text:
MDOT Assigns the Cutest Names Ever to Its 299 Snowplows
George McIntyre
George McIntyre Published: January 12, 2022
The days of snowplows having boring names like 'Maintenance Vehicle #MDOT-148' are over. Today, all of Michigan's approximately 300 plow trucks have been given fun (and creative) names which you can view on the Michigan Department of Transportation's website.
Last year, MDOT debuted the contest, inviting residents across the state to submit their name suggestions. All in all, 15,400 name suggestions were submitted and MDOT employees were tasked with sifting through the entries to find the best ones.
What Are Some of The Best Names?
Some of the winning suggestions have real local or regional appeal, like 'Detroit SnoWings' which pays tribute to Michigan's beloved hockey team. Good old Michigan Rock and Roll is honored with 'Kid Rock Salt,' a name assigned to a plow in the Metro Detroit region.
Beloved actress Betty White has been immortalized on a Michigan plow truck that now bears the name 'Betty Whiteout.'
There's even one for the tech enthusiasts, as 'Ctrl Salt Delete' is now assigned to a truck in the Southwest region of the state.
Keep reading for a complete list of the names by region below.
Why Are Michigan Snowplows Being Given Fun Names?
Nick Schirripa helped coordinate the project for MDOT. He tells the Detroit Free Press that it's a way of honoring the snowplow drivers who are the unsung heroes working tirelessly during Michigan's brutal winters.
"It is a lot of fun," he said. "But one of the biggest drivers internally for me was that this is a great way to humanize a group of folks in our agency who really don't get enough attention, and who really go unnoticed, and are often taken for granted. And that's our snowplow drivers, our maintenance workers, who I believe, and a lot of us believe, are absolute rock stars, they are superheroes."
While names won't be painted on each individual truck, the new names will be visible on MDOT's website which shows the location of each truck while they're out working.
Michigan's 299 Snowplows Get the Cutest Names Ever
The Michigan Department of Transportation has revealed the winning names assigned to each of its snowplows throughout the state.
Here they are, sorted by region.
These Are the 10 Best Colleges and Universities in Michigan
Picking a college is a huge decision whether you're going right out of high school or looking to increase your earning potential as a working adult.
Niche compiled the data, taking many factors into account from more than 1,000 top colleges and universities throughout the United States.
These are the highest-ranking schools here Michigan.
Take a Look Inside the Most Expensive Home on the Market in Genesee County to Start 2022
Maybe 2022 means a new house for you, and we have the perfect pick! Starting the new year, this home right on Lake Fenton is the priciest piece of property in Genesee County. A total of 7132+ sq. ft., there are 5 bedrooms, 4 full and 2 half baths, 6 plus car garages, and a view to die for. The place is perfect for a big family, maybe with the in-laws spending extra time since it boasts 2 separate living spaces with private entrances. The master suite has a custom closet Carrie Bradshaw would be impressed with. There's a theatre room, exercise room, and so much more. Take a little look inside!
Filed Under: MDOT, snowplows


text:
Yve-Alain Bois (born April 16, 1952) is a professor of Art History at the School of Historical Studies at the Institute for Advanced Study in Princeton, New Jersey.

Education
Bois received an M.A. from the École Pratique des Hautes Études in 1973 for his work on El Lissitzky's typography, and a Ph.D. from the École des Hautes Études en Sciences Sociales in 1977 for his work on Lissitzky's and Malevich's conceptions of space.  Both of his degrees were supervised under Roland Barthes.

Career

Academic
Bois is a professor at the School of Historical Studies at the Institute for Advanced Study in Princeton, New Jersey, in the chair inaugurated by Erwin Panofsky, and at the European Graduate School. From 1991 to 2005, he served on the faculty at Harvard University as Joseph Pulitzer Jr. Professor in Modern Art, after teaching at Johns Hopkins University and at the Centre National de la Recherche Scientifique.

Bois was elected to the American Philosophical Society in 2016.

Writing
Bois has written books and articles on artists of European modernism. He is an editor of the journal October.

Articles
"Whose Formalism?" Art Bulletin, Mar. 1996 European Graduate School
Review of Tony Smith retrospective at the Museum of Modern Art, New York, Artforum, Nov. 1998
Review of "Supports/Surfaces" exhibition at the Galerie Nationale du Jeu de Paume, Artforum, Dec. 1998
Bois and Linda Nochlin discuss the Matisse and Picasso exhibition, Artforum, Feb. 1999
Review of Barnett Newman retrospective, Philadelphia Museum of Art, Artforum, Mar. 2002
"The Mourning After," panel discussion on painting, Artforum, Mar. 2003
On Fred Sandback, Artforum, Oct. 2003

References

External links
Bois faculty page at European Graduate School
Interview with Bois for Folha de Sao Paulo, Caderno Mais!, 2005
MIT Press: list of books and articles by Bois
All About Yve: An Interview with Yve-Alain Bois (1995)
"From Art to Barthes and Back Again", The Harvard Crimson, September 19, 1991

1952 births
Living people
People from Constantine, Algeria
Algerian art critics
Algerian art historians
Institute for Advanced Study faculty
Harvard University faculty
Johns Hopkins University faculty
Academic staff of European Graduate School
21st-century Algerian people

redpajama_set_name: RedPajamaWikipedia


text:
#include "ScintillaSyntax.h"
#include "3rdparty/scintilla/include/SciLexer.h"
#include "3rdparty/scintilla/include/qt/ScintillaEdit.h"
#include "Code/QRDUtils.h"

static const char *python_keywords =
    "False None True and as assert break class continue def del elif else except finally for from "
    "global if import in is lambda nonlocal not or pass raise return try while with yield";

static const char *hlsl_keywords[2] = {
    // keyword set 0:
    // Secondary keywords and identifiers
    R"EOKEYWORDS(
defined

register packoffset static const

break continue discard do for if else switch while case default return true false

abort abs acos all AllMemoryBarrier AllMemoryBarrierWithGroupSync any asdouble asfloat asin asint
asuint atan atan2 ceil clamp clip cos cosh countbits cross D3DCOLORtoUBYTE4 ddx ddx_coarse ddx_fine
ddy ddy_coarse ddy_fine degrees determinant DeviceMemoryBarrier DeviceMemoryBarrierWithGroupSync
distance dot dst errorf EvaluateAttributeAtCentroid EvaluateAttributeAtSample
EvaluateAttributeSnapped exp exp2 f16tof32 f32tof16 faceforward firstbithigh firstbitlow floor fma
fmod frac frexp fwidth GetRenderTargetSampleCount GetRenderTargetSamplePosition GroupMemoryBarrier
GroupMemoryBarrierWithGroupSync InterlockedAdd InterlockedAnd InterlockedCompareExchange
InterlockedCompareStore InterlockedExchange InterlockedMax InterlockedMin InterlockedOr
InterlockedXor isfinite isinf isnan ldexp length lerp lit log log10 log2 mad max min modf msad4 mul
noise normalize pow printf Process2DQuadTessFactorsAvg Process2DQuadTessFactorsMax
Process2DQuadTessFactorsMin ProcessIsolineTessFactors ProcessQuadTessFactorsAvg
ProcessQuadTessFactorsMax ProcessQuadTessFactorsMin ProcessTriTessFactorsAvg
ProcessTriTessFactorsMax ProcessTriTessFactorsMin radians rcp reflect refract reversebits round
rsqrt saturate sign sin sincos sinh smoothstep sqrt step tan tanh tex1D tex1Dbias tex1Dgrad tex1Dlod
tex1Dproj tex2D tex2Dbias tex2Dgrad tex2Dlod tex2Dproj tex3D tex3Dbias tex3Dgrad tex3Dlod tex3Dproj
texCUBE texCUBEbias texCUBEgrad texCUBElod texCUBEproj transpose trunc

