OpenLLM-France/wikimedia huggingface dataset:
# PlanetPhysics/Test OCR

The operation $v/c$ is bilinear, and it is easy to verify that $(7.2)==\quad \delta v/c=v/\partial c+(-1)^{\mathfrak {i}}\delta (v/c).$ \quad Assume now that $v$ is an equivariant cochain; for ow $\epsilon \pi$ we have $\alpha c=\alpha \Sigma n_{J}e_{f}=\Sigma (\alpha n_{j})(\alpha e_{j})$, then $(v/\alpha c)\cdot \sigma =\Sigma (\alpha n_{j})v\cdot (\alpha e_{f})\otimes \sigma =\Sigma (\alpha n_{j})\alpha v\cdot (e_{j}\otimes \sigma )$ $=\alpha ^{2}\Sigma n_{j}v\cdot (e_{f}\otimes \sigma )=(v/c)\cdot \sigma .$ Thus, in this case,
\noindent (7.3) $v/\alpha c=v/c$ and $v/(\alpha c-c)=0$.
\noindent Consequently, the definition of $v/c$ extends to the case of $v$, an equi- variant cochain, and $c$ an element of $[C_{i}(W;Z_{m}^{\langle q)})]_{\pi }\approx C_{i}(Z_{m}^{(q)}\otimes _{\pi }W)$;the relation (7.2) holds for this extended operation.
\quad Now take $v=\emptyset ^{\#}u^{n}$ and $c\epsilon C_{i}(Z_{m}^{1q)}\otimes _{\pi }W)$, then $\phi \#u^{n}fc\epsilon C^{nq-i}(K;Z_{m})$ is defined as the reduction by $c$ of the $n^{\mathrm {t} \mathrm {h} }$ power of $u$. Suppose that $u$ is a cocycle, then $\phi \#u^{n}$ is an equivariant cocycle, and if $c$ is a cycle, it follows from (7.2) that $\phi \#u^{n}/c$ is a cocycle. Moreover, if the cycle $c$ is varied by a boundary, then (7.2) implies that $\phi \#u^{n}/c$ varies by a co- boundary. If $u$ is varied by a coboundary $\phi \#u^{n}/c$ also varies by a coboundary. We only remark here that the proof of this last fact requires a special argument and is not, as in the preceding case, an immediate consequence of (7.2). Thus the class $\{\phi \#u^{n}/c\}$ is a function of the classes $\{u\},\{c\}$, and it is independent of the particular $\phi _{\#}$, since by (3.1) any two choices of $\phi _{\#}$ are equivariantly homotopic. Then Steenrod defines $\{u\}^{n}/\{c\}$, the reduction by $\{c\}$ of the $n^{\mathrm {t} \mathrm {h} }$ power of $\{u\}$, by $\{u\}^{n}/\{c\}=\{\phi \#u^{n}/c\}.$ This gives the Steenrod reduced power operations; they are operations defined for $u\epsilon H^{q}(K;Z_{m})$ and $c\epsilon H_{i}(\pi ;Z_{m}^{\langle q)})$, and the value is $u^{n}/c\epsilon H^{nq-i}(K;Z_{m}).$ \quad In general, the reduced powers $u^{n}/c$ are linear operations in $c$, but may not be linear in $u$. We will list some of their $\mathrm {p} \mathrm {r} \mathrm {o} \varphi$ rties. Unless otherwise stated, we assume $u$ and $c$ as above.
\quad First, we have
(7.4) $u^{n}/c=0$ if $i>nq-q$.
\quad Let $f:K\rightarrow L$ be a map and $f^{*}:H^{q}(L;Z_{m})\rightarrow H^{q}(K;Z_{m})$, the induced homomorphism; then $(7.5)==\quad f^{*}(u^{n}/c)=(f^{*}u)^{n}/c.$ This result implies topological invariance for reduced powers
OCR based on this tiff scan
# PlanetPhysics/Theoretical Programs in Quantum Gravity

There are several distinct research programs aimed at developing the mathematical foundations of quantum gravity theories. These include, but are not limited to, the following.

