Key Definition: The pressure exerted by the vapour in equilibrium with its liquid phase at a particular temperature is called its vapour pressure.
Important Note (JEE Focus): The surface area of the liquid *does not* affect the equilibrium vapour pressure. It affects the *rate* at which equilibrium is reached (a larger surface area means faster evaporation), but once equilibrium is established, the pressure exerted by the vapour remains the same for a given liquid at a given temperature.
Analogy: Think of it like a molecular tug-of-war. A molecule in the middle is pulled equally by teams in all directions. A molecule on the surface has teams pulling it from below and sides, but almost no team pulling it upwards. So, it gets pulled inwards!
Key Definition: Surface tension is the force acting per unit length perpendicular to the line drawn on the surface of a liquid, or it can be defined as the energy required to increase the surface area of a liquid by a unit amount. It is typically denoted by the Greek letter gamma ($gamma$).
CBSE vs. JEE Focus: For both CBSE and JEE, a strong qualitative understanding of how IMFs and temperature affect both vapour pressure and surface tension is crucial. JEE might present more complex comparative problems (e.g., comparing VP/ST of different liquids or the effect of various solutes), while CBSE focuses more on defining and explaining the phenomena with simple examples.
The pressure exerted by the vapour molecules in equilibrium with the liquid at a given temperature is called the Vapour Pressure of the liquid.
| Factor | Effect on Vapour Pressure | Reason |
|---|---|---|
| Strength of IMFs | Weaker IMFs → Higher Vapour Pressure | Molecules escape more easily. |
| Temperature | Higher Temperature → Higher Vapour Pressure | More molecules have sufficient kinetic energy to escape. |
A liquid boils when its vapour pressure becomes equal to the external atmospheric pressure.
Due to this net inward pull, surface molecules are at a higher potential energy compared to molecules in the bulk. To minimize this higher energy, liquids tend to reduce their surface area as much as possible.
As the force per unit length acting perpendicular to a line drawn on the surface of the liquid, tending to pull the surface inwards.
As the surface energy per unit area. It is the amount of work required to increase the surface area of a liquid by one unit against the net inward pull.
| Factor | Effect on Surface Tension | Reason |
|---|---|---|
| Strength of IMFs | Stronger IMFs → Higher Surface Tension | Greater net inward pull on surface molecules. |
| Temperature | Higher Temperature → Lower Surface Tension | Increased kinetic energy weakens IMFs. |
| Surfactants | Presence of Surfactants → Lower Surface Tension | Disrupt IMFs at the surface. |
Acing the 'Liquid State' concepts like Vapour Pressure and Surface Tension often hinges on remembering the key definitions and, more importantly, how different factors influence them. Here are some mnemonics and short-cuts to help you commit these qualitative relationships to memory for your JEE and board exams.
Vapour pressure is the pressure exerted by the vapour in equilibrium with its liquid phase at a given temperature. Think of it as the liquid's 'desire' to escape into the gas phase.
The two main factors are Temperature (T) and Intermolecular Forces (IMF).
Surface tension is the force per unit length acting perpendicular to the surface of a liquid, causing the surface to behave like a stretched elastic membrane. It arises from the unbalanced attractive forces on surface molecules pulling them inwards.
The main factors are Intermolecular Forces (IMF), Temperature (T), and impurities.
| Factor | Effect on Vapour Pressure (VP) | Effect on Surface Tension (ST) |
|---|---|---|
| Temperature ($uparrow$) | VP $uparrow$ (Mnemonic: "Vapor Up, Temperature's Cup") | ST $downarrow$ (Mnemonic: "Surface Weak, Temperature's Peak") |
| Intermolecular Forces (IMF $uparrow$) | VP $downarrow$ (Mnemonic: "Vapor Down, IMF's Crown") | ST $uparrow$ (Mnemonic: "Surface Strong, IMF's Song") |
| Impurities/Surfactants | (Generally negligible/depends) | ST $downarrow$ (Mnemonic: "Soap drops ST") |
JEE Tip: Remember the inverse relationship between VP and BP. Questions often test this indirectly. Also, the effect of temperature is opposite for VP and ST, which is a common point of confusion β use the mnemonics!
Mastering these fundamental relationships qualitatively is key for both objective (JEE) and descriptive (CBSE) questions. Keep practicing!
Keep these qualitative relationships clear in your mind for quick problem-solving!
Understanding the properties of liquids like vapour pressure and surface tension is crucial for comprehending their behaviour. These are not just theoretical concepts but observable phenomena that dictate how liquids interact with their surroundings and themselves.
Imagine a liquid in an open container. You've seen it evaporate, right? This happens because molecules at the surface, with enough kinetic energy, can overcome the attractive forces from their neighbours and escape into the gas phase. This process is called evaporation.
Now, consider the same liquid in a closed container:
Intuitive understanding: Think of it like a crowded dance floor (liquid). Some dancers are always leaving the floor (evaporation). If the room is enclosed, those who leave eventually hit a wall and might decide to rejoin the dance (condensation). Vapour pressure is the "push" exerted by the dancers who have left the floor but are still in the room, once the number leaving equals the number rejoining.