BINORMAL BINORMAL0 BINORMAL1 BINORMAL2 BINORMAL3 BINORMAL4 BINORMAL5 BINORMAL6 BINORMAL7
BLENDINDICES BLENDINDICES0 BLENDINDICES1 BLENDINDICES2 BLENDINDICES3 BLENDINDICES4 BLENDINDICES5
BLENDINDICES6 BLENDINDICES7 BLENDWEIGHT BLENDWEIGHT0 BLENDWEIGHT1 BLENDWEIGHT2 BLENDWEIGHT3
BLENDWEIGHT4 BLENDWEIGHT5 BLENDWEIGHT6 BLENDWEIGHT7 COLOR COLOR0 COLOR1 COLOR2 COLOR3 COLOR4 COLOR5
COLOR6 COLOR7 NORMAL NORMAL0 NORMAL1 NORMAL2 NORMAL3 NORMAL4 NORMAL5 NORMAL6 NORMAL7 POSITION
POSITION0 POSITION1 POSITION2 POSITION3 POSITION4 POSITION5 POSITION6 POSITION7 POSITIONT PSIZE
PSIZE0 PSIZE1 PSIZE2 PSIZE3 PSIZE4 PSIZE5 PSIZE6 PSIZE7 TANGENT TANGENT0 TANGENT1 TANGENT2 TANGENT3
TANGENT4 TANGENT5 TANGENT6 TANGENT7 TEXCOORD TEXCOORD0 TEXCOORD1 TEXCOORD2 TEXCOORD3 TEXCOORD4
TEXCOORD5 TEXCOORD6 TEXCOORD7 TEXCOORD8 TEXCOORD9 TEXCOORD0 TEXCOORD1 TEXCOORD2 TEXCOORD3 TEXCOORD4
TEXCOORD5 TEXCOORD6 TEXCOORD7 TEXCOORD8 TEXCOORD9

SV_Coverage SV_Depth SV_DispatchThreadID SV_DomainLocation SV_GroupID SV_GroupIndex SV_GroupThreadID
SV_GSInstanceID SV_InsideTessFactor SV_IsFrontFace SV_OutputControlPointID SV_POSITION SV_Position
SV_RenderTargetArrayIndex SV_SampleIndex SV_TessFactor SV_ViewportArrayIndex SV_InstanceID
SV_PrimitiveID SV_VertexID SV_TargetID SV_TARGET SV_Target SV_Target0 SV_Target1 SV_Target2
SV_Target3 SV_Target4 SV_Target5 SV_Target6 SV_Target7 SV_ClipDistance0 SV_ClipDistance1
SV_ClipDistance2 SV_ClipDistance3 SV_ClipDistance4 SV_ClipDistance5 SV_ClipDistance6
SV_ClipDistance7 SV_CullDistance0 SV_CullDistance1 SV_CullDistance2 SV_CullDistance3
SV_CullDistance4 SV_CullDistance5 SV_CullDistance6 SV_CullDistance7
)EOKEYWORDS",

    // keyword set 1:
    // Secondary keywords and identifiers
    R"EOKEYWORDS(
bool bool1 bool2 bool3 bool4 bool1x1 bool1x2 bool1x3 bool1x4 bool2x1 bool2x2 bool2x3 bool2x4 bool3x1
bool3x2 bool3x3 bool3x4 bool4x1 bool4x2 bool4x3 bool4x4

int int1 int2 int3 int4 int1x1 int1x2 int1x3 int1x4 int2x1 int2x2 int2x3 int2x4 int3x1 int3x2 int3x3
int3x4 int4x1 int4x2 int4x3 int4x4

uint uint1 uint2 uint3 uint4 uint1x1 uint1x2 uint1x3 uint1x4 uint2x1 uint2x2 uint2x3 uint2x4 uint3x1
uint3x2 uint3x3 uint3x4 uint4x1 uint4x2 uint4x3 uint4x4

UINT UINT2 UINT3 UINT4

dword dword1 dword2 dword3 dword4 dword1x1 dword1x2 dword1x3 dword1x4 dword2x1 dword2x2 dword2x3
dword2x4 dword3x1 dword3x2 dword3x3 dword3x4 dword4x1 dword4x2 dword4x3 dword4x4

half half1 half2 half3 half4 half1x1 half1x2 half1x3 half1x4 half2x1 half2x2 half2x3 half2x4 half3x1
half3x2 half3x3 half3x4 half4x1 half4x2 half4x3 half4x4

float float1 float2 float3 float4 float1x1 float1x2 float1x3 float1x4 float2x1 float2x2 float2x3
float2x4 float3x1 float3x2 float3x3 float3x4 float4x1 float4x2 float4x3 float4x4

double double1 double2 double3 double4 double1x1 double1x2 double1x3 double1x4 double2x1 double2x2
double2x3 double2x4 double3x1 double3x2 double3x3 double3x4 double4x1 double4x2 double4x3 double4x4

snorm unorm string void cbuffer struct

Buffer AppendStructuredBfufer ByteAddressBuffer ConsumeStructuredBuffer StructuredBuffer RWBuffer
RWByteAddressBuffer RWStructuredBuffer RWTexture1D RWTexture1DArray RWTexture2D RWTexture2DArray
RWTexture3D

InputPatch OutputPatch

linear centroid nointerpolation noperspective sample

sampler sampler1D sampler2D sampler3D samplerCUBE SamplerComparisonState SamplerState sampler_state
AddressU AddressV AddressW BorderColor Filter MaxAnisotropy MaxLOD MinLOD MipLODBias ComparisonFunc
ComparisonFilter

texture Texture1D Texture1DArray Texture2D Texture2DArray Texture2DMS Texture2DMSArray Texture3D
TextureCube
)EOKEYWORDS"};

static const char *glsl_keywords[2] = {
    // keyword set 0:
    // Secondary keywords and identifiers
    R"EOKEYWORDS(
defined

in out inout static const

break continue do for while switch case default if else true false discard return

radians degrees sin cos tan asin acos atan sinh cosh tanh asinh acosh atanh pow exp log exp2 log2
sqrt inversesqrt abs sign floor trunc round roundEven ceil fract mod modf min max clamp mix step
smoothstep isnan isinf floatBitsToInt floatBitsToUint intBitsToFloat uintBitsToFloat fma frexp ldexp

packUnorm2x16 packSnorm2x16 packUnorm4x8 packSnorm4x8 unpackUnorm2x16 unpackSnorm2x16 unpackUnorm4x8
unpackSnorm4x8 packDouble2x32 unpackDouble2x32 packHalf2x16 unpackHalf2x16 length distance dot cross
normalize faceforward reflect refract matrixCompMult outerProduct transpose determinant inverse
lessThan lessThanEqual greaterThan greaterThanEqual equal notEqual any all not uaddCarry usubBorrow
umulExtended imulExtended bitfieldExtract bitfieldInsert bitfieldReverse bitCount findLSB findMSB

textureSize textureQueryLod textureQueryLevels textureSamples texture textureProj textureLod
textureOffset texelFetch texelFetchOffset textureProjOffset textureLodOffset textureProjLod
textureProjLodOffset textureGrad textureGradOffset textureProjGrad textureProjGradOffset
textureGather textureGatherOffset textureGatherOffsets

