58192
Comment:
|
58516
|
Deletions are marked like this. | Additions are marked like this. |
Line 10: | Line 10: |
[[http://aleph.sagemath.org/?z=eJytU02P2yAQvedXjCxFC4njJP06bOOqrdqe9hBVbS-rNMIY1ki2sQDvev99B5zYzq62l5aDPcDw5jHvkQsJmbKCu2MlXKFzImNgMWQxiMbS6xngcOaxD_yQkIJMjpJZd5SlZu5IZHLPjGJZKSyht5sDDcmi46Jx8Mk5o7LWia_GaDPiNMzaMFG1E-aelRaBbwmLM3roqz5oX8qXIK_oe89nmHtuIemhUKWAH6YVIzLHNMKWGV0jxMib-dOEIZLMQpj5kIeQ0yFPSWCZJZJT2Pma12CEa00NPB6pTrMlWyDKDjYjAz98ExEbf3xYF6XP5wsk8FI-Vskm-VZcZhmGYsEvVrZ9P2OIJFStdVCwewEMrLpDqgWr7wTSBVeIgTWQuY3nlkbz0OXxDudbJaxpRJ2TsE1nhatKEu2K7YcvukVxYW8EV1bpGr5r7eCbqnNV38FP67-fg4twc7fGExGdfQy4jLtZjiZDl_jbaUs6Civo0GWDmhva372fbWnwXkpWr2Oy2r5LktWW0pMVUauOprKPe0dsN78x6Fcag0Uh6jfmNpo_scullcGpSlzoiqf-8hpOVXtfjxpMAE_1p5LoptFWOdErw1yQBLvcaEy1oOWFRtGIZQv9QJpSu5EE16U26ZUR-RU2qatUnTL_Z1161vOJZU6EjNcrjaZeHLii-X2zDDZr-g7O-8qL6HW1AaAUNRnaNcneI8bLZMe8wj_OffKInIk3gg9VTShdA9kmbxeX-JODN3jQthUpVS3ILeFxsVDYBJKH4EBBagMKF3icU299UbeVpy4meHABuHyOuCrWb2gAwcnST_4Dcj5Fzv8FOXhiD0u4eSb_HxOSmYw%3D|Interact]] {{{ |
{{{#!sagecell |
Line 60: | Line 59: |
{{{ | {{{#!sagecell |
Line 102: | Line 101: |
{{{ | {{{#!sagecell |
Line 118: | Line 117: |
{{{ | {{{#!sagecell |
Line 138: | Line 137: |
{{{ | {{{#!sagecell |
Line 166: | Line 165: |
{{{ | {{{#!sagecell |
Line 239: | Line 238: |
{{{ | {{{#!sagecell |
Line 252: | Line 251: |
{{{ | {{{#!sagecell |
Line 350: | Line 349: |
{{{ | {{{#!sagecell |
Line 456: | Line 455: |
{{{ | {{{#!sagecell |
Line 458: | Line 457: |
# polar coordinates #(x,y)=(u*cos(v),u*sin(v)); (u_range,v_range)=([0..6],[0..2*pi,step=pi/12]) # weird example (x,y)=(u^2-v^2,u*v+cos(u*v)); (u_range,v_range)=([-5..5],[-5..5]) thickness=4 square_length=.05 |
|
Line 461: | Line 469: |
def trans(x=input_box(u^2-v^2, label="x=",type=SR), \ y=input_box(u*v+cos(u*v), label="y=",type=SR), \ t_val=slider(0,10,0.2,6, label="Length of curves"), \ |
def trans(x=input_box(x, label="x",type=SR), y=input_box(y, label="y",type=SR), |
Line 466: | Line 473: |
u_range=input_box(range(-5,5,1), label="u lines"), v_range=input_box(range(-5,5,1), label="v lines")): thickness=4 u_val = min(u_range)+(max(u_range)-min(u_range))*u_percent v_val = min(v_range)+(max(v_range)-min(v_range))*v_percent t_min = -t_val t_max = t_val g1=sum([parametric_plot((i,v), (v,t_min,t_max), rgbcolor=(1,0,0)) for i in u_range]) g2=sum([parametric_plot((u,i), (u,t_min,t_max), rgbcolor=(0,0,1)) for i in v_range]) vline_straight=parametric_plot((u,v_val), (u,t_min,t_max), rgbcolor=(0,0,1), linestyle='-',thickness=thickness) uline_straight=parametric_plot((u_val, v), (v,t_min,t_max),rgbcolor=(1,0,0), linestyle='-',thickness=thickness) (g1+g2+vline_straight+uline_straight).save("uv_coord.png",aspect_ratio=1, figsize=[5,5], axes_labels=['$u$','$v$']) xuv = fast_float(x,'u','v') yuv = fast_float(y,'u','v') xvu = fast_float(x,'v','u') yvu = fast_float(y,'v','u') g3=sum([parametric_plot((partial(xuv,i),partial(yuv,i)), (v,t_min,t_max), rgbcolor=(1,0,0)) for i in u_range]) g4=sum([parametric_plot((partial(xvu,i),partial(yvu,i)), (u,t_min,t_max), rgbcolor=(0,0,1)) for i in v_range]) uline=parametric_plot((partial(xuv,u_val),partial(yuv,u_val)),(v,t_min,t_max),rgbcolor=(1,0,0), linestyle='-',thickness=thickness) vline=parametric_plot((partial(xvu,v_val),partial(yvu,v_val)), (u,t_min,t_max), rgbcolor=(0,0,1), linestyle='-',thickness=thickness) (g3+g4+vline+uline).save("xy_coord.png", aspect_ratio=1, figsize=[5,5], axes_labels=['$x$','$y$']) print jsmath("x=%s, \: y=%s"%(latex(x), latex(y))) print "<html><table><tr><td><img src='cell://uv_coord.png'/></td><td><img src='cell://xy_coord.png'/></td></tr></table></html>" }}} |