### Mathematical Programs being Developed in Quantum Gravity

* The twistors program applied to an open curved space-time (see refs.
), (which is presumably a globally hyperbolic, relativistic space-time). This may also include the idea of developing a `sheaf cohomology' for twistors (see ref. ) but still needs to justify the assumption in this approach of a charged, fundamental fermion of spin-3/2 of undefined mass and unitary `homogeneity' (which has not been observed so far);
* The supergravity theory program, which is consistent with supersymmetry and superalgebra, and utilizes graded Lie algebras and \emph{matter-coupled
superfields} in the presence of weak gravitational fields;
* The no boundary (closed), continuous space-time programme (ref.
) in quantum cosmology, concerned with singularities, such as black and `white' holes; S. W. Hawking combines, joins, or glues an initially flat Euclidean metric with convex Lorentzian metrics in the expanding, and then contracting, space-times with a very small value of Einstein's cosmological `constant'. Such Hawking, double-pear shaped, space-times also have an initial Weyl tensor value close to zero and, ultimately, a largely fluctuating Weyl tensor during the `final crunch' of our Universe, presumed to determine the irreversible arrow of time; furthermore, an observer will always be able to access through measurements only a limited part of the global space-times in our universe;
* The TQFT/ approach that aims at finding the topological invariants of a
manifold embedded in an abstract vector space related to the statistical mechanics problem of defining extensions of the partition function for many-particle quantum systems;
* The string and superstring theories/M-theory that `live' in higher dimensional
spaces (e.g., $n\geq 6$, preferred $n-dim=11$), and can be considered to be topological representations of physical entities that vibrate, are quantized, interact, and that might also be able to predict fundamental masses relevant to quantum particles;
* The `categorification' and groupoidification programs that aims to deal with quantum field and QG problems at the abstract level of categories and functors in what seems to be mostly a global approach;
* The `monoidal category' and valuation approach initiated by Isham to the quantum measurement problem and its possible solution through local-to-global, finite constructions in small categories.
# PlanetPhysics/Test OCR2

necessary to consider the second bundle. The curvature form of our connection is a tensorial quadratic differential form in $M$, of type $ad(G^{\prime })$ and with values in the Lie Algebra $L(O^{\prime })$ of $G^{\prime }$. Since the Lie algebra $L(O)$ of $G$ is a subalgebra of $L(G^{\prime })$, there is a natural projection of $L(O^{\prime })$ into the quotient space $L(G^{\prime })/L(G)$. The image of the cur- vature form under this proiection will be called the torsion form or the torsion tensor. If the forms $\pi ^{\rho }$ in (13) define a $G$-connection, the vanishing of the torsion form is expressed analytically by the con- ditions $(22)==\quad c_{f^{\prime \prime }k^{\prime \prime }}^{i^{\prime \prime }}=0.$ \quad We proceed to derive the analytical formulas for the theory of a $G$-connection without torsion in the tangent bundle. In general we will consider such formulas in $B_{G}$. The fact that the O-connection has no torsion simplifies (13) into the form $(23)==\quad d\omega ^{i}=\Sigma _{\rho ,k}a_{\rho k}^{i}\pi ^{\rho }\wedge \omega ^{k}.$ By taking the exterior derivative of (23) and using (18), we get $(24)==\quad \Sigma _{\rho ,k}a_{\rho k}^{i}\Pi \rho _{\mathrm {A} \omega ^{k}=0_{;}}$ where we put $(25)==\quad \Pi \rho =d\pi ^{\rho }+\#\Sigma _{\sigma .\tau }\gamma _{\sigma \tau }^{\rho }\pi ^{\sigma }\mathrm {A} \pi ^{\tau }.$ For a fixed value of $k$ we multiply the above equation by $\omega ^{1}==A.=..=A==\omega ^{k-1}==A==\omega ^{k+1_{\Lambda }}\ldots ==A==\omega ^{n},$ getting $\sum _{\rho }a_{\rho k^{\prod \rho }}^{i}==A==\omega ^{1}==A.=..=A==\omega ^{n}=0,$ or $\Sigma _{\rho }a_{\rho k^{\Pi \rho }}^{l}\equiv 0,\ \mathrm {m} \mathrm {o} \mathrm {d} \ \omega ^{;}$.
\noindent Since the infinitesimal transformations $X_{\rho }$ are linearly independent, this implies that $\Pi \rho \equiv 0,==\mathrm {m} \mathrm {o} \mathrm {d} \ \omega ^{j}.$ It followo that II $\rho$ is of the form $IA==\rho _{=\Sigma _{j}\phi _{J^{\mathrm {A} \omega ^{f}}}^{\rho }}$ where $\phi _{j}^{\rho }$ are Pfaffian forms. Substituting these expressions into (24), we get $\Sigma _{\rho ,j,k(a_{\rho k}^{i}\phi _{j}^{\rho }-a_{\rho j}^{i}\phi _{k}^{\rho })\mathrm {A} \omega ^{j}\mathrm {A} \omega ^{k}=0}.$ It follows that $\Sigma _{\rho }(a_{\rho k}^{i}\phi _{f}^{\rho }-a_{\rho j}^{1}\phi _{k}^{\rho })\equiv 0,==\mathrm {m} \mathrm {o} \mathrm {d} \ \omega ^{\prime }.$ Since $G$ has the property $(C)$, the above equations imply that $\phi _{f}^{\rho }\equiv 0,==\mathrm {m} \mathrm {o} \mathrm {d} \ \omega ^{k}.$
OCR based on this tiff scan
# PlanetPhysics/Theorem of the Addition of Velocities Employed In