atomicCounterIncrement atomicCounterDecrement atomicCounter atomicAdd atomicMin atomicMax atomicAnd
atomicOr atomicXor atomicExchange atomicCompSwap

imageSize imageSamples imageLoad imageStore imageAtomicAdd imageAtomicMin imageAtomicMax
imageAtomicAnd imageAtomicOr imageAtomicXor imageAtomicExchange imageAtomicCompSwap

dFdx dFdy dFdxFine dFdyFine dFdxCoarse dFdyCoarse fwidth fwidthFine fwidthCoarse
interpolateAtCentroid interpolateAtSample interpolateAtOffset EmitStreamVertex EndStreamPrimitive
EmitVertex EndPrimitive barrier memoryBarrier memoryBarrierAtomicCounter memoryBarrierBuffer
memoryBarrierShared memoryBarrierImage groupMemoryBarrier

gl_CullDistance gl_FragCoord gl_FragDepth gl_FrontFacing gl_GlobalInvocationID gl_HelperInvocation
gl_in gl_InstanceID gl_InvocationID gl_Layer gl_LocalInvocationID gl_LocalInvocationIndex
gl_MaxPatchVertices gl_NumWorkGroups gl_out gl_PatchVerticesIn gl_PerVertex gl_PointCoord
gl_PointSize gl_Position gl_PrimitiveID gl_PrimitiveIDIn gl_SampleID gl_SampleMask gl_SampleMaskIn
gl_SamplePosition gl_TessCoord gl_TessLevelInner gl_TessLevelOuter gl_VertexID gl_ViewportIndex
gl_WorkGroupID gl_WorkGroupSize

gl_MaxComputeWorkGroupCount gl_MaxComputeWorkGroupSize gl_MaxComputeUniformComponents
gl_MaxComputeTextureImageUnits gl_MaxComputeImageUniforms gl_MaxComputeAtomicCounters
gl_MaxComputeAtomicCounterBuffers gl_MaxVertexAttribs gl_MaxVertexUniformComponents
gl_MaxVaryingComponents gl_MaxVertexOutputComponents gl_MaxGeometryInputComponents
gl_MaxGeometryOutputComponents gl_MaxFragmentInputComponents gl_MaxVertexTextureImageUnits
gl_MaxCombinedTextureImageUnits gl_MaxTextureImageUnits gl_MaxImageUnits
gl_MaxCombinedImageUnitsAndFragmentOutputs gl_MaxCombinedShaderOutputResources gl_MaxImageSamples
gl_MaxVertexImageUniforms gl_MaxTessControlImageUniforms gl_MaxTessEvaluationImageUniforms
gl_MaxGeometryImageUniforms gl_MaxFragmentImageUniforms gl_MaxCombinedImageUniforms
gl_MaxFragmentUniformComponents gl_MaxDrawBuffers gl_MaxClipDistances
gl_MaxGeometryTextureImageUnits gl_MaxGeometryOutputVertices gl_MaxGeometryTotalOutputComponents
gl_MaxGeometryUniformComponents gl_MaxGeometryVaryingComponents gl_MaxTessControlInputComponents
gl_MaxTessControlOutputComponents gl_MaxTessControlTextureImageUnits
gl_MaxTessControlUniformComponents gl_MaxTessControlTotalOutputComponents
gl_MaxTessEvaluationInputComponents gl_MaxTessEvaluationOutputComponents
gl_MaxTessEvaluationTextureImageUnits gl_MaxTessEvaluationUniformComponents
gl_MaxTessPatchComponents gl_MaxPatchVertices gl_MaxTessGenLevel gl_MaxViewports
gl_MaxVertexUniformVectors gl_MaxFragmentUniformVectors gl_MaxVaryingVectors
gl_MaxVertexAtomicCounters gl_MaxTessControlAtomicCounters gl_MaxTessEvaluationAtomicCounters
gl_MaxGeometryAtomicCounters gl_MaxFragmentAtomicCounters gl_MaxCombinedAtomicCounters
gl_MaxAtomicCounterBindings gl_MaxVertexAtomicCounterBuffers gl_MaxTessControlAtomicCounterBuffers
gl_MaxTessEvaluationAtomicCounterBuffers gl_MaxGeometryAtomicCounterBuffers
gl_MaxFragmentAtomicCounterBuffers gl_MaxCombinedAtomicCounterBuffers gl_MaxAtomicCounterBufferSize
gl_MinProgramTexelOffset gl_MaxProgramTexelOffset gl_MaxTransformFeedbackBuffers
gl_MaxTransformFeedbackInterleavedComponents gl_MaxCullDistances gl_MaxCombinedClipAndCullDistances
gl_MaxSamples gl_MaxVertexImageUniforms gl_MaxFragmentImageUniforms gl_MaxComputeImageUniforms
gl_MaxCombinedImageUniforms gl_MaxCombinedShaderOutputResources gl_DepthRangeParameters
gl_DepthRange gl_NumSamples
)EOKEYWORDS",

    // keyword set 1:
    // Secondary keywords and identifiers
    R"EOKEYWORDS(
float double int void bool

mat2 mat3 mat4 dmat2 dmat3 dmat4 mat2x2 mat2x3 mat2x4 dmat2x2 dmat2x3 dmat2x4 mat3x2 mat3x3 mat3x4
dmat3x2 dmat3x3 dmat3x4 mat4x2 mat4x3 mat4x4 dmat4x2 dmat4x3 dmat4x4 vec2 vec3 vec4 ivec2 ivec3
ivec4 bvec2 bvec3 bvec4 dvec2 dvec3 dvec4 uint uvec2 uvec3 uvec4

atomic_uint patch sample buffer subroutine struct

invariant precise layout

lowp mediump highp precision attribute uniform varying shared coherent volatile restrict readonly
writeonly centroid flat smooth noperspective

sampler1D sampler2D sampler3D samplerCube sampler1DShadow sampler2DShadow samplerCubeShadow
sampler1DArray sampler2DArray sampler1DArrayShadow sampler2DArrayShadow isampler1D isampler2D
isampler3D isamplerCube isampler1DArray isampler2DArray usampler1D usampler2D usampler3D
usamplerCube usampler1DArray usampler2DArray sampler2DRect sampler2DRectShadow isampler2DRect
usampler2DRect samplerBuffer isamplerBuffer usamplerBuffer sampler2DMS isampler2DMS usampler2DMS
sampler2DMSArray isampler2DMSArray usampler2DMSArray samplerCubeArray samplerCubeArrayShadow
isamplerCubeArray usamplerCubeArray

image1D iimage1D uimage1D image2D iimage2D uimage2D image3D iimage3D uimage3D image2DRect
iimage2DRect uimage2DRect imageCube iimageCube uimageCube imageBuffer iimageBuffer uimageBuffer
image1DArray iimage1DArray uimage1DArray image2DArray iimage2DArray uimage2DArray imageCubeArray
iimageCubeArray uimageCubeArray image2DMS iimage2DMS uimage2DMS image2DMSArray iimage2DMSArray
uimage2DMSArray
)EOKEYWORDS"};

void ConfigureSyntax(ScintillaEdit *scintilla, int language)
{
  bool hlsl = false;
  bool glsl = false;

  if(language == SCLEX_HLSL)
  {
    hlsl = true;
    language = SCLEX_CPP;
  }

  if(language == SCLEX_GLSL)
  {
    glsl = true;
    language = SCLEX_CPP;
  }

  scintilla->setLexer(language);
  scintilla->styleSetSize(STYLE_DEFAULT, 10);

#define SC_COL(qcol) SCINTILLA_COLOUR(qcol.red(), qcol.green(), qcol.blue())

