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An introduction to creating and using loops in VPython. | |||
==The Main Idea== | |||
The most commonly used loop structures in VPython are the 'for' loop and the 'while' loop. In Physics modeling, the 'for' loop is useful when one wants to check a condition before running the code in the 'for' loop. For example, the code following the statement -- 'for i in range(0,3):' -- will only run when i is within the specified range. The 'while' loop is useful when one wants to run a code for a specified interval or while a condition is true. For example, the code following the statement -- 'while t < 100:' -- will run until t is greater than or equal to 100 (1,2,3). | |||
===A Mathematical Model=== | |||
When computing iterations for physics problems, using the iterative method with small delta t increments can produce near accurate results. To have truly small delta t increments, however, computational modeling is necessary for computation. | |||
In a problem that requires use of the momentum principle and a specific number of time steps for iteration, we update momentum for each time step using the following equation: | |||
<pre> | |||
delta P = Fnet * deltat | |||
</pre> | |||
With this equation, the final momentum is updated after each time step (deltat) up to a time (t). We can only manually do this with a small number of increments, however, and as a result, with less accuracy than if our delta t increments were smaller. This is where computational modeling and VPython loops come in. | |||
===A Computational Model=== | |||
With computational modeling using VPython, we can reduce the size of delta t and increase the number of time steps in the approximation of an iteration. Instead of two or three time steps, VPython loops make it possible to test infinitely small time steps, making the final result more accurate. For example, to calculate an approximation from t = 0 to t = 2 using two time steps, one could write the following time update: | |||
== | <pre> | ||
deltat = 1 | |||
t = 0 | |||
while t < 2: | |||
t += deltat | |||
</pre> | |||
However, loops can be used to test much smaller time steps than deltat = 1; the smaller the time step, the more accurate the iteration. | |||
== | ==Examples== | ||
The following examples cover a range of loops that can be created in VPython from the simplest 'for' loops to more complicated 'for' and 'while' loops. | |||
===Simple=== | |||
The simplest example is a basic 'for' loop. The following code will print each integer in a range: | |||
<pre> | |||
for i in range(0,10): | |||
print i | |||
</pre> | |||
The same thing can be accomplished with a 'while' loop as well. See the following: | |||
<pre> | |||
i = 0 | |||
while i < 10: | |||
print i | |||
i += 1 | |||
</pre> | |||
When modeling momentum updates, using a 'while' loop allows the code to run until Tfinal has been reached by adding deltat to t each time the loop runs. | |||
===Middling=== | |||
To solve more complex problems, we need to create values and objects before the loop that will then be updated within the loop until a certain time, t. In the following example, the final position and final velocity of object ball is updated until t = 10 using a time step of deltat = 1. | |||
== | <pre> | ||
t = 0 | |||
deltat = 1 | |||
while t < 10: | |||
Fgrav = vector(0,-ball.m*g,0) | |||
Fdrag=(.5)*dragCoeff*airDensity*areaBall*mag(ball.p/ball.m)**2*norm(ball.p) | |||
Fnet = Fgrav - Fdrag | |||
= | ball.p = ball.p + Fnet*deltat | ||
ball.pos = ball.pos + (ball.p/ball.m)*deltat | |||
ball = | |||
t += deltat | |||
print(ball.pos) #prints final ball position | |||
print(ball.p/mball) #prints final ball velocity | |||
</pre> | |||
===Difficult=== | |||
The following code calculates the final position and velocity of a ball attached to a string mounted to a ceiling. After code is written listing the constants, creating the objects, and setting an initial value of t = 0, the following statements update the position and velocity values until t = 10 seconds. | |||
<pre> | |||
t = 0 | |||
deltat = 1 | |||
while t < 10: | |||
L = ball.pos - ceiling.pos | |||
s=mag(L) - L0 | |||
Lhat = L/mag(L) | |||
Fs = -(ks)*s*Lhat | |||
Fg = vector(0,-g*mball,0) | |||
Fdrag = (-1)*b*(ball.p/mball) | |||
Fnet = Fg + Fs + Fdrag | |||
ball.p = ball.p + Fnet*deltat | |||
ball.pos = ball.pos + (ball.p/(mball))*deltat | |||
spring.axis = ball.pos - ceiling.pos | |||
t += deltat | |||
print(ball.pos) #prints final ball position | |||
print(ball.p/mball) #prints final ball velocity | |||
</pre> | |||
== | ==Connectedness== | ||