\subsection{The Theorem of the Addition of Velocities Employed in Classical Mechanics} From Relativity: The Special and General Theory by Albert Einstein
Let us suppose our old friend the railway carriage to be travelling along the rails with a constant velocity $v$, and that a man traverses the length of the carriage in the direction of travel with a velocity $w$. How quickly or, in other words, with what velocity $W$ does the man advance relative to the embankment during the process? The only possible answer seems to result from the following consideration: If the man were to stand still for a second, he would advance relative to the embankment through a distance $v$ equal numerically to the velocity of the carriage. As a consequence of his walking, however, he traverses an additional distance $w$ relative to the carriage, and hence also relative to the embankment, in this second, the distance w being numerically equal to the velocity with which he is walking. Thus in total be covers the distance $W=v+w$ relative to the embankment in the second considered. We shall see later that this result, which expresses the theorem of the addition of velocities employed in classical mechanics, cannot be maintained; in other words, the law that we have just written down does not hold in reality. For the time being, however, we shall assume its correctness.
# PlanetPhysics/Theorem on CW Complex Approximation of Quantum State Spaces in QAT

\htmladdnormallink{theorem {http://planetphysics.us/encyclopedia/Formula.html} 1.}
Let $[QF_{j}]_{j=1,...,n}$ be a complete sequence of commuting quantum spin `foams' (QSFs) in an arbitrary quantum state space (QSS), and let $(QF_{j},QSS_{j})$ be the corresponding sequence of pair subspaces of QST. If $Z_{j}$ is a sequence of CW-complexes such that for any $j$ , $QF_{j}\subset Z_{j}$, then there exists a sequence of $n$-connected models $(QF_{j},Z_{j})$ of $(QF_{j},QSS_{j})$ and a sequence of induced isomorphisms ${f_{*}}^{j}:\pi _{i}(Z_{j})\rightarrow \pi _{i}(QSS_{j})$ for $i>n$, together with a sequence of induced monomorphisms for $i=n$.
There exist weak homotopy equivalences between each $Z_{j}$ and $QSS_{j}$ spaces in such a sequence. Therefore, there exists a $CW$--complex approximation of QSS defined by the sequence $[Z_{j}]_{j=1,...,n}$ of CW-complexes with dimension $n\geq 2$. This $CW$--approximation is unique up to regular homotopy equivalence.
Corollary 2.
The $n$-connected models $(QF_{j},Z_{j})$ of $(QF_{j},QSS_{j})$ form the Model category of Quantum Spin Foams $(QF_{j})$, whose \htmladdnormallink{morphisms {http://planetphysics.us/encyclopedia/TrivialGroupoid.html} are maps $h_{jk}:Z_{j}\rightarrow Z_{k}$ such that $h_{jk}\mid QF_{j}=g:(QSS_{j},QF_{j})\rightarrow (QSS_{k},QF_{k})$, and also such that the following diagram is commutative:} \\