  // set the default style to base/text
  QColor base = scintilla->palette().color(QPalette::Base);
  QColor text = scintilla->palette().color(QPalette::Text);
  scintilla->styleSetBack(STYLE_DEFAULT, SC_COL(base));
  scintilla->styleSetFore(STYLE_DEFAULT, SC_COL(text));

  scintilla->setCaretFore(SC_COL(text));

  // default all lexer styles up to STYLE_DEFAULT as the same, then override per-colour below
  for(sptr_t i = 0; i < STYLE_DEFAULT; i++)
  {
    scintilla->styleSetBack(i, SC_COL(base));
    scintilla->styleSetFore(i, SC_COL(text));
  }

  // set highlight text colour
  QColor highlight = scintilla->palette().color(QPalette::Highlight);
  QColor highlightedText = scintilla->palette().color(QPalette::HighlightedText);
  scintilla->setSelBack(true, SC_COL(highlight));
  scintilla->setSelFore(true, SC_COL(highlightedText));

  // set margin colours
  QColor window = scintilla->palette().color(QPalette::Window);
  QColor windowText = scintilla->palette().color(QPalette::WindowText);
  for(sptr_t i = 0; i < 5; i++)
    scintilla->setMarginBackN(i, SC_COL(window));
  scintilla->styleSetBack(STYLE_LINENUMBER, SC_COL(window));
  scintilla->styleSetFore(STYLE_LINENUMBER, SC_COL(windowText));

  sptr_t blue = IsDarkTheme() ? SCINTILLA_COLOUR(105, 105, 255) : SCINTILLA_COLOUR(0, 0, 150);
  sptr_t magenta = IsDarkTheme() ? SCINTILLA_COLOUR(255, 105, 255) : SCINTILLA_COLOUR(150, 0, 150);
  sptr_t rouge = IsDarkTheme() ? SCINTILLA_COLOUR(255, 150, 150) : SCINTILLA_COLOUR(175, 70, 70);

  // works for either dark or light
  sptr_t green = SCINTILLA_COLOUR(0, 150, 0);
  sptr_t teal = SCINTILLA_COLOUR(0, 150, 150);
  sptr_t olive = SCINTILLA_COLOUR(150, 150, 0);

  if(language == SCLEX_CPP)
  {
    scintilla->setProperty("lexer.cpp.track.preprocessor", "0");
    scintilla->setProperty("styling.within.preprocessor", "1");

    scintilla->styleSetFore(SCE_C_COMMENT, green);
    scintilla->styleSetFore(SCE_C_COMMENTDOC, green);
    scintilla->styleSetFore(SCE_C_COMMENTLINE, green);
    scintilla->styleSetFore(SCE_C_WORD, blue);
    scintilla->styleSetFore(SCE_C_WORD2, blue);
    scintilla->styleSetFore(SCE_C_PREPROCESSOR, blue);
    scintilla->styleSetBold(SCE_C_PREPROCESSOR, true);

    if(hlsl)
    {
      scintilla->setKeyWords(0, hlsl_keywords[0]);
      scintilla->setKeyWords(1, hlsl_keywords[1]);
    }
    else if(glsl)
    {
      scintilla->setKeyWords(0, glsl_keywords[0]);
      scintilla->setKeyWords(1, glsl_keywords[1]);
    }
  }
  else if(language == SCLEX_PYTHON)
  {
    scintilla->setProperty("tab.timmy.whinge.level", "1");
    scintilla->setProperty("fold", "1");

    scintilla->setKeyWords(0, python_keywords);

    scintilla->styleSetFore(SCE_P_COMMENTLINE, green);
    scintilla->styleSetFore(SCE_P_COMMENTBLOCK, green);
    scintilla->styleSetFore(SCE_P_NUMBER, teal);
    scintilla->styleSetFore(SCE_P_STRING, magenta);
    scintilla->styleSetFore(SCE_P_TRIPLE, rouge);
    scintilla->styleSetFore(SCE_P_TRIPLEDOUBLE, rouge);
    scintilla->styleSetFore(SCE_P_CHARACTER, magenta);
    scintilla->styleSetFore(SCE_P_DEFNAME, olive);
    scintilla->styleSetFore(SCE_P_CLASSNAME, magenta);
    scintilla->styleSetFore(SCE_P_WORD, blue);
    scintilla->styleSetFore(SCE_P_WORD2, blue);
    scintilla->styleSetBold(SCE_P_WORD, true);
    scintilla->styleSetBold(SCE_P_WORD2, true);
  }
}