t_val=slider(0,10,0.2,6, label="Length"), u_range=input_box(u_range, label="u lines"), v_range=input_box(v_range, label="v lines")): x(u,v)=x y(u,v)=y u_val = min(u_range)+(max(u_range)-min(u_range))*u_percent v_val = min(v_range)+(max(v_range)-min(v_range))*v_percent t_min = -t_val t_max = t_val uvplot=sum([parametric_plot((i,v), (v,t_min,t_max), color='red',axes_labels=['u','v'],figsize=[5,5]) for i in u_range]) uvplot+=sum([parametric_plot((u,i), (u,t_min,t_max), color='blue',axes_labels=['u','v']) for i in v_range]) uvplot+=parametric_plot((u,v_val), (u,t_min,t_max), rgbcolor=(0,0,1), linestyle='-',thickness=thickness) uvplot+=parametric_plot((u_val, v), (v,t_min,t_max),rgbcolor=(1,0,0), linestyle='-',thickness=thickness) pt=vector([u_val,v_val]) du=vector([(t_max-t_min)*square_length,0]) dv=vector([0,(t_max-t_min)*square_length]) uvplot+=polygon([pt,pt+dv,pt+du+dv,pt+du],color='purple',alpha=0.7) uvplot+=line([pt,pt+dv,pt+du+dv,pt+du],color='green') T(u,v)=(x,y) xuv = fast_float(x,'u','v') yuv = fast_float(y,'u','v') xvu = fast_float(x,'v','u') yvu = fast_float(y,'v','u') xyplot=sum([parametric_plot((partial(xuv,i),partial(yuv,i)), (v,t_min,t_max), color='red', axes_labels=['x','y'],figsize=[5,5]) for i in u_range]) xyplot+=sum([parametric_plot((partial(xvu,i),partial(yvu,i)), (u,t_min,t_max), color='blue') for i in v_range]) xyplot+=parametric_plot((partial(xuv,u_val),partial(yuv,u_val)),(v,t_min,t_max),color='red', linestyle='-',thickness=thickness) xyplot+=parametric_plot((partial(xvu,v_val),partial(yvu,v_val)), (u,t_min,t_max), color='blue', linestyle='-',thickness=thickness) jacobian=abs(T.diff().det()).simplify_full() t_vals=[0..1,step=t_val*.01] vertices=[(x(*c),y(*c)) for c in [pt+t*dv for t in t_vals]] vertices+=[(x(*c),y(*c)) for c in [pt+dv+t*du for t in t_vals]] vertices+=[(x(*c),y(*c)) for c in [pt+(1-t)*dv+du for t in t_vals]] vertices+=[(x(*c),y(*c)) for c in [pt+(1-t)*du for t in t_vals]] xyplot+=polygon(vertices,color='purple',alpha=0.7) xyplot+=line(vertices,color='green') html("$T(u,v)=%s$"%(latex(T(u,v)))) html("Jacobian: $%s$"%latex(jacobian(u,v))) html("A very small region in $xy$ plane is approximately %0.4g times the size of the corresponding region in the $uv$ plane"%jacobian(u_val,v_val).n()) html.table([[uvplot,xyplot]])}}} |
Line 498: | Line 521: |
{{{ | {{{#!sagecell |
Line 521: | Line 544: |
{{{ | {{{#!sagecell |
Line 548: | Line 571: |
{{{ | {{{#!sagecell |
Line 574: | Line 597: |
{{{ | {{{#!sagecell |
Line 589: | Line 612: |
{{{ | {{{#!sagecell |
Line 635: | Line 658: |
{{{ from scipy.special.orthogonal import p_roots |
{{{#!sagecell import scipy import numpy from scipy.special.orthogonal import p_roots, t_roots, u_roots |
Line 645: | Line 670: |
'Chebyshev': {'w': 1/sqrt(1-x**2), 'xmin': -1, 'xmax': 1, 'func': t_roots}, 'Chebyshev2': {'w': sqrt(1-x**2), 'xmin': -1, 'xmax': 1, 'func': u_roots}, 'Trapezoid': {'w': 1, 'xmin': -1, 'xmax': 1, 'func': lambda n: (linspace(-1r,1,n), numpy.array([1.0r]+[2.0r]*(n-2)+[1.0r])*1.0r/n)}, 'Simpson': {'w': 1, 'xmin': -1, 'xmax': 1, 'func': lambda n: (linspace(-1r,1,n), numpy.array([1.0r]+[4.0r,2.0r]*int((n-3.0r)/2.0r)+[4.0r,1.0r])*2.0r/(3.0r*n))}} |
'Chebyshev': {'w': 1/sqrt(1-x**2), 'xmin': -1, 'xmax': 1, 'func': t_roots}, 'Chebyshev2': {'w': sqrt(1-x**2), 'xmin': -1, 'xmax': 1, 'func': u_roots}, 'Trapezoid': {'w': 1, 'xmin': -1, 'xmax': 1, 'func': lambda n: (linspace(-1r,1,n), numpy.array([1.0r]+[2.0r]*(n-2)+[1.0r])*1.0r/n)}, 'Simpson': {'w': 1, 'xmin': -1, 'xmax': 1, 'func': lambda n: (linspace(-1r,1,n), numpy.array([1.0r]+[4.0r,2.0r]*int((n-3.0r)/2.0r)+[4.0r,1.0r])*2.0r/(3.0r*n))}} |