</math> \begin{CD} Z_j @> f_j >> QSS_j \\ @V h_{jk} VV @VV g V \\ Z_k @ > f_k >> QSS_k \end{CD} Failed to parse (syntax error): {\displaystyle \\ ''Furthermore, the maps <math>h_{jk'' } are unique up to the homotopy rel $QF_{j}$ , and also rel $QF_{k}$}.
{Theorem 1} complements other data presented in the parent entry on QAT.
# PlanetPhysics/Theory of Heat Radiation

The Theory of Heat Radiation is an attempt to make the translated work of Max Planck availabe on PlanetPhysics. The sections are derivatives from the public domain work in [1].
{\subsection Part 1: Fundamental Facts and Definitions}
{\mathbf Chapter I:} General Introduction \\ {\mathbf Chapter II:} Radiation at Thermodynamic Equilibrium. Kirchoff's Law. Black Radiation

### The Theory of Heat Radiation Part 2

Deductions from Electrodynamics and Thermodynamics

### The Theory of Heat Radiation Part 3

Entropy and Probability

### The Theory of Heat Radiation Part 4

A system of Oscillators in a Stationary field of radiation

### The Theory of Heat Radiation Part 5

Irreversible Radiation Processes
# Virginia Native Tree Leaf Identification Project/Black Locust

Robinia pseudoacacia
* Tree location: Near a pile of bushes--bit far from my house
* Tree type: Deciduous
* Leaf: Pinnate
* Leaf margin: Smooth-edged
* Leaf arrangement: Alternate
* Habitat: Variety of sites--grows best on moist loams with limestone origin.
* Virginia Range: Mostly the western side of Virginia
* Fruit: 2-4 inch, flat, brownish pods having 4-8 kidney shaped smooth red seeds--ripening in fall.
# Virginia Native Tree Leaf Identification Project/Pin Oak

Quercus palustris
* Tree location: In a bush near my house
* Tree type: Deciduous
* Leaf: Simple
* Leaf margin: Lobed
* Leaf arrangement: Alternate
* Habitat: Clay soils
* Fruit: 1/2 inch brown rounded striped acorn
# Virginia Native Tree Leaf Identification Project/Slippery Elm

Ulmus rubra (Slippery Elm)
* Tree location: A bit far from my house
* Tree type: Deciduous
* Leaf: Simple
* Leaf margin: Serrated
* Leaf arrangement on branch: Alternate
* Habitat: Best on moist, rich bottomlands--but also found on drier, upland soils
* Virginia Range: All over Virginia
* Fruit: Small seed secured by a papery, wafer-like covering; 3/4 - 1 inch across; smooth; ripening in spring.
# Virginia Native Tree Leaf Identification Project/White Oak

Quercus alba
* Location: Near my house.
* Tree Type: Deciduous
* Leaf: Simple
* Leaf margin: Lobed
* Leaf arrangement on branch: Alternate
* Habitat: Varies, but best grown on well-drained and loamy soil
* Virginia Range: All over Virginia
* Fruit: Egg-shaped to oval-shaped acorn, 3/4 inches long--Light chestnut brown.
# Virginia Native Tree Leaf Identification Project/Allegheny Chinkapin