Understanding the basics of VPython creates a framework for more easily learning to write in coding languages other than Python. Additionally, understanding the basics of the 'for' loop and the 'while' loop enables one to write more complex code using both 'for' and 'while' loops, even nesting both types of loops in creating complex conditionals. In more advanced Physics modeling, being able to write more complex conditional statements enables these more complex equations and relationships to be solved via computational modeling. | |||
Even for non-computing majors, coding experience is a highly valuable trait employers are increasingly looking for in candidates. In 2016, analytics firm Burning Glass reported that programming jobs were growing 12% faster than the market average. Additionally, half of the projected job openings looking for programming experience are in non-technology fields such as 'finance, manufacturing, and healthcare' (4). In 2017, Forbes ranked Python as the top-ranked in-demand coding language among the top five: 'Python, Java, JavaScript, C#, and PHP' (5). | |||
== | ==History== | ||
Python is an interpreted language that originated in the 1980s and was released from development in the 1990s. Because it is interpreted, compiling is not required to convert lines of code into machine-understandable instructions (6). In 1998, David Scherer saw a need for a better 2D and 3D graphics programming environment and created the idea for Visual (a.k.a. VPython), a Python module (7). | |||
=== | ==See Also== | ||
===Further Reading=== | |||
'Why Coding Is Still The Most Important Job Skill Of The Future' (Dishman, 2016) | |||
'The Five Most In-Demand Coding Languages' (Kauflin, 2017) | |||
===External Links=== | |||
http://vpython.org/contents/docs/VisualIntro.html | |||
http://vpython.org/contents/docs/ | |||
https://faculty.math.illinois.edu/~gfrancis/illimath/windows/aszgard_mini/pylibs/visual/docs/visual/VisualIntro.html | |||
https://www.fastcompany.com/3060883/why-coding-is-the-job-skill-of-the-future-for-everyone | |||
https://www.forbes.com/sites/jeffkauflin/2017/05/12/the-five-most-in-demand-coding-languages/#6b86011fb3f5 | |||
https://en.wikipedia.org/wiki/Python_(programming_language) | |||
https://en.wikipedia.org/wiki/VPython#History | |||
==References== | |||
1. http://vpython.org/contents/docs/VisualIntro.html | |||
2. http://vpython.org/contents/docs/ | |||
3. https://faculty.math.illinois.edu/~gfrancis/illimath/windows/aszgard_mini/pylibs/visual/docs/visual/VisualIntro.html | |||
4. https://www.fastcompany.com/3060883/why-coding-is-the-job-skill-of-the-future-for-everyone | |||
5. https://www.forbes.com/sites/jeffkauflin/2017/05/12/the-five-most-in-demand-coding-languages/#6b86011fb3f5 | |||
6. https://en.wikipedia.org/wiki/Python_(programming_language) | |||
7. https://en.wikipedia.org/wiki/VPython#History |
Latest revision as of 02:52, 22 October 2019
An introduction to creating and using loops in VPython.
The Main Idea
The most commonly used loop structures in VPython are the 'for' loop and the 'while' loop. In Physics modeling, the 'for' loop is useful when one wants to check a condition before running the code in the 'for' loop. For example, the code following the statement -- 'for i in range(0,3):' -- will only run when i is within the specified range. The 'while' loop is useful when one wants to run a code for a specified interval or while a condition is true. For example, the code following the statement -- 'while t < 100:' -- will run until t is greater than or equal to 100 (1,2,3).
A Mathematical Model
When computing iterations for physics problems, using the iterative method with small delta t increments can produce near accurate results. To have truly small delta t increments, however, computational modeling is necessary for computation.
In a problem that requires use of the momentum principle and a specific number of time steps for iteration, we update momentum for each time step using the following equation:
delta P = Fnet * deltat
With this equation, the final momentum is updated after each time step (deltat) up to a time (t). We can only manually do this with a small number of increments, however, and as a result, with less accuracy than if our delta t increments were smaller. This is where computational modeling and VPython loops come in.
A Computational Model
With computational modeling using VPython, we can reduce the size of delta t and increase the number of time steps in the approximation of an iteration. Instead of two or three time steps, VPython loops make it possible to test infinitely small time steps, making the final result more accurate. For example, to calculate an approximation from t = 0 to t = 2 using two time steps, one could write the following time update:
deltat = 1 t = 0 while t < 2: t += deltat
However, loops can be used to test much smaller time steps than deltat = 1; the smaller the time step, the more accurate the iteration.
Examples
The following examples cover a range of loops that can be created in VPython from the simplest 'for' loops to more complicated 'for' and 'while' loops.
