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An ideal gas is initially at temperature...

An ideal gas is initially at temperature T and volume V . Its volume is increased by `DeltaV` due to an increase in temperature `Delta` , pressure remaining constant . The quantity `delta=DeltaV//VDeltaT` varies with temperature as

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To solve the problem step by step, we will analyze the relationship between volume, temperature, and the given quantities in an isobaric process (constant pressure). ### Step 1: Understand the Ideal Gas Law The ideal gas law is given by the equation: \[ PV = nRT \] Where: - \( P \) = pressure - \( V \) = volume - \( n \) = number of moles of gas - \( R \) = universal gas constant - \( T \) = temperature Since the pressure is constant in this scenario, we can express the relationship between volume and temperature. ### Step 2: Express Volume in Terms of Temperature From the ideal gas law, if \( P \) is constant, we can write: \[ V \propto T \] This means that volume \( V \) is directly proportional to temperature \( T \). We can express this as: \[ V = kT \] Where \( k \) is a constant. ### Step 3: Differentiate the Volume Equation Now, we differentiate both sides of the equation \( V = kT \): \[ dV = k \, dT \] This equation shows how a small change in volume relates to a small change in temperature. ### Step 4: Relate Changes in Volume and Temperature Next, we can write the ratio of changes: \[ \frac{dV}{V} = \frac{k \, dT}{kT} \] This simplifies to: \[ \frac{dV}{V} = \frac{dT}{T} \] ### Step 5: Convert to Finite Changes Since the problem mentions finite changes (denoted by \( \Delta \)), we can replace \( d \) with \( \Delta \): \[ \frac{\Delta V}{V} = \frac{\Delta T}{T} \] ### Step 6: Rearranging the Equation We can rearrange the equation to express the relationship between \( \Delta V \), \( V \), \( \Delta T \), and \( T \): \[ \Delta V \cdot \Delta T = \frac{V}{T} \] ### Step 7: Define the Quantity \( \delta \) The problem defines \( \delta \) as: \[ \delta = \frac{\Delta V}{V \Delta T} \] Substituting from our previous result: \[ \delta = \frac{1}{T} \] ### Step 8: Analyze the Relationship From the equation \( \delta = \frac{1}{T} \), we can see that \( \delta \) is inversely proportional to the temperature \( T \). ### Conclusion Thus, the quantity \( \delta \) varies inversely with temperature \( T \). If we were to graph this relationship, it would show a hyperbolic decline, indicating that as temperature increases, \( \delta \) decreases.
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