Castanea pumila
* Leaves found in a small tree in my front yard
* Tree type: deciduous
* Leaf: simple
* Leaf margin: toothed
* Leaf arrangement on branch: Alternate
* Habitat: Understory of [most commonly: drier soils] of upland hardwood forests.
* The tree is found all over Virginia
* Fruit; 1-1 1/2 inches long--shiny, dark brown, sweet nut.
# Virginia Native Tree Leaf Identification Project/Eastern Redbud

Cercis canadensis
* Location: Right in front of my yard
* Type: Deciduous
* Leaf: Simple
* Margin: Smooth/Smooth edged
* Arrangement: Alternate
* Habitat: Understory of moist forests
* Fruit: Red, Brown, Flattened, Oblong, 2-4 inches
* Virginia Range: Nearly entire state except for the extreme southeastern part of Virginia.
# Virginia Native Tree Leaf Identification Project/Eastern Redcedar

Juniperus virginiana
* Location: Near the fence of my house.
* Tree type: Evergreen
* Leaf: Simple
* Leaf Margin: Entire
* Arrangement: Spiral
* Habitat: Varies--from wetlands to dry, rocky ridges.
* Virginia Range: Entire state
* Fruit: Black, Blue fruit--1/8 inch in diameter
# Virginia Native Tree Leaf Identification Project/Allegheny Chinkapin/Workspace

* Tree where leaf is from
* Sideways view of the leaf
* [Majority] opposite leaves displayed
* Edited out picture of "LeafOnTree2018.jpg"
* Half between Opposite leaves and Alternative leaves: More pictures needed
* Edited out picture of "LeafOnTree22018.jpg"

## Information

Source: http://www.dof.virginia.gov/infopubs/Native-Tree-ID-spreads_2016_pub.pdf
Work: Virginia Native Tree Leaf Identification Project/Allegheny Chinkapin/Introduction
Leaf Types #1: https://scioly.org/wiki/index.php/Forestry/Leaf_Types
Pinnately vs. Palmetly: Here
---EDIT BEFORE HERE IF MISTAKE: https://en.wikiversity.org/w/index.php?title=Virginia_Native_Tree_Leaf_Identification_Project/1st_page&diff=1745161&oldid=1745160---

### Steps to Identification
#### 1

a. Leaves are needle or scale-like, go to 2. b. Leaves are broad and flat, go to 14.

#### 14

a. Leaves opposite, go to 15. b. Leaves alternate, go to 25.

#### 25

a. Leaves compound, go to 26. b. Leaves simple, go to 36.

#### 36

a. Leaves have lobes with or without teeth, or large rounded teeth appearing like a wavy margin, go to 37'. b. Leaves do not have lobes or margins as above, and may or may not be toothed or spined, go to 53.

#### 53

a. The leaf margin is toothed or spiny; teeth may be widely spaced or very tiny, go to 54. b. The leaf margin is not toothed or spiny, go to 74.

#### 54

a. The leaf has more teeth than veins, or has widely spaced sharp spines, go to 55. b. The leaf has one tooth at the end of each vein, go to 63.

#### 63

a. Leaf less than 3 times long as wide, bark smooth and gray, brown buds up to 1 inch long, like pointed cigars – American Beech pg. 50. b. Leaf length at least 3 times its width, teeth turned toward tip of leaf, go to 64.

#### 64

a. Top and bottom of leaf smooth and hairless. One or two stems, generally not over 4 inches in diameter – American Chestnut pg. 51. b. Bottom of leaf hairy, one nut per husk. Large shrub or small tree, often multistemmed and forming thickets – Alleghany Chinkapin pg. 52.
# BCP/Hemerocallis fulva/Logs

This page contains recent bloom logs for Hemerocallis fulva (Ditch Lily). If you saw this plant blooming today (or sometime within the last 3 days), you can help improve the bloom clock by logging it. Just click on "edit" next to the Recent Logs heading, add *~~~~ (an asterisk followed by four tildes) on a new line just below the last signature, and then click "save page". This will add your signature and the date to log the plant.
Please make sure you've signed up on the contributors' page so that we can know the location of the plant you saw blooming and use your contribution to create a flora for your region! When you're done, you can go back to one of the main pages and find logs of other flowers you might have seen today.

