Coriolis and different refererence frames

In summary, the conversation discusses the Coriolis force and its effects on an object being dropped or thrown from Earth's surface. The speaker is seeking clarification on how to calculate the eastward and westward deflections in an inertial frame. The conversation also mentions a Java applet that can aid in visualizing the motion and provides a simplified explanation of the Coriolis effect. The speaker also mentions a textbook by Stephen Thornton and Jerry Marion that discusses this topic.
  • #1
Wondering
4
0
Hello,

I am stuck on the coriolis force. If an object is dropped how do I get the eastward deflection when looking from an inertial frame? I know how from the rotating frame but for some reason I am stuck, i.e. what terms to use.
Also, if I throw a ball straight up from Earth what is the westward deflection, do I solve this twice? Once for the ball moving up and then again once it is at the max height falling down?

Thank you
 
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  • #2
Wondering said:
Hello,
I am stuck on the coriolis force. If an object is dropped how do I get the eastward deflection when looking from an inertial frame?
What you see there initially is the ball that has the same angular velocity but a higher tangential velocity than the ground. As it descends it outruns the ground due to that higher tangential velocity. The angular velocity of the ball increases to preserve it's angular momentum.
Wondering said:
Also, if I throw a ball straight up from Earth what is the westward deflection, do I solve this twice? Once for the ball moving up and then again once it is at the max height falling down?
Yes the west acceleration during rise is canceled by the east acceleration during fall, so the ball lands with zero velocity in the east-west direction, but in a point west to the throw position. The defection is the same during both phases, so you just calculate it once and multiply by two.
 
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  • #3
Wondering said:
Hello,
I am stuck on the coriolis force. If an object is dropped how do I get the eastward deflection when looking from an inertial frame? I know how from the rotating frame but for some reason I am stuck, i.e. what terms to use.
Also, if I throw a ball straight up from Earth what is the westward deflection, do I solve this twice? Once for the ball moving up and then again once it is at the max height falling down?
Thank you

I won't give you the derivations, but you can check your results against the following Java applet that is available on my website. http://www.cleonis.nl/physics/ejs/ballistics_and_orbits_simulation.php"
The Coriolis effect is the main subject of my website. (http://www.cleonis.nl)

The applet http://www.cleonis.nl/physics/ejs/ballistics_and_orbits_simulation.php" shows the motion of a launched object. The panel on the left shows the motion with respect to the inertial coordinate system, the panel on the right shows the motion with respect to the coordinate system that is co-rotating with the Earth.

You can launch from any latitude, you can launch at any angle (eastward, westward etc), you can launch at any elevation, and you can specify the nozzle velocity (zero for release to free motion, high speed for launch with a gun.)

If memory serves me the textbook 'Classical dynamics' by (authors Stephen Thornton and Jerry Marion) offers several discussions.

If an object is dropped from a high tower, why does it not land at the base of the tower? Answer: (simplified version that neglects air resistance effects). Once the object is released it is effectively in orbital motion. (An orbit that will be shortlived, as it intersects the Earth's surface.)
There is Kepler's law for orbital motion: when an orbiting object is pulled closer to its primary its speed increases, (in such a way that equal areas are swept out in equal intervals of time.)
An extreme example is the orbit of Halley's comet: during the part of the orbit that the comet is falling to the center of the solar system the comet is gaining speed all the time. Halley's comet sweeps around the Sun, and then starts climbing outward again. Moving against the pull of the Sun the comet is losing velocity all the time.

Returning to the example of releasing an object from the top of a high tower: the Earth's gravity is pulling the object in, so the angular velocity of the object increases. The Java applet I mentioned is also designed to illustrate the 'object released from high tower' scenario.

In this particular case the fastest calculation strategy to obtain the motion with respect to the inertial coordinate system is to apply conservation of angular momentum.

Cleonis
http://www.cleonis.nl
 
Last edited by a moderator:

Related to Coriolis and different refererence frames

1. What is the Coriolis effect?

The Coriolis effect is the apparent deflection of an object's path due to the rotation of the Earth. This effect is caused by the difference in linear velocity between different latitudes on Earth.

2. How does the Coriolis effect impact weather patterns?

The Coriolis effect plays a significant role in the formation of weather patterns. It causes air masses to rotate in a clockwise direction in the Northern Hemisphere and counterclockwise in the Southern Hemisphere, which helps to create high and low-pressure systems.

3. Can the Coriolis effect be observed in everyday life?

Yes, the Coriolis effect can be observed in everyday life. For example, water draining from a sink or bathtub will rotate in a different direction depending on which hemisphere you are in, due to the Coriolis effect.

4. How does the Coriolis effect impact ocean currents?

The Coriolis effect also plays a significant role in ocean currents. In the Northern Hemisphere, ocean currents are deflected to the right, while in the Southern Hemisphere, they are deflected to the left. This is due to the Coriolis effect acting on the water as it moves across the Earth's surface.

5. Can the Coriolis effect impact the trajectory of a moving object?

Yes, the Coriolis effect can impact the trajectory of a moving object, such as an airplane or a missile. It can cause the object to veer off course if the rotation of the Earth is not taken into account in its flight path.

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