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What is natural convection? How does it differ from forced convection? What force causes natural convection currents?

Short Answer

Expert verified
Natural convection is a process in which fluid motion or heat transfer occurs due to temperature differences within a fluid or between different fluids, without any external force applied. The main difference between natural convection and forced convection lies in the driving force behind fluid motion: In natural convection, buoyancy forces due to density variations caused by temperature differences are responsible, while in forced convection, an external force like a fan or pump drives the fluid motion. The buoyancy force, resulting from differences in fluid density caused by temperature variations, is the force responsible for natural convection currents.

Step by step solution

01

Define Natural Convection

Natural convection is a process where fluid motion or heat transfer occurs due to the temperature difference between different fluids or within a fluid, without any external force applied to cause the motion. In other words, natural convection occurs when the fluid motion is induced by buoyancy forces that result from density variations caused by temperature differences in the fluid.
02

Compare Natural and Forced Convection

The main difference between natural and forced convection is the driving force behind fluid motion or heat transfer. In natural convection, as described earlier, the driving force is the buoyancy force caused by temperature differences in the fluid, leading to density variations. On the other hand, forced convection occurs when an external force, such as a fan, pump, or an object moving through the fluid, drives the fluid motion or heat transfer. Additionally, forced convection usually provides a more uniform and efficient heat transfer compared to natural convection, which can be slower and less predictable due to the lack of control over fluid motion.
03

Identify the Force Causing Natural Convection Currents

The force that causes natural convection currents is the buoyancy force. The buoyancy force is a result of the differences in fluid density caused by temperature variations in the fluid. When a fluid is heated at the bottom, the warmer fluid becomes less dense and rises, while the colder and denser fluid sinks, creating a buoyancy-driven convection current. These natural convection currents are responsible for the fluid motion and heat transfer in natural convection.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Buoyancy Force
Buoyancy force is a fundamental concept of fluid dynamics and plays a crucial role in natural convection. In simple terms, buoyancy force is the upward force exerted on an object or fluid parcel when it is immersed in a fluid. This force is caused by the differences in density within the fluid. As the temperature of a fluid increases, its density usually decreases. This phenomenon makes the fluid lighter, and as a result, it experiences an upward buoyancy force. This is why warm air rises and cold air sinks, creating a natural flow pattern.

In the context of natural convection, the buoyancy force is the driving mechanism. It generates the movement needed for heat transfer without the need for external mechanical devices like fans or pumps. Let's consider a pot of boiling water on a stove. The water at the bottom, in contact with the heat source, warms up, becomes less dense, and rises. This movement creates a circulation loop within the pot due to the continuous action of buoyancy forces as colder, denser fluid from above sinks to replace the rising warm fluid.
Heat Transfer
Heat transfer in natural convection involves the conveyance of thermal energy from regions of higher temperature to regions of lower temperature. This process occurs naturally due to temperature differences within a fluid, leading to density variations and the movement of fluid as described in natural convection.

There are three key mechanisms of heat transfer: conduction, convection, and radiation. Convection, the key mechanism in the context of the current discussion, can be natural or forced. Natural convection relies on the buoyancy forces discussed earlier to create the movement of fluid without any mechanical intervention.
  • Conduction: Transfer of heat through a substance due to temperature gradient, like in solids or still fluids.
  • Radiation: Transfer of energy through electromagnetic waves without the need for a medium.
In natural convection, as the fluid heats up and moves due to buoyancy forces, thermal energy is transferred to different parts of the fluid, as well as to any surfaces the fluid comes in contact with. This results in a gradual equalization of temperature, showcasing the powerful role of heat transfer in processes like atmospheric currents, ocean currents, and even heating food in a pot.
Density Variations
Density variations are central to the occurrence of natural convection. When fluid is heated or cooled, its density changes. Typically, heating a fluid decreases its density, as the molecules move faster and spread apart, whereas cooling a fluid increases its density as the molecules slow down and come closer together. These variations in density are what set natural convection into motion.

In natural convection, these density variations create differences in buoyancy forces within the fluid. Because less dense (warmer) fluid rises and more dense (cooler) fluid sinks, a continuous cycle of motion is established. This cycle is crucial, as the movement of fluid helps distribute heat and can assist in regulating temperature in both natural and engineered systems.
  • A heated fluid at the bottom of a container will rise because it is warmer and thus less dense.
  • Cooler fluid which is denser, will replace the space where the warm fluid used to be, starting a convection current.
This natural circulation due to density variations is vital in many natural phenomena, such as weather patterns, ocean currents, and even in engineered systems like heating and cooling in buildings.

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Most popular questions from this chapter

A circular grill of diameter \(0.25 \mathrm{~m}\) has an emissivity of \(0.8\). If the surface temperature is maintained at \(150^{\circ} \mathrm{C}\), determine the required electrical power when the room air and surroundings are at \(30^{\circ} \mathrm{C}\).

A 150 -mm-diameter and 1-m-long rod is positioned horizontally and has water flowing across its outer surface at a velocity of \(0.2 \mathrm{~m} / \mathrm{s}\). The water temperature is uniform at \(40^{\circ} \mathrm{C}\) and the rod surface temperature is maintained at \(120^{\circ} \mathrm{C}\). Under these conditions are the natural convection effects important to the heat transfer process?

A room is to be heated by a coal-burning stove, which is a cylindrical cavity with an outer diameter of \(32 \mathrm{~cm}\) and a height of \(70 \mathrm{~cm}\). The rate of heat loss from the room is estimated to be \(1.5 \mathrm{~kW}\) when the air temperature in the room is maintained constant at \(24^{\circ} \mathrm{C}\). The emissivity of the stove surface is \(0.85\), and the average temperature of the surrounding wall surfaces is \(14^{\circ} \mathrm{C}\). Determine the surface temperature of the stove. Neglect the heat transfer from the bottom surface and take the heat transfer coefficient at the top surface to be the same as that on the side surface. The heating value of the coal is \(30,000 \mathrm{~kJ} / \mathrm{kg}\), and the combustion efficiency is 65 percent. Determine the amount of coal burned a day if the stove operates \(14 \mathrm{~h}\) a day. Evaluate air properties at a film temperature of \(77^{\circ} \mathrm{C}\) and \(1 \mathrm{~atm}\) pressure. Is this a good assumption?

The primary driving force for natural convection is (a) shear stress forces (b) buoyancy forces (c) pressure forces (d) surface tension forces (e) none of them

A \(1.5\)-m-diameter, 4-m-long cylindrical propane tank is initially filled with liquid propane, whose density is \(581 \mathrm{~kg} / \mathrm{m}^{3}\). The tank is exposed to the ambient air at \(25^{\circ} \mathrm{C}\) in calm weather. The outer surface of the tank is polished so that the radiation heat transfer is negligible. Now a crack develops at the top of the tank, and the pressure inside drops to \(1 \mathrm{~atm}\) while the temperature drops to \(-42^{\circ} \mathrm{C}\), which is the boiling temperature of propane at \(1 \mathrm{~atm}\). The heat of vaporization of propane at \(1 \mathrm{~atm}\) is \(425 \mathrm{~kJ} / \mathrm{kg}\). The propane is slowly vaporized as a result of the heat transfer from the ambient air into the tank, and the propane vapor escapes the tank at \(-42^{\circ} \mathrm{C}\) through the crack. Assuming the propane tank to be at about the same temperature as the propane inside at all times, determine how long it will take for the tank to empty if it is not insulated.

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