### Logs
#### 2008 Logs

* (no archived logs yet)

##### Recent Logs

* --SB_Johnny | 11:37, 4 July 2007 (UTC)
* --SB_Johnny | 09:12, 28 June 2008 (UTC)
* --Clarinetguy097 (discuss • contribs) 20:19, 16 June 2018 (UTC)
* --Clarinetguy097 (discuss • contribs) 23:32, 24 June 2018 (UTC)
* --Clarinetguy097 (discuss • contribs) 02:56, 24 June 2019 (UTC)
* --Clarinetguy097 (discuss • contribs) 17:36, 2 July 2019 (UTC)
# BCP/Heuchera americana

Heuchera americana
| Inflorescence Wikipedia • Commons • Wikibooks (horticulture) • Wikibooks (subject) • Wikispecies • Fruit and seed clock | Profile for Heuchera americana (Alumroot) Identifying Characteristics Recent Logs SB Johnny-LM 11:17, 7 July 2007 (UTC) SB Johnny-LM 10:46, 25 July 2007 (UTC) SBJ 08:30, 25 August 2007 (UTC) SB Johnny-LM 09:23, 8 September 2007 (UTC) --SB_Johnny | 11:04, 29 June 2008 (UTC) SB Johnny-LM 09:52, 20 July 2008 (UTC) (view all logs) |
Global data:
Regional data: Southeastern Pennsylvania: (cultivated) June, July, August, September
Additional images:
# BCP/Heuchera americana/Logs

This page contains recent bloom logs for Heuchera americana (Alumroot). If you saw this plant blooming today (or sometime within the last 3 days), you can help improve the bloom clock by logging it. Just click on "edit" next to the Recent Logs heading, add *~~~~ (an asterisk followed by four tildes) on a new line just below the last signature, and then click "save page". This will add your signature and the date to log the plant.
Please make sure you've signed up on the contributors' page so that we can know the location of the plant you saw blooming and use your contribution to create a flora for your region! When you're done, you can go back to one of the main pages and find logs of other flowers you might have seen today.

### Logs
#### 2008 Logs

* (no archived logs yet)

##### Recent Logs

* SB Johnny-LM 11:17, 7 July 2007 (UTC)
* SB Johnny-LM 10:46, 25 July 2007 (UTC)
* SBJ 08:30, 25 August 2007 (UTC)
* SB Johnny-LM 09:23, 8 September 2007 (UTC)
* --SB_Johnny | 11:04, 29 June 2008 (UTC)
* SB Johnny-LM 09:52, 20 July 2008 (UTC)
# BCP/Hepatica nobilis/Logs

This page contains recent bloom logs for the plant Hepatica nobilis (Anemone hepatica). If you saw this plant blooming today (or sometime within the last 3 days), you can help improve the bloom clock by logging it. Just click on "edit" next to the Recent Logs heading, add *~~~~ (an asterisk followed by four tildes) on a new line just below the last signature, and then click "save page". This will add your signature and the date to log the plant.
Please make sure you've signed up on the contributors' page so that we can know the location of the plant you saw blooming and use your contribution to create a flora for your region! When you're done, you can go back to one of the main pages and find logs of other flowers you might have seen today.