redpajama_set_name: RedPajamaGithub


text:
Quantum Numbers | Article about Quantum Numbers by The Free Dictionary
https://encyclopedia2.thefreedictionary.com/Quantum+Numbers
Also found in: Dictionary.
Related to Quantum Numbers: Electron configuration
The quantities, usually discrete with integer or half-integer values, which are needed to characterize a physical system of one or more atomic or subatomic particles. Specification of the set of quantum numbers serves to define such a system or, in other words, to label the possible states the system may have. In general, quantum numbers are obtained from conserved quantities determinable by performing symmetry transformations consisting of arbitrary variations of the system which leave the system unchanged. For example, since the behavior of a set of particles should be independent of the location of the origin in space and time (that is, the symmetry operation is translation in space-time), it follows that momentum and energy are rigorously conserved. See Symmetry laws (physics)
In general, each physical system must be studied individually to find the symmetry transformations, and thus the conserved quantities and possible quantum numbers. The quantum numbers themselves, that is, the actual state labels, are usually the eigenvalues of the physical operators corresponding to the conserved quantities for the system in question. See Eigenvalue (quantum mechanics), Elementary particle, Parity (quantum mechanics)
It is not necessary that the conserved quantity be "quantized" in order to be regarded as a quantum number; for example, a free particle possesses energy and momentum, both of which can have values from a continuum but which are used to specify the state of the particle.
integers (0, 1, 2, … ) or half-integers (1/2, 3/2, 5/2, …) that define the possible discrete values of the physical quantities characterizing quantum systems (atomic nucleus, atom, molecule) and individual elementary particles. The use of quantum numbers in quantum mechanics reflects features of the discreteness of processes occurring in the mi-croworld, and is closely connected with the existence of the quantum of action, or the Planck constant ℏ. Quantum numbers were first introduced in physics to describe the empirically determined regularities of atomic spectra, but the meaning of quantum numbers and the associated discreteness of certain quantities characterizing the dynamics of microparticles were revealed only by quantum mechanics.
A set of quantum numbers that thoroughly defines the state of a quantum system is said to be complete. The aggregate of the states that satisfy all possible values of the quantum numbers of a complete set forms the complete system of states. The state of an electron in the atom is determined by four quantum numbers corresponding to the four degrees of freedom of the electron (three degrees of freedom are connected with the three coordinates that define the electron's spatial position, and the fourth, internal, degree of freedom is connected with its spin). For the hydrogen atom and hydrogen-like atoms these quantum numbers forming a complete set are given below.
(1)The principal quantum number n = 1, 2, 3, … defines the energy levels of the electron.
(2)The azimuthal (or orbital) quantum number l = 0, 1, 2, …, n – 1 gives the spectrum of the possible values of the square of the orbital angular momentum of an electron: M2i = ℏ2l(l + 1).
(3)The magnetic quantum number ml characterizes the possible values of a projection Mlz of the orbital angular momentum Ml on some arbitrarily selected direction (taken as the z-axis): Mlz =ℏml. This number may assume integer values in the interval from –l to +l (for a total of 2l + 1 values).
(4)The magnetic spin quantum number, or simply the spin quantum number, ms characterizes the possible values of a projection of the electron's spin and may assume two values: ms = ±1/2.
Definition of a state of an electron using the quantum numbers n, l, ml, and ms does not take into account the so-called fine structure of energy levels—the splitting of levels with a given n (when n ≥ 2) as a result of the spin's influence on the orbital motion of the electron. When this interaction is taken into account, the quantum numbers j and mj are used to characterize the state of the electron instead of ml and ms.
(5)The quantum number j of the total angular momentum M of an electron (the orbital moment + the spin moment) determines the possible values of the square of the total momentum: M2 = ℏ2j(j + 1) and, for a given l, may assume two values: j = l ± 1/2.
(6)The magnetic quantum number mj of the total angular momentum determines the possible values of the projection of the total angular momentum on the z-axis, Mz = ℏmj, it may assume 2j + 1 values: mj = -j, -j + 1, …, +j.
The same quantum numbers approximately describe the states of individual electrons in complex (multielectron) atoms as well as the state of the individual nucleons—protons and neutrons— in atomic nuclei. In this case, n represents the successive (in order of increasing energy) energy levels with a given l. The state of a multielectron atom as a whole is defined by the following quantum numbers: (1) the quantum number of the total orbital angular momentum of an atom L, which is defined by the motion of all electrons, L = 0, 1, 2, … ; (2) the quantum number of the total angular momentum of the atom j, which may assume all values differing by units of 1 from J = | L — S | to J = L + S, where S is the the total spin of the atom (in ℏ units); and (3) the magnetic quantum number mj, which defines the possible values of a projection of the atom's total angular momentum on the z-axis, Mz = mjℏ, and which assumes 2J + 1 values.
Still another quantum number—the parity of the state P —is used to characterize the state of the atom and of the quantum System in general. It assumes the values +1 or −1 depending on whether the wave function defining the state of the system retains its sign on inversion of the coordinates r with respect to the origin of coordinates (that is, when r —?> — r is replaced) or changes its sign. The parity Pis equal to (-1)l for the hydrogen atom and (—1)L for multielectron atoms.
Quantum numbers also have proved convenient for formulating the selection rules that determine the possible types of quantum transitions.
A number of other quantum numbers are introduced in the physics of elementary particles and nuclear physics. The quantum numbers of elementary particles are internal characteristics of the particles that define their interactions and the regularities of mutual transformations. In addition to the spin s, which may be an integer or half-integer (in ℏ units), the following includes quantum numbers of elementary particles: (1) the electric charge Q, which in all known elementary particles is equal either to 0 or to a positive or negative integer (in units of the elementary electric charge e); (2) the baryon charge B, which is equal to 0 or 1 (for antiparticles, 0 or — 1); (3) lepton charges, or lepton numbers—the electric number Le and the muons —which are equal to 0 or +1 (for antiparticles, 0 or —1);(4) the isotopic spin T, which is an integer or half-integer; (5) the strangeness S or the hypercharge Y (which is related to S by the equation Y = S + B) —all known elementary particles (or antiparticles) have S=0 or ±1, ±2, ±3; and (6) the intrinsic parity II, a quantum number that characterizes the properties of the symmetry of elementary particles with respect to inversion of the coordinates and may be equal to +1 (such particles are called particles of even parity) or —1 (particles of odd parity). These quantum numbers also are applied to systems consisting of several elementary particles and, in particular, to atomic nuclei. Here, the total values of the electric, baryon, and lepton charges and of the strangeness of a system of particles are equal to the algebraic sum of the corresponding quantum numbers of the individual particles; the total spin and isotopic spin are obtained on the basis of the quantum rules for the addition of angular momentums; and the intrinsic parities of the particles are multiplied.
Physical quantities defining the motion of a quantum mechanical particle (or system) that are conserved in the process of motion but that do not necessarily belong to the discrete spectrum of possible values are often said to be quantum numbers in the broad sense. For example, the energy of a free-moving electron (which has a continuous spectrum of values) may be considered as one of its quantum numbers.
D. V. GAL'TSOV
Quantum Numbers
anomalous series
Atomic Nucleus
Atomic structure and spectra
atomic-beam resonance
azimuthal quantum number
Balmer continuum
Balmer formula
Balmer lines
baryon number
Birge-Sponer extrapolation
chemical bond
correspondence principle
diffuse series
* [S.sub.2] = [[(e-, [v.sup.0.sub.e], [N.sup.0]) [producto cruzado] e+].sub.L] with quantum numbers (1, 3*, -1/3) and (1, 1, 1) respectively.
Nuevos modelos 3-3-1 universales
In 1913, Bohr introduced the Principal Quantum Number to explain the Rydberg Formula for the spectral emission lines of atomic hydrogen.
Helical Solenoid Model of the Electron
In accordance with current standard notation in spectral analysis, here we use exclusively symbols J for rotational quantum number and v for vibrational quantum number, regardless of the symbols employed in the original sources.
[(J + 1/2).sup.2] OR J(J + 1) AS FUNCTIONAL FOR ROTATIONAL TERMS IN ANALYSIS OF MOLECULAR SPECTRA
In Figure 3, we show as example the potential curves for the case [gamma] = 0.5, [R.sub.b] = 6[a.sup.*.sub.0], [R.sub.t] = 4[a.sup.*.sub.0] for which quantum numbers m = 4,5,6,7, 8,9 satisfy conditions (8).
One-Electron Conical Nanotube in External Electric and Magnetic Fields
The obtained formula is basic and valid for arbitrary integer and noninteger principal quantum numbers.
Evaluation of Self-Friction Three-Center Nuclear Attraction Integrals with Integer and Noninteger Principal Quantum Numbers n over Slater Type Orbitals
The results obtained in [1-9] data show that in a homogeneous conductive metal conductor structure comprising quantum number n = 1,2,3...
Calculation-experimental method of research in a metallic conductor with the pulse current of electronic wavepackages and de Broglie electronic half-waves
In this notation, M* is the effective mass of the captured charged particle in an orbital state with angular momentum quantum number L.
Strongly localized image states of spherical graphitic particles
Here, we assign the vibrational quantum number n to a diatom if its energy is closest to the one of the n-th state of the corresponding quantum oscillator [28].
Effects of the vibrational motion of [XHY.sup.-] on the post-photo detachment dissociation dynamics of the XHY complex (X, Y = Br, I)
Current suppression in a small magnetic field can ultimately be traced back to the famous Pauli exclusion principle, the quantum mechanical principle that states that no two electrons (fermions) may have identical quantum numbers. Since the electric wires are essentially one-dimensional, the effect of the Pauli exclusion principle is dramatic, comparable to an accident on a single-lane road that brings traffic to a standstill.
Radically Better Smartphones Inspired by Birds
To unambiguously characterize this new particle, detailed studies of its properties (mass, production rates, spin/CP quantum numbers, self-couplings) are needed, while searches for other similar particles are important.
United Kingdom - Study of the ElectroWeak Symmetry Breaking and the Higgs Sector with the ATLAS detector at the LHC
For different quantum numbers, there are specific radii of confinement for which exact solutions are known.
Wide effectiveness of a sine basis for quantum-mechanical problems in d dimensions
Quantum physics is usually considered to be the theory of extremely lightweight objects, such as atoms or photons, or of exceptionally small units, namely very small quantum numbers.
World record for entanglement of twisted light quanta set
Quantum Electronics
Quantum Evolution
Quantum Fluid
Quantum Frequency Standards
Quantum Generator
quantum gravitation
quantum gravity
Quantum Gyroscope
quantum Hall effect
quantum Hall liquid
quantum Hall state
quantum hydrodynamics
quantum hypothesis
quantum limit
Quantum Magnetometer
quantum measurement paradox
Quantum Mechanical Amplifier
quantum mineralogy
quantum nondemolition measurement
quantum number
quantum of action
Quantum Paper
quantum size effects
quantum solid
Quantum solids
quantum state
quantum statistics
quantum theory of heat capacity
quantum theory of light
quantum theory of matter
quantum theory of measurement
quantum theory of radiation
quantum theory of spectra
quantum theory of valence
Quantum Transitions
quantum turbulence
quantum well
quantum well infrared photodetector
quantum well injection transit-time diode
quantum wire
quantum yield
Quantum-dot Cellular Automata
QuantumFilm
Quantum meruit
Quantum Metaphysics Institute
Quantum Metrology Division
Quantum Mini-Reliability Test
Quantum Modeling
Quantum Modulation in Scattering and Tunneling
Quantum Molecular Dynamics
Quantum Monte Carlo
Quantum Monte Carlo Diagonalization
Quantum Monte-Carlo
Quantum Monte-Carlo Renormalization Group
quantum mottle
Quantum multiverse
Quantum Nagic Angle Spinning
Quantum Network Design
Quantum Noiseless Coding Theorem
Quantum Non-Demolition
Quantum nonlocality
Quantum Online
Quantum Opportunities Program
Quantum Optical Coherence Tomography
Quantum Optical Random Walk
Quantum optics
Quantum Optics and Condensed Matter Physics
Quantum Optics and Laser Science
Quantum Optics for Information Technology
Quantum Optics Lab Olomouc
Quantum Owners Club
Quantum particle
Quantum Particle State Analyzer
Quantum Particle Swarm Optimization
Quantum Path Integral Molecular Dynamics
Quantum Percolation Model
Quantum Performance Group, Inc.
Quantum Performance Solutions
Quantum Phase Gate
Quantum phase transition
Quantum Physics Division
quantum placeat
Quantum Placet
Quantum point contact

