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That was a rather bold statement in that time period, and it took more than three hundred years before anyone performed a successful parachute jump (1797)1. The design was a bit different than the one shown in the Da Vinci sketch, but the principles involved were the same (Leonardo's design was proven viable more than 500 years after his sketch was done2). Let's take a closer look at the principles behind the parachute. First, a question: Why do we use a parachute when jumping from a high altitude? One answer is obvious - the parachutist wants to be moving slowly so that he/she can land with no problems! From a physics standpoint, the goal is to oppose the force of gravity which is acting downward on you with a constant force. Thus, the goal of the parachute is to oppose the gravitational force, and this is done by a drag force which acts upward. In simple terms, a drag force is a force that created when trying
to move The drag force tends to always oppose the direction of motion so when something is falling downward through the sky the drag force acts upward.
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With the Freefall
Lab we can study how things behave as they are falling
This Gizmo represents a laboratory situation in which a sonic ranger (a device which measures distance at specific time intervals) is placed at a certain distance above the ground and objects can be studied as they are falling beneath the sonic ranger. Freefall Lab In this activity there are many possible teaching opportunities. We'll walk through one aspect this month and discuss another next month. Notice that there are many variables that can be changed in this simulation.
Set the radius of the ball to 0.02 meters, the mass to 0.25 kilograms.
Leave all Find the average acceleration during the drop. Since this is a relatively heavy object with a small radius the acceleration should be approximately 9.8 m/s2. Was this the case. If not, there might be a small bit of systematic error in the sonic ranger. Keep this in mind for future readings. Reduce the mass of the ball several times and continue to find the average acceleration (it is sometimes helpful to use the 'Clear Trails' button between releases). Suggested values are 0.15 kg, 0.10 kg, 0.05 kg, and 0.01 kg. Is the average acceleration changing as the mass changes? Make a plot of average acceleration vs. the density of the falling object. Recall that density = M/V where M is the mass of the sphere and V is the volume of the sphere. Is there a trend shown in the data that was obtained? How could you test this trend? If possible change the radius of the object and select a mass in such a way that the density of the object can be found on your graph. Does it fit in with the trend? If not, what are some possible reasons? Next month we will discuss terminal velocity. |
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