Qualitative Factors Affecting Vapour Pressure:
Have you ever seen an insect walk on water, or observed how water forms spherical droplets on a waxy surface? These phenomena are due to Surface Tension.
At the molecular level, molecules within the bulk of a liquid are surrounded by other molecules and experience attractive forces from all directions, resulting in a net force of zero. However, molecules at the liquid's surface are different:
Intuitive understanding: Imagine pulling a blanket taut across a bed. The blanket resists stretching and tries to minimize its area. Similarly, a liquid's surface behaves like this stretched membrane, resisting any increase in its surface area. This resistance is surface tension.
Qualitative Factors Affecting Surface Tension:
For both CBSE and JEE Main, a clear qualitative understanding of these phenomena, the factors affecting them, and common examples is crucial. Numerical problems are less common for surface tension at this level, but understanding the trends and underlying principles is essential.
Understanding Vapour Pressure and Surface Tension isn't just for textbooks; these fundamental properties of liquids govern many phenomena we encounter daily and are crucial in various industries. Let's explore some real-world applications.
Understanding these properties qualitatively is crucial not just for exams (JEE Main & CBSE) but also to appreciate the chemistry at play in our everyday lives and various industrial processes.
Understanding abstract concepts like vapour pressure and surface tension can be greatly simplified through relatable analogies. These analogies help in visualizing the microscopic world and the forces at play.
Imagine a closed concert hall or a large room (representing a closed container) where:
Here's how the analogy works:
Consider a large, tightly stretched trampoline (representing a liquid) to understand surface tension:
Here's how the analogy unfolds:
These analogies provide a qualitative understanding of these phenomena, crucial for both board exams and competitive tests like JEE Main.
To effectively understand the qualitative aspects of vapour pressure and surface tension, a solid grasp of certain fundamental concepts is essential. These foundational ideas will enable you to appreciate the underlying molecular behavior driving these phenomena.
Tip for JEE: While the topic is qualitative, a strong conceptual base in these prerequisites will allow you to quickly analyze and answer application-based questions, especially those involving comparisons between different liquids.
Navigating the concepts of vapour pressure and surface tension requires a sharp eye, as exams often feature subtle traps designed to test your conceptual clarity. Be aware of these common pitfalls to maximize your scores.
JEE Main & CBSE Tip: For both exams, qualitative understanding of these properties and the factors affecting them is crucial. Focus on the 'why' behind the trends rather than complex calculations.
By understanding these common traps, you can approach questions on vapour pressure and surface tension with greater confidence and accuracy. Keep practicing!
Question: Arrange the following liquids in increasing order of their vapour pressure at 25Β°C: Water (H2O), Ethanol (CH3CH2OH), Diethyl Ether (CH3CH2OCH2CH3).
Approach:
Answer: Water < Ethanol < Diethyl Ether (increasing vapour pressure).
Mastering these qualitative relationships will enable you to confidently tackle conceptual questions on these topics. Focus on the underlying intermolecular forces and how they dictate physical properties.
The Liquid State, particularly concepts like vapour pressure and surface tension, forms a foundational part of the CBSE Chemistry syllabus. For board exams, the focus is primarily on qualitative understanding, definitions, factors affecting these properties, and their everyday applications, rather than complex derivations or numerical problems. Mastering these basic concepts is crucial for scoring well in this section.
For CBSE, a clear understanding of what vapour pressure is and what influences it is key.
CBSE questions on surface tension typically involve its definition, the molecular basis, factors affecting it, and real-world examples.
For CBSE, ensure you can define these terms accurately and explain the 'why' behind the qualitative observations and phenomena related to them. Focus on the relationship between intermolecular forces, temperature, and these properties.
Understanding Vapour Pressure and Surface Tension qualitatively is crucial for JEE Main, as questions often test your conceptual clarity regarding intermolecular forces and their impact on physical properties.
| Concept | Typical JEE Question |
|---|---|
| Vapour Pressure | Which of the following liquids will have the highest vapour pressure at 25Β°C: (A) H2O (B) C2H5OH (C) (CH3)2CO (D) CCl4? (Requires understanding IMF) |
| Surface Tension | Explain why water drops are spherical but fall flat on a very hot surface. (Involves surface tension vs. temperature) |
| Both | Compare the boiling points and surface tensions of glycerol and ethanol. Justify your answer. (Links IMF to both properties) |
| Applications | Why do detergents enhance the cleaning action of water? (Relates to reduction of surface tension) |
Mastering these qualitative aspects will help you tackle conceptual questions efficiently in JEE Main.
No CBSE problems available yet.
No JEE problems available yet.
No videos available yet.
No images available yet.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
Consider Liquid X at 320 K confined in a closed space:
| Condition | Time to Reach Equilibrium | Final Vapour Pressure (P) |
|---|---|---|
| Small Surface Area (5 cmΒ²) | Longer | P (e.g., 50 torr) |
| Large Surface Area (50 cmΒ²) | Shorter | P (50 torr) |
The final VP is the same; only the time taken differs.
No summary available yet.
No educational resource available yet.