894, p. 1221\()\) reacted beryllium with the anion \(\mathrm{C}_{5} \mathrm{H}_{7} \mathrm{O}_{2}^{-}\) and measured the density of the gaseous product. Combes's data for two different experiments are as follows: If beryllium is a divalent metal, the molecular formula of the product will be \(\mathrm{Be}\left(\mathrm{C}_{3} \mathrm{H}_{7} \mathrm{O}_{2}\right)_{2} ;\) if it is trivalent, the formula will be \(\mathrm{Be}\left(\mathrm{C}_{5} \mathrm{H}_{7} \mathrm{O}_{2}\right)_{3}\). Show how Combes's data help to confirm that beryllium is a divalent metal.

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