Line 652: | Line 680: |
return polygon([(center-width2,0),(center+width2,0),(center+width2,height),(center-width2,height)],**kwds) | return polygon([(center-width2,0), (center+width2,0),(center+width2,height),(center-width2,height)],**kwds) |
Line 656: | Line 685: |
def weights(n=slider(1,30,1,default=10),f=input_box(default=3*x+cos(10*x)),show_method=["Legendre", "Chebyshev", "Chebyshev2", "Trapezoid","Simpson"]): | def weights(n=slider(1,30,1,default=10),f=input_box(default=3*x+cos(10*x),type=SR), show_method=["Legendre", "Chebyshev", "Chebyshev2", "Trapezoid","Simpson"]): |
Line 665: | Line 695: |
scaled_ff = fast_float(scaled_func) | scaled_ff = fast_float(scaled_func, 'x') |
Line 673: | Line 703: |
stems = sum(line([(x,0),(x,scaled_ff(x))],rgbcolor=(1-y,1-y,1-y),thickness=2,markersize=6,alpha=y) for x,y in coords_scaled) points = sum([point([(x,0),(x,scaled_ff(x))],rgbcolor='black',pointsize=30) for x,_ in coords]) |
stems = sum(line([(x,0),(x,scaled_ff(x))],rgbcolor=(1-y,1-y,1-y), thickness=2,markersize=6,alpha=y) for x,y in coords_scaled) points = sum([point([(x,0), (x,scaled_ff(x))],rgbcolor='black',pointsize=30) for x,_ in coords]) |
Line 679: | Line 711: |
show(graph,xmin=plot_min,xmax=plot_max) | show(graph,xmin=plot_min,xmax=plot_max,aspect_ratio="auto") |
Line 687: | Line 719: |
html("$$\sum_{i=1}^{i=%s}w_i\left(%s\\right)= %s\\approx %s =\int_{-1}^{1}%s \,dx$$"%(n,latex(f.subs(x="x_i")), approximation, integral, latex(scaled_func))) | html("$$\sum_{i=1}^{i=%s}w_i\left(%s\\right)= %s\\approx %s =\int_{-1}^{1}%s \,dx$$"%(n, latex(f), approximation, integral, latex(scaled_func))) |
Line 700: | Line 733: |
{{{ | {{{#!sagecell |
Line 812: | Line 845: |
{{{ | {{{#!sagecell |
Line 849: | Line 882: |
velocity = derivative( position(t) ) acceleration = derivative(velocity(t)) |
velocity = derivative( position(t), t) acceleration = derivative(velocity(t), t) |
Line 852: | Line 885: |
speed_deriv = derivative(speed) | speed_deriv = derivative(speed, t) |
Line 854: | Line 887: |
dT = derivative(tangent(t)) | dT = derivative(tangent(t), t) |
Line 857: | Line 890: |
## dB = derivative(binormal(t)) | ## dB = derivative(binormal(t), t) |
Line 940: | Line 973: |
{{{ | {{{#!sagecell |
Line 975: | Line 1008: |
{{{ | {{{#!sagecell |
Line 1012: | Line 1045: |
{{{ | {{{#!sagecell |
Line 1065: | Line 1098: |
{{{ %hide %auto |
{{{#!sagecell |
Line 1126: | Line 1157: |
{{{ | {{{#!sagecell |
Line 1164: | Line 1195: |
{{{ | {{{#!sagecell |
Line 1204: | Line 1235: |
{{{ | {{{#!sagecell |
Line 1311: | Line 1342: |
{{{ | {{{#!sagecell |
Line 1368: | Line 1399: |
{{{ | {{{#!sagecell |
Line 1389: | Line 1420: |
{{{ | {{{#!sagecell |
Sage Interactions - Calculus
goto interact main page
Contents
-
Sage Interactions - Calculus
- Root Finding Using Bisection
- Newton's Method
- A contour map and 3d plot of two inverse distance functions
- A simple tangent line grapher
- Numerical integrals with the midpoint rule
- Numerical integrals with various rules
- Some polar parametric curves
- Function tool
- Newton-Raphson Root Finding
- Coordinate Transformations
- Taylor Series
- Illustration of the precise definition of a limit
- A graphical illustration of sin(x)/x -> 1 as x-> 0
- Quadric Surface Plotter
- The midpoint rule for numerically integrating a function of two variables
- Gaussian (Legendre) quadrature
- Vector Calculus, 2-D Motion
- Vector Calculus, 3-D Motion
- Multivariate Limits by Definition
- Directional Derivatives
- 3D graph with points and curves
- Approximating function in two variables by differential
- Taylor approximations in two variables
- Volumes over non-rectangular domains
- Lateral Surface Area
- Parametric surface example
- Line Integrals in 3D Vector Field
Root Finding Using Bisection
by William Stein
Newton's Method
Note that there is a more complicated Newton's method below.
by William Stein
http://sagenb.org/home/pub/2824/
A contour map and 3d plot of two inverse distance functions
by William Stein
http://sagenb.org/home/pub/2823/
A simple tangent line grapher
by Marshall Hampton
Numerical integrals with the midpoint rule
by Marshall Hampton
Numerical integrals with various rules
by Nick Alexander (based on the work of Marshall Hampton)
Some polar parametric curves
by Marshall Hampton. This is not very general, but could be modified to show other families of polar curves.
Function tool
Enter symbolic functions f, g, and a, a range, then click the appropriate button to compute and plot some combination of f, g, and a along with f and g. This is inspired by the Matlab funtool GUI.
Newton-Raphson Root Finding
by Neal Holtz
This allows user to display the Newton-Raphson procedure one step at a time. It uses the heuristic that, if any of the values of the controls change, then the procedure should be re-started, else it should be continued.
Coordinate Transformations
by Jason Grout
Taylor Series
by Harald Schilly
Illustration of the precise definition of a limit
by John Perry
I'll break tradition and put the image first. Apologies if this is Not A Good Thing.
A graphical illustration of sin(x)/x -> 1 as x-> 0
by Wai Yan Pong
Quadric Surface Plotter
by Marshall Hampton. This is pretty simple, so I encourage people to spruce it up. In particular, it isn't set up to show all possible types of quadrics.
The midpoint rule for numerically integrating a function of two variables
by Marshall Hampton
Gaussian (Legendre) quadrature
by Jason Grout
The output shows the points evaluated using Gaussian quadrature (using a weight of 1, so using Legendre polynomials). The vertical bars are shaded to represent the relative weights of the points (darker = more weight). The error in the trapezoid, Simpson, and quadrature methods is both printed out and compared through a bar graph. The "Real" error is the error returned from scipy on the definite integral.
Vector Calculus, 2-D Motion
By Rob Beezer
A fast_float() version is available in a worksheet
Vector Calculus, 3-D Motion
by Rob Beezer
Available as a worksheet
Multivariate Limits by Definition
by John Travis
http://www.sagenb.org/home/pub/2828/
Directional Derivatives
This interact displays graphically a tangent line to a function, illustrating a directional derivative (the slope of the tangent line).
3D graph with points and curves
By Robert Marik
This sagelet is handy when showing local, constrained and absolute maxima and minima in two variables. Available as a worksheet
Approximating function in two variables by differential
by Robert Marik
Taylor approximations in two variables
by John Palmieri
This displays the nth order Taylor approximation, for n from 1 to 10, of the function sin(x2 + y2) cos(y) exp(-(x2+y2)/2).
Volumes over non-rectangular domains
by John Travis
http://www.sagenb.org/home/pub/2829/
Lateral Surface Area
by John Travis
http://www.sagenb.org/home/pub/2826/
Parametric surface example
by Marshall Hampton
Line Integrals in 3D Vector Field
by John Travis
http://www.sagenb.org/home/pub/2827/