GO Icicles. Liquid water coats an active (growing) icicle and extends up a short, narrow tube along the central axis (Fig 18-55). Because the water–ice interface must have a temperature of 0°C, the water in the tube cannot lose energy through the sides of the icicle or down through the tip because there is no temperature change in those directions. It can lose energy and freeze only by sending energy up (through distance L ) to the top of the icicle, where the temperature T r can be below 0°C. Take L = 0.12 m and T r = −5°C. Assume that the central tube and the upward conduction path both have cross-sectional area A. In terms of A , what rate is (a) energy conducted upward and (b) mass converted from liquid to ice at the top of the central tube? (c) At what rate does the top of the tube move downward because of water freezing there? The thermal conductivity of ice is 0.400 W/mžK, and the density of liquid water is 1000 kg/m 3 . Figure 18-55 Problem 78.
GO Icicles. Liquid water coats an active (growing) icicle and extends up a short, narrow tube along the central axis (Fig 18-55). Because the water–ice interface must have a temperature of 0°C, the water in the tube cannot lose energy through the sides of the icicle or down through the tip because there is no temperature change in those directions. It can lose energy and freeze only by sending energy up (through distance L ) to the top of the icicle, where the temperature T r can be below 0°C. Take L = 0.12 m and T r = −5°C. Assume that the central tube and the upward conduction path both have cross-sectional area A. In terms of A , what rate is (a) energy conducted upward and (b) mass converted from liquid to ice at the top of the central tube? (c) At what rate does the top of the tube move downward because of water freezing there? The thermal conductivity of ice is 0.400 W/mžK, and the density of liquid water is 1000 kg/m 3 . Figure 18-55 Problem 78.
GOIcicles. Liquid water coats an active (growing) icicle and extends up a short, narrow tube along the central axis (Fig 18-55). Because the water–ice interface must have a temperature of 0°C, the water in the tube cannot lose energy through the sides of the icicle or down through the tip because there is no temperature change in those directions. It can lose energy and freeze only by sending energy up (through distance L) to the top of the icicle, where the temperature Tr can be below 0°C. Take L = 0.12 m and Tr = −5°C. Assume that the central tube and the upward conduction path both have cross-sectional area A. In terms of A, what rate is (a) energy conducted upward and (b) mass converted from liquid to ice at the top of the central tube? (c) At what rate does the top of the tube move downward because of water freezing there? The thermal conductivity of ice is 0.400 W/mžK, and the density of liquid water is 1000 kg/m3.
Part C
Find the height yi
from which the rock was launched.
Express your answer in meters to three significant figures.
Learning Goal:
To practice Problem-Solving Strategy 4.1 for projectile motion problems.
A rock thrown with speed 12.0 m/s and launch angle 30.0 ∘ (above the horizontal) travels a horizontal distance of d = 19.0 m before hitting the ground. From what height was the rock thrown? Use the value g = 9.800 m/s2 for the free-fall acceleration.
PROBLEM-SOLVING STRATEGY 4.1 Projectile motion problems
MODEL: Is it reasonable to ignore air resistance? If so, use the projectile motion model.
VISUALIZE: Establish a coordinate system with the x-axis horizontal and the y-axis vertical. Define symbols and identify what the problem is trying to find. For a launch at angle θ, the initial velocity components are vix=v0cosθ and viy=v0sinθ.
SOLVE: The acceleration is known: ax=0 and ay=−g. Thus, the problem becomes one of…
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