Simple
The simplest example is a basic 'for' loop. The following code will print each integer in a range:
for i in range(0,10): print i
The same thing can be accomplished with a 'while' loop as well. See the following:
i = 0 while i < 10: print i i += 1
When modeling momentum updates, using a 'while' loop allows the code to run until Tfinal has been reached by adding deltat to t each time the loop runs.
Middling
To solve more complex problems, we need to create values and objects before the loop that will then be updated within the loop until a certain time, t. In the following example, the final position and final velocity of object ball is updated until t = 10 using a time step of deltat = 1.
t = 0 deltat = 1 while t < 10: Fgrav = vector(0,-ball.m*g,0) Fdrag=(.5)*dragCoeff*airDensity*areaBall*mag(ball.p/ball.m)**2*norm(ball.p) Fnet = Fgrav - Fdrag ball.p = ball.p + Fnet*deltat ball.pos = ball.pos + (ball.p/ball.m)*deltat t += deltat print(ball.pos) #prints final ball position print(ball.p/mball) #prints final ball velocity
Difficult
The following code calculates the final position and velocity of a ball attached to a string mounted to a ceiling. After code is written listing the constants, creating the objects, and setting an initial value of t = 0, the following statements update the position and velocity values until t = 10 seconds.
t = 0 deltat = 1 while t < 10: L = ball.pos - ceiling.pos s=mag(L) - L0 Lhat = L/mag(L) Fs = -(ks)*s*Lhat Fg = vector(0,-g*mball,0) Fdrag = (-1)*b*(ball.p/mball) Fnet = Fg + Fs + Fdrag ball.p = ball.p + Fnet*deltat ball.pos = ball.pos + (ball.p/(mball))*deltat spring.axis = ball.pos - ceiling.pos t += deltat print(ball.pos) #prints final ball position print(ball.p/mball) #prints final ball velocity
Connectedness
Understanding the basics of VPython creates a framework for more easily learning to write in coding languages other than Python. Additionally, understanding the basics of the 'for' loop and the 'while' loop enables one to write more complex code using both 'for' and 'while' loops, even nesting both types of loops in creating complex conditionals. In more advanced Physics modeling, being able to write more complex conditional statements enables these more complex equations and relationships to be solved via computational modeling.
Even for non-computing majors, coding experience is a highly valuable trait employers are increasingly looking for in candidates. In 2016, analytics firm Burning Glass reported that programming jobs were growing 12% faster than the market average. Additionally, half of the projected job openings looking for programming experience are in non-technology fields such as 'finance, manufacturing, and healthcare' (4). In 2017, Forbes ranked Python as the top-ranked in-demand coding language among the top five: 'Python, Java, JavaScript, C#, and PHP' (5).
History
Python is an interpreted language that originated in the 1980s and was released from development in the 1990s. Because it is interpreted, compiling is not required to convert lines of code into machine-understandable instructions (6). In 1998, David Scherer saw a need for a better 2D and 3D graphics programming environment and created the idea for Visual (a.k.a. VPython), a Python module (7).
See Also
Further Reading
'Why Coding Is Still The Most Important Job Skill Of The Future' (Dishman, 2016) 'The Five Most In-Demand Coding Languages' (Kauflin, 2017)
External Links
http://vpython.org/contents/docs/VisualIntro.html http://vpython.org/contents/docs/ https://faculty.math.illinois.edu/~gfrancis/illimath/windows/aszgard_mini/pylibs/visual/docs/visual/VisualIntro.html https://www.fastcompany.com/3060883/why-coding-is-the-job-skill-of-the-future-for-everyone https://www.forbes.com/sites/jeffkauflin/2017/05/12/the-five-most-in-demand-coding-languages/#6b86011fb3f5 https://en.wikipedia.org/wiki/Python_(programming_language) https://en.wikipedia.org/wiki/VPython#History
References
1. http://vpython.org/contents/docs/VisualIntro.html 2. http://vpython.org/contents/docs/ 3. https://faculty.math.illinois.edu/~gfrancis/illimath/windows/aszgard_mini/pylibs/visual/docs/visual/VisualIntro.html 4. https://www.fastcompany.com/3060883/why-coding-is-the-job-skill-of-the-future-for-everyone 5. https://www.forbes.com/sites/jeffkauflin/2017/05/12/the-five-most-in-demand-coding-languages/#6b86011fb3f5 6. https://en.wikipedia.org/wiki/Python_(programming_language) 7. https://en.wikipedia.org/wiki/VPython#History