##### Recent Logs

* --Juan Karlstein 19:59, 22 April 2008 (UTC)

##### Archived Logs

(If there are more than 5 signatures under the recent logs heading, move the oldest logs to under this heading (generally leave the 3 most recent).
# BCP/Hesperis matronalis

Hesperis matronalis
| Closeup of purple flowers, flowers can range from white through pink, purple, or red Wikipedia • Commons • Wikibooks (horticulture) • Wikibooks (subject) • Wikispecies • Fruit and seed clock | Profile for Hesperis matronalis (Dame's Rocket) Identifying Characteristics Habit:Upright forbFlowers:4 showy petalsScent:Strong, sweet scent in early morning and evening Recent Logs Jomegat 04:13, 5 June 2009 (UTC) Jomegat 00:19, 15 July 2009 (UTC) (view all logs) |
Global data: Temperate zone season(s): Late Spring, Early Summer, Late Summer, Mid Fall
Regional data: Southeastern Pennsylvania: (invasive or naturalized) (cultivated) May, June, September, November New Hampshire: June, July
Additional images:
# BCP/Hesperis matronalis/Logs

This page contains recent bloom logs for Hesperis matronalis (Dame's Rocket). If you saw this plant blooming today (or sometime within the last 3 days), you can help improve the bloom clock by logging it. Just click on "edit" next to the Recent Logs heading, add *~~~~ (an asterisk followed by four tildes) on a new line just below the last signature, and then click "save page". This will add your signature and the date to log the plant.
Please make sure you've signed up on the contributors' page so that we can know the location of the plant you saw blooming and use your contribution to create a flora for your region! When you're done, you can go back to one of the main pages and find logs of other flowers you might have seen today.

### Logs
#### 2007 Logs

* --SB_Johnny | 14:06, 21 May 2007 (UTC)
* SBJ 00:32, 23 May 2007 (UTC)
* --SB_Johnny | 17:27, 23 May 2007 (UTC)
* SBJ 09:18, 25 May 2007 (UTC)
* --SB_Johnny | 10:21, 26 May 2007 (UTC)
* --SB_Johnny | 23:49, 31 May 2007 (UTC)
* --SB_Johnny | 10:47, 3 June 2007 (UTC)
* SBJ 16:16, 7 June 2007 (UTC)
* --SB_Johnny | 15:33, 9 June 2007 (UTC)
* --SB_Johnny | 14:00, 17 September 2007 (UTC) (sporadic, but on several plants)
* --SB_Johnny | 14:12, 16 November 2007 (UTC) (sporadic still, but blooming)

#### 2008 Logs

* --SB_Johnny | 00:20, 7 May 2008 (UTC)
* --SB_Johnny | 10:13, 17 May 2008 (UTC)
* --SB_Johnny | 09:56, 27 May 2008 (UTC)
* --SB_Johnny | 10:49, 4 June 2008 (UTC)

##### Recent Logs

* Jomegat 04:13, 5 June 2009 (UTC)
* Jomegat 00:19, 15 July 2009 (UTC)
# BCP/Heuchera sanguinea

Heuchera sanguinea
| Search for Heuchera sanguinea on commons) Wikipedia • Commons • Wikibooks (horticulture) • Wikibooks (subject) • Wikispecies • Fruit and seed clock | Profile for Heuchera sanguinea (Coral Bells) Identifying Characteristics Recent Logs SB Johnny-LM 15:11, 9 May 2008 (UTC) (view all logs) |
Global data: Temperate zone season(s): Late Spring
Regional data: Southeastern Pennsylvania: (cultivated) May
Additional images:
# BCP/Hemerocallis fulva

Hemerocallis fulva
| Flower Wikipedia • Commons • Wikibooks (horticulture) • Wikibooks (subject) • Wikispecies • Fruit and seed clock | Profile for Hemerocallis fulva (Ditch Lily) Identifying Characteristics Recent Logs --SB_Johnny | 11:37, 4 July 2007 (UTC) --SB_Johnny | 09:12, 28 June 2008 (UTC) --Clarinetguy097 (discuss • contribs) 20:19, 16 June 2018 (UTC) --Clarinetguy097 (discuss • contribs) 23:32, 24 June 2018 (UTC) --Clarinetguy097 (discuss • contribs) 02:56, 24 June 2019 (UTC) --Clarinetguy097 (discuss • contribs) 17:36, 2 July 2019 (UTC) (view all logs) |
Global data:
Regional data: Southeastern Pennsylvania: (invasive or naturalized) June, July
Additional images: