Convergence problem: Difference between revisions

From formulasearchengine
Jump to navigation Jump to search
en>Brad7777
References: removed catgeory mathematical analysis
 
en>Xnn
remove opinion
Line 1: Line 1:
Alyson is what my spouse enjoys to contact me but I don't like when individuals use my full title. My wife and I live in Mississippi and I adore each day residing here. My working day occupation is  are psychics real ([http://galab-work.cs.pusan.ac.kr/Sol09B/?document_srl=1489804 galab-work.cs.pusan.ac.kr]) a journey agent. I am truly fond of to go to karaoke but I've been taking on new things lately.<br><br>Also visit my web-site :: telephone [https://www.machlitim.org.il/subdomain/megila/end/node/12300 psychic phone] ([http://www.aseandate.com/index.php?m=member_profile&p=profile&id=13352970 Privacy of Data: This tool is built-with and functions-in Client Side JavaScripting, so only your computer will see or process your data input/output.a cool way to improve])
The following is a list of [[second moment of area|area moments of inertia]]. The area moment of inertia or [[second moment of area]] has a [[physical unit|unit]] of dimension length<sup>4</sup>, and should not be confused with the [[mass moment of inertia]]. If the piece is thin, however, the mass moment of inertia equals the area density times the area moment of inertia. Each is with respect to a horizontal axis through the [[centroid]] of the given shape, unless otherwise specified.
 
==Area moments of inertia==
 
{|class="wikitable"
|-
! Description || Figure || Area moment of inertia || Comment || Reference
|-
| a filled circular area of radius ''r''||[[Image:Area moment of inertia of a circle.svg]]||<math>I_0 = \frac{\pi}{4} r^4</math>|| ||<ref>{{cite web|url=http://www.efunda.com/math/areas/Circle.cfm|title=Circle|accessdate=2006-12-30|publisher=eFunda}}</ref>
|-
| an [[annulus (mathematics)|annulus]] of inner radius''r''<sub>1</sub> and outer radius''r''<sub>2</sub>||[[Image:Area moment of inertia of a circular area.svg]]||<math>I_0 = \frac{\pi}{4} \left({r_2}^4-{r_1}^4\right)</math>|| For thin tubes, this is approximately equal to: <math>\pi \left(\frac{{r_2}+{r_1}}{2}\right)^3 \left({r_2}-{r_1}\right)</math>  or <math>\pi {r}^3{t}</math> .||
|-
| a filled [[circular sector]] of angle ''θ'' in [[radian]]s and radius ''r'' with respect to an axis through the centroid of the sector and the center of the circle||[[Image:Area moment of inertia of a circular sector.svg]]||<math>I_0 = \left( \theta -\sin \theta \right) \frac{r^{4}}{8}</math>||This formula is valid for only for 0 ≤ <math>\theta</math> ≤ <math>\pi</math> ||
|-
| a filled semicircle with radius ''r'' with respect to a horizontal line passing through the centroid of the area||[[Image:Area moment of inertia of a semicircle 2.svg]]||<math>I_0 = \left(\frac{\pi}{8} - \frac{8}{9\pi}\right)r^4 \approx 0.1098r^4 </math>|| ||<ref name=semicircle>{{cite web|url=http://www.efunda.com/math/areas/CircleHalf.cfm|title=Circular Half|accessdate=2006-12-30|publisher=eFunda}}</ref>
|-
| a filled semicircle as above but with respect to an axis collinear with the base||[[Image:Area moment of inertia of a semicircle.svg]]||<math>I = \frac{\pi r^4}{8}</math>||This is a consequence of the [[parallel axis theorem]] and the fact that the distance between these two axes is <math>\frac{4r}{3\pi}</math>||<ref name=semicircle />
|-
| a filled semicircle as above but with respect to a vertical axis through the centroid||<center>[[Image:Area moment of inertia of a semicircle 3.svg]]</center>||<math>I_0 = \frac{\pi r^4}{8}</math>|| ||<ref name=semicircle />
|-
| a filled quarter circle with radius ''r'' entirely in the 1st quadrant of the [[Cartesian coordinate system]]||[[Image:Area moment of inertia of a quartercircle.svg]]||<math>I = \frac{\pi r^4}{16}</math>|| ||<ref name=quartercircle>{{cite web|url=http://www.efunda.com/math/areas/CircleQuarter.cfm|title=Quarter Circle|accessdate=2006-12-30|publisher=eFunda}}</ref>
|-
| a filled quarter circle as above but with respect to a horizontal or vertical axis through the centroid||[[Image:Area moment of inertia of a quartercircle 2.svg]]||<math>I_0 = \left(\frac{\pi}{16}-\frac{4}{9\pi}\right)r^4</math>||This is a consequence of the [[parallel axis theorem]] and the fact that the distance between these two axes is <math>\frac{4r}{3\pi}</math> ||<ref name=quartercircle />
|-
| a filled [[ellipse]] whose radius along the ''x''-axis is ''a'' and whose radius along the ''y''-axis is ''b''||[[Image:Area moment of inertia of an ellipsis.svg]]</td><td><math>I_0 = \frac{\pi}{4} ab^3</math>|| ||
|-
| a filled rectangular area with a base width of ''b'' and height ''h''||[[Image:Area moment of inertia of a rectangle.svg]]||<math>I_0 = \frac{bh^3}{12}</math>|| ||<ref name=rect>{{cite web|url=http://www.efunda.com/math/areas/rectangle.cfm|title=Rectangular area|accessdate=2006-12-30|publisher=eFunda}}</ref>
|-
| a filled rectangular area as above but with respect to an axis collinear with the base||[[Image:Area moment of inertia of a rectangle 2.svg]]||<math>I = \frac{bh^3}{3}</math>||This is a result from the [[parallel axis theorem]]||<ref name=rect />
|-
| a filled rectangular area as above but with respect to an axis collinear, where ''r'' is the perpendicular distance from the centroid of the rectangle to the axis of interest|| ||<math>I = \frac{bh^3}{12}+bhr^2</math>||This is a result from the [[parallel axis theorem]]||<ref name=rect />
|-
| a filled triangular area with a base width of ''b'' and height ''h'' with respect to an axis through the centroid||[[Image:Area moment of inertia of a triangle.svg]]||<math>I_0 = \frac{bh^3}{36}</math>|| ||<ref name=tri>{{cite web|url=http://www.efunda.com/math/areas/triangle.cfm|title=Triangular area|accessdate=2006-12-30|publisher=eFunda}}</ref>
|-
| a filled triangular area as above but with respect to an axis collinear with the base||[[Image:Area moment of inertia of a triangle 2.svg]]||<math>I = \frac{bh^3}{12}</math>||This is a consequence of the [[parallel axis theorem]] ||<ref name=tri />
|-
| a filled [[regular hexagon]] with a side length of ''a''||[[Image:Area moment of inertia of a regular hexagon.svg]]||<math>I_0 = \frac{5\sqrt{3}}{16}a^4</math>||The result is valid for both a horizontal and a vertical axis through the centroid, and therefore is also valid for an axis with arbitrary direction that passes through the origin.||
|
|-
| Any plane region with a known area moment of inertia for a parallel axis. (Main Article [[parallel axis theorem]]) ||[[Image:Parallel Axes Compact.png]]||<math>I_z = I_x + Ar^2</math> || This can be used to determine the second moment of area of a rigid body about any axis, given the body's moment of inertia about a parallel axis through the object's center of mass and the perpendicular distance (r) between the axes.
|}
 
==See also==
 
* [[List of moments of inertia]]
 
==References==
{{reflist}}
 
==External links==
* [http://www.amesweb.info/SectionalPropertiesTabs/SectionalProperties.aspx Online Sectional Properties Calculator]
* [http://civilengineer.webinfolist.com/str/micalc.htm Online Calculator for Area Moment of Inertia ]
[[Category:Mechanics|Area moment of inertia]]
[[Category:Physics-related lists|Area moments of inertia]]

Revision as of 18:07, 12 March 2013

The following is a list of area moments of inertia. The area moment of inertia or second moment of area has a unit of dimension length4, and should not be confused with the mass moment of inertia. If the piece is thin, however, the mass moment of inertia equals the area density times the area moment of inertia. Each is with respect to a horizontal axis through the centroid of the given shape, unless otherwise specified.

Area moments of inertia

Description Figure Area moment of inertia Comment Reference
a filled circular area of radius r File:Area moment of inertia of a circle.svg I0=π4r4 [1]
an annulus of inner radiusr1 and outer radiusr2 File:Area moment of inertia of a circular area.svg I0=π4(r24r14) For thin tubes, this is approximately equal to: π(r2+r12)3(r2r1) or πr3t .
a filled circular sector of angle θ in radians and radius r with respect to an axis through the centroid of the sector and the center of the circle File:Area moment of inertia of a circular sector.svg I0=(θsinθ)r48 This formula is valid for only for 0 ≤ θπ
a filled semicircle with radius r with respect to a horizontal line passing through the centroid of the area File:Area moment of inertia of a semicircle 2.svg I0=(π889π)r40.1098r4 [2]
a filled semicircle as above but with respect to an axis collinear with the base File:Area moment of inertia of a semicircle.svg I=πr48 This is a consequence of the parallel axis theorem and the fact that the distance between these two axes is 4r3π [2]
a filled semicircle as above but with respect to a vertical axis through the centroid
File:Area moment of inertia of a semicircle 3.svg
I0=πr48 [2]
a filled quarter circle with radius r entirely in the 1st quadrant of the Cartesian coordinate system File:Area moment of inertia of a quartercircle.svg I=πr416 [3]
a filled quarter circle as above but with respect to a horizontal or vertical axis through the centroid File:Area moment of inertia of a quartercircle 2.svg I0=(π1649π)r4 This is a consequence of the parallel axis theorem and the fact that the distance between these two axes is 4r3π [3]
a filled ellipse whose radius along the x-axis is a and whose radius along the y-axis is b File:Area moment of inertia of an ellipsis.svgI0=π4ab3
a filled rectangular area with a base width of b and height h File:Area moment of inertia of a rectangle.svg I0=bh312 [4]
a filled rectangular area as above but with respect to an axis collinear with the base File:Area moment of inertia of a rectangle 2.svg I=bh33 This is a result from the parallel axis theorem [4]
a filled rectangular area as above but with respect to an axis collinear, where r is the perpendicular distance from the centroid of the rectangle to the axis of interest I=bh312+bhr2 This is a result from the parallel axis theorem [4]
a filled triangular area with a base width of b and height h with respect to an axis through the centroid File:Area moment of inertia of a triangle.svg I0=bh336 [5]
a filled triangular area as above but with respect to an axis collinear with the base File:Area moment of inertia of a triangle 2.svg I=bh312 This is a consequence of the parallel axis theorem [5]
a filled regular hexagon with a side length of a File:Area moment of inertia of a regular hexagon.svg I0=5316a4 The result is valid for both a horizontal and a vertical axis through the centroid, and therefore is also valid for an axis with arbitrary direction that passes through the origin.
Any plane region with a known area moment of inertia for a parallel axis. (Main Article parallel axis theorem) File:Parallel Axes Compact.png Iz=Ix+Ar2 This can be used to determine the second moment of area of a rigid body about any axis, given the body's moment of inertia about a parallel axis through the object's center of mass and the perpendicular distance (r) between the axes.

See also

References

43 year old Petroleum Engineer Harry from Deep River, usually spends time with hobbies and interests like renting movies, property developers in singapore new condominium and vehicle racing. Constantly enjoys going to destinations like Camino Real de Tierra Adentro.