redpajama_set_name: RedPajamaCommonCrawl


Fort William and Glen Nevis is an important part in the Outdoor Capital of the UK - hardly surprising when you consider the highest mountain in the British Isles towers behind our small Highland town and community. Fort William is a key destination for people wishing to take part or spectate in world class outdoor sporting activities. This area is unique in that almost all major, recognised sports can be enjoyed like diving in our coastal waters to kayaking or sailing on the seas and lochs to climbing many of the highest mountains in the British Isles - and lots of activities in between.
Let us explain this word "Lochaber". Lochaber is the name given to a huge area of the Scottish west Highlands that includes Glencoe, Fort William & Glen Nevis, Ben Nevis, a good part of the Great Glen and much of Glen Spean, the Road to the Isles including Mallaig, the Ardnamurchan peninsula and in the north, the lands of Knodart. Some of the key historical-political moments in the UK occurred in this area.
Check the activity providers on our Outdoor Activities section of this site. We also consider "Outdoor Capital" to describe all the traditional activities like highland games, touring by car, motorcycle or bicycle, simply enjoying our peaceful and quite countryside locations - we have more than most communities in the British Isles !
A great many people work outdoors doing traditional things like fishing and estate working, crofting and forestry.
The Lochaber community is a small one - less than 20,000 people living in an area greater than the whole of Luxembourg. Our community is mostly a rural one with many small villages and communities scattered all over Lochaber. Our economy is potentially fragile and is increasingly dependent on lots of small, family businesses providing all sorts of products and services. Our college - West Highland College UHI, is a fantastic learning resource where locals can study Further Education and even a growing number of Degree courses through the UHI - University of the Highlands and Islands. if you are coming to Fort William and Lochaber, we really hope you enjoy your visit and find everyone you meet friendly and welcoming.


Creamer Makin' Patsy pottery throwing rib makes a 24-36 ounce pitcher, 6" tall by 4-6" wide. Use 2-2.5 pounds of clay.
By using these Wiziwig potter's ribs with distinct profiles, you can easily throw the sets of cups and bowls on the potters wheel that have the same shape. You can modify the width of the pieces as desired but the nice thing is that when you view your finished items they will all have the same height and profile.
Each rib has 2 different sides for two versions of your pots. They also have notches for smoothing the foot and rim of the pieces to clean and comfortable shapes.
Wiziwig profile ribs were created by a potter with an artist's eye so they help you create beautiful and graceful forms just awaiting your finishing touches, glazing, and firing !
1. On a Pottery Wheel, Throw a Cylinder similar to the Dimensions and Weight listed for your Specific WiziWig Rib.
2. With One Hand on the Inside of the Cylinder and the other Holding your WiziWig Rib to the Outside of the Cylinder, Press your Rib into the Cylinder, while Applying Gentle Outward Pressure with your Inside Hand, Forming it to your WiziWig Rib Profile Shape.
3.Gently do this until a Continuous, Smooth line of Clay touches your Rib. Be Sure to Add Water.
4. For a Nice, Rounded Rim, Choose a Rim Size located at the Bottom of your WiziWig Profile Rib and Place Over your Rim with Very Gentle Pressure.
Leave As Is or Add your Own Wiz to Personalize.


text:
Q: Direct way to get the Hyodo-Kato Galois action A group object $G$ in smooth proper rigid spaces has formal semistable model (possibly after a finite extension).
Hyodo-Kato give the cohomology of $G$ a $(\phi, N)$-model structure which by Fontaine-Colmez is the same as a Galois action.
Is there a more direct way to get this action starting from $G$?

redpajama_set_name: RedPajamaStackExchange


But since I'm obviously not in a men's fraternity, I brushed off the thought.
The next day, there was a meeting of the sorority sisters in the dance hall. There must have been about 150 or so of us in the room. Some of the women were yelling a chant that I never learned, and there was a line in the song about how we would show St. Peter our sorority pins and be admitted into heaven. Mind you, that's not an official song of the sorority, but again, it gave me pause. It caused a restlessness in my spirit that I couldn't shake.
So I began to ask Him questions: God, what do You think about sororities and fraternities? Did these organizations exist in biblical times? Would Jesus join a fraternity? Can I imagine Him throwing up the hand signs? What does the Bible say about what I pledged to 21 years ago?
That last question led me to do something that I had not done since…ever! I didn't actually know what all I had pledged to because, as secret societies go, you can't completely know what you're pledging to until you've already pledged. You don't get to read "the books" until you're already in. It's like signing a blank check based on the fact that so many other people you admire signed it blind, too.
To be honest, the night I "went over", I put on my T-shirt, pranced around campus with my new sorority sisters, and rejoiced like crazy. When we finally received our sorority books, I didn't actually sit down and read them. I put them on a shelf. Admired them. Smiled at them. The only time I pulled them out was when I had to go to a ceremony and read a portion of text. Otherwise, I didn't read those books any more than I read every single page of my car insurance policy or my student loan papers. In fact, ALL of the sorority members who have sincerely asked me about my renouncement have admitted to me that they've NEVER read their books completely, either.
Truth be told: When I really started to think about it in 2013, I didn't want to read the books. Not prayerfully. Not with my growing knowledge of the Scriptures. Not with the Holy Spirit's magnifying glass handy. I didn't want to find out anything that would cause me to lose connection with my line sisters, make me have to renounce, make me have to risk people thinking I'm "too deep" spiritually, or even cause people to stop reading my books if they found out I had renounced. And what was I supposed to do with all that paraphernalia?
Despite the fact that I didn't want to re-examine what I had pledged to, there was no way I could quench those burning questions without reading "the books". Even more, I had to question myself: Why am I resisting this? If it's all good, there shouldn't be a problem, right? Why am I trusting all these other admirable Christian women's interpretations rather reading the books for myself?
So I did it. When I returned from my weekend at the yard, I read all three of my little books from cover to cover in one sitting for the very first time ever. The result: I no longer agreed with what I had pledged to.
As I read some of the passages from our intake process again, I remembered how (back in '92) I'd had an uneasy feeling with some of the vows. I remember thinking, "This kind of sounds like a Scripture…but it's…different." Yet, I'd carried on. I wasn't going to abort the process. Back then, I didn't recognize the "uneasy feeling" as the Holy Spirit's check. Secondly, I didn't want the disgrace of having "dropped" the line. People at my small college would look at me crazy from that day forward. Last but not least, I sure wasn't going to waste all the hard-earned money I had spent to pledge. No ma'am!
I didn't understand the power of words.
Needless to say, after reading the books decades later and researching the disturbing history of secret societies, I could no longer remain a member of a Greek letter organization.
I was content to leave quietly, like an uncontested divorce. But in recent months, I've heard the buzz from my younger cousins and nieces about pledging sororities and I'm cringing because I know what they are about to agree to. They can't know because no one within the organization will inform them ahead of time. Like me, my sweet relatives probably see the strong women on campus exemplifying sisterhood, doing good things, and they want to be a part of it. They have no concept of how these organizations are inherently bound to Greek gods.
I can't speak for every fraternity or sorority because, obviously, I haven't read all their books. But I have Googled and found the official lyrics of the anthems of the "Divine Nine" (isn't that something to be questioned right there?) and I can tell you that I wouldn't advise any believer to sing or speak those words. This is why I am compelled to share what I know now.
Thank you so much for reading this post. I welcome any comments/questions. I pray that it will help you make an informed decision about joining, leaving, or staying in a Greek Letter Organization. Please know that I have shared this in Christ's love and a deep concern for His body. He is Lord!
In my next post on this topic, I'll share some of the most frequently asked questions from people who have wanted more information about this decision. I've been hit with some hard questions – everything from "Is it really that serious?" to "Why are you trying to break up the black community?" to "You think you're holier than my Pastor, who is a proud member of…?" I'll share my answers to those questions and more.
If you'd like to ask something, please feel free to comment, inbox, or email me! Be blessed!
*Note: While I was only privy to one sorority's information, I think it's important that every believer in any sorority/fraternity/secret society read their books entirely!


text:
Q: Is there any 3D modelling app in AS2 / AS3? I could not find any online app in flash that you can use to create models similar to http://www.3dtin.com/
I know that with 3d library Papervision3D you can do a lot, but to build an app 100% alone seems to be overwhelming.
It would be sufficient to have a tool to create simple shapes (cuboid, cone, pyramid). And the option to export it as PNG image.
Any advice appreciated!

A: For simple objects, i've have great success using ERain's Swift 3D.
http://www.erain.com/


Personal and professional protection for personal trainers and instructors of individual or group exercise programs such as Pilates, yoga, martial arts and more.
Questions? Call us at (800) 844-0536.
NOTE: Fitness Professionals who occupy more than 1,000 square feet or have employees do not qualify for the Individual Fitness Professional Program and must complete an application as a Facility.
Change Request to Add an Additional Insured for Personal Trainer/Yoga/Pilates Instructor Policy (PDF) or complete the online form to request addition of an insured.
Scroll down for a general description of Liability Coverages provided under this program.
You are unique and so are your coverage needs. We offer multiple levels of coverage so that you can be confident that you are protected, without paying for excess coverage that you don't need.
If you teach exclusively group exercise classes, you may be eligible for lower rates. Check out our lower rates for group exercise instructors or call us at 800-844-0536.
If you teach only group exercise classes, you qualify for our Group Exercise Rate.
Note that trainers who work one-on-one with clients are not eligible for this classification and should check out Coverage for Personal Trainers, Yoga and Pilates Instructors.
Please email Olivia Brown, or call us at (800) 844-0536 if you have questions.


Welcome to the Prime Logistics application page.
Must own official version of ETS2 or ATS.
Must be willing to log jobs.
If any bans occured in the previous 3 months, please let us know in your application.
Please make sure you also unhide your TMP bans and make your games on steam public!


text:
Mirwaiz Kashmir listed among world's most influential Muslim politicians
Mirwaiz Umar Farooq has for the seventh consecutive time been chosen among the 500 most influential Muslim personalities across the globe by the Royal Islamic Strategic Studies Centre, Jordan.
Mirwaiz has been listed among the world's 500 most influential Muslims and is categorized in the political group for the seventh consecutive year by RISSC, Jordon.
Pertinently, Mirwaiz continues to be under house arrest for more than 18 months.
On Mirwaiz, RISSC Jordan said, "He has been advocating dialogue with both India and Pakistan so that the aspirations of the Kashmiri people may be realised."
Specifically mentioning Mirwaiz's arrest, it stated that he has been under house arrest since August 2019.
The Royal Islamic Strategic Studies Centre is an independent research entity affiliated with the Royal Aal al-Bayt Institute for Islamic thought, an international Islamic non-governmental, independent institute headquartered in Amman, the capital of Jordan.
Topping the list, personalities include King Salman of Saudi Arabia, Ayatollah Khamenei of Iran, Pakistan Prime Minister Imran Khan and King Abdullah of Jordan. (KNS)
Two JeM militant associates arrested in Bandipora
Tourist arrivals in J&K declined since revocation of special status: Govt tells Parliament
KU postpones MBBS exam scheduled today
Woman dies of suffocation in Kawdara blaze
Gunmen fire shots at residence of political activist in Srinagar
Former J&K Minister Sharief Naiz Passes Away
Inzamam-ul-Haq undergoes angioplasty after suffering heart attack


text:
Emilie Otterdahl (7. november 1882 i København – 20. juni 1971) var en dansk stumfilmsskuespillerinde der spillede med i række stumfilm i perioden 1912 – 1915. Hun forblev ugift, med tog i 1910 sin mors pigenavn.

Filmografi
 1912 – Den flyvende Cirkus (som Erna, Strøms datter, instruktør Alfred Lind)
 1912 – Cirkusluft (som Anna, Löwenhjelms datter, instruktør Poul Welander) (svensk)
 1913 – Bristet Lykke (instruktør August Blom)
 1913 – Atlantis (som fin dame ved bal, instruktør August Blom)
 1913 – Frederik Buch som Dekoratør (instruktør Sofus Wolder)
 1913 – Den gamle Majors Ungdomskærlighed (instruktør Axel Breidahl)
 1913 - Et Mandfolk til Auktion (instruktør Axel Breidahl)
 1913 – En farlig Forbryder (som Edith, instruktør August Blom)
 1913 – Kongens Foged (instruktør Sofus Wolder)
 1913 – Broder mod Broder (instruktør Robert Dinesen)
 1913 – Giftslangen (instruktør Hjalmar Davidsen)
 1913 – Frk. Studenten (som Doris, Ruths søster, instruktør Sofus Wolder)
 1913 – Privatdetektivens Offer (instruktør Sofus Wolder)
 1913 – Fem Kopier (instruktør August Blom)
 1914 – Et Kærlighedsoffer (instruktør Robert Dinesen)
 1914 – Under falsk Flag (instruktør Sofus Wolder)
 1914 – Vasens Hemmelighed (som Marie, stuepige, instruktør August Blom)
 1914 – Fra Mørke til Lys (som Anna, stuepige og Antons kæreste, instruktør Hjalmar Davidsen)
 1914 - Det svage Punkt (instruktør Sofus Wolder)
 1915 – Fattig og rig (som Iris, Lady Dombeys datter, ubekendt instruktør)
 1916 – To Mennesker (som Carmian, blomsterpige, ubekendt instruktør)

 Ormen (instruktør Poul Welander) (svensk)

Eksterne henvisninger

Stumfilmskuespillere fra Danmark


Periodic Table of Elements Pdf – Here you can get all knowledge about periodic table of elements with atomic mass and valency. You can also check our Modern Periodic Table of Elements …... Module Two – Atoms, Molecules and Moles mass units (amu), where 1 amu is defined as 1/12 of the mass of an atom of carbon-12. The atomic mass of carbon-12, therefore, is exactly 12 amu.
It has the highest atomic number and highest atomic mass of all the elements discovered so far. According to the IUPAC, new elements can be named after a mythological concept, a mineral, a place or country, a property or a scientist.... atomic mass.pdf - Free download as PDF File (.pdf), Text File (.txt) or read online for free.
Module Two – Atoms, Molecules and Moles mass units (amu), where 1 amu is defined as 1/12 of the mass of an atom of carbon-12. The atomic mass of carbon-12, therefore, is exactly 12 amu.... Relative isotopic mass: the same quantity as atomic mass, but with different units. Relative isotopic mass (a property of a single atom) is not to be confused with the averaged quantity atomic weight (see above), that is an average of values for many atoms in a given sample of a chemical element.
Relative isotopic mass: the same quantity as atomic mass, but with different units. Relative isotopic mass (a property of a single atom) is not to be confused with the averaged quantity atomic weight (see above), that is an average of values for many atoms in a given sample of a chemical element.


It's okay to get in a rut!
Hmmm. Seems like an odd title doesn't it? I've always thought that it was bad to get in a rut. This week, however, it really paid off.
I'm in the middle of my fifth week in Idaho and I've posted about 250 photos to my website so far. (Click on the link on my main page at www.SaltForkImages.com to check out the fun.) If you were to look through my newest gallery and the other galleries that I've posted in the past from my visits to Idaho and Wyoming, you would notice a lot of the same locations - over and over, again. Some people might think that would get boring. I'm learning to LOVE IT! Every time I visit Grand Teton National Park to shoot the barns on Mormon Row or the reflection at Schwabacher's Landing, I get something different.
The Tetons are an incredible mountain range. Take a shot before 9am and you're almost certain to get something good. The difference between "good" and "spectacular," however, usually depends on the weather. And since the weather changes all the time, it becomes an adventure every time you go back to that same old place.
This week I decided to mix things up and try some sunset photography in GTNP, expecting the mountains to silhouette against the evening sky. What I got was a great surprise. I watched the afternoon weather in Teton Valley, Idaho, just west of the Tetons and noticed some really interesting clouds headed toward the peaks. I raced across Teton Pass and found myself sitting at Schwabacher's Landing an hour later. Schwabacher's is the perfect "poster shot" with the reflection in the beaver pond and the beautiful trees along the shoreline. I've shot it so many times you might say I've gotten in a rut! But this time the weather cooperated and gave me a gorgeous sky.
I hope you like it. It's one of my new favorites.... all because I went back to the same old place.
Keep shooting the same things over and over and you will begin to discover that it can be different every time. Look up! Check the sky. Let the weather help your landscape photographs.
It's been a while since I last posted. I'm sure all of my fans out there - you both know who you are - have missed me..... right?
This spring has been busy. I've done a few portrait sessions and I've done something new: Architectural Photography. I was hired by a friend who builds custom homes to take photos for his new promotional brochure. It's been a unique challenge that has helped to reinforce all those lessons about good photography - remember shutterspeed, aperture, and ISO? All the tradeoffs come into play just like I taught back in our early lessons together.
I shot the indoor shots with low ISO to eliminate graininess, small aperture for sharpness and greater depth of field, and long shutterspeed to ensure proper exposure. And of course, with long shutterspeeds I used a tripod to hold the camera steady.
The other "something different" from the last few weeks is that I did my first Bridal Portrait Shoot. Emily is such a beautiful young lady. Here are a couple of my favorites from her shoot.
We're headed back to Teton Valley, Idaho, for a few weeks of cool mountain weather! Watch my galleries at www.SaltForkImages.com for additions to the Travel and Nature section. I'll be getting up close and personal with the very best that our National Parks have to offer. Grand Teton, Yellowstone, and (hopefully) Glacier are all on the agenda for this summer. I'll update the blog a few times and I'll shoot about 10,000 photos while we are out west. Hopefully there will be a few keepers.
As always, feel free to e-mail me if you have any photography questions or just want to keep up with our adventures.
The Theatre is my Life!
Okay, maybe the title was an exaggeration but I have discovered that it is a lot of fun to photograph theatrical performances.
I told you about the fun I had back in February shooting the winter musical production at Aledo High School. This time I got to shoot a serious one-act play entitled, "The Diary of Anne Frank" and a series of short, one-act comedies that included, "Variations on the Death of Trotsky." These were two very different kinds of plays but the photographic challenges were the same. High ISO, wide open apertures, and a monopod to hold the camera are the only way to have a chance at sharp photos. Even then, about one-third of the shots I took were blurry. That's why I love digital! Just keep shootin' - you're bound to hit SOMETHING!
Here's a shot from, "The Diary of Anne Frank."
And, here's a shot from "Variations on the Death of Trotsky."
I'll be back soon with another lesson so keep checking in.
In early April I made a trip to Las Vegas for a little business with the Nevada Department of Transportation. Those of you that know me well know that a place like Vegas doesn't really interest me. So what did I do? I took the scenic route! We finished with NDOT early and headed for Hoover Dam and the Nevada desert. The tour at Hoover Dam took us down to the generator facility which was very cool. But the real spectacular stuff was the view from the top.
Here's a shot of the generator room.
And this is the view of the back of the dam and an old crane used for transporting men and materials across the canyon.
On the way back to Las Vegas we spotted some cacti blooming in the desert. The sun was high overhead but I think I managed to salvage some pretty good shots.
In Lesson #7 I said, "Get out there and shoot!" So I did.
On Saturday, March 22nd, Spring Break was winding down for Aaron and Sara. Aaron agreed to go with me for a little evening shoot in Downtown Fort Worth and we had SOME KIND OF FUN! We parked at the base of the bridge on North Main Street just north of downtown and walked up to a vantage point where we could see the Tarrant County Courthouse. Aaron enjoyed this part because he's a big "Walker, Texas Ranger" fan and they often use footage of the courthouse on the show.
There are some spots along the side of the bridge deck that are perfect for photographers: away from the traffic and with a great view. We setup the tripod and camera and dialed in a very small aperture with a very long shutterspeed. We were generally shooting about f/22 with 15 to 30 seconds of exposure time. Check out the results below. The red and white streaks are from the traffic going by on the bridge. Very Cool!!!
It was a little harrowing walking up and down the bridge with traffic whizzing by..... but, you know.... anything for the shot!
We left downtown and headed west for home but along the way we got another surprise: there was a carnival in the parking lot at Ridgmar Mall! I've wanted to do some ferris wheel shots ever since I saw the ones my brother posted on his website at www.MyMochaLady.com.
Here are a couple of my favorites. Two to four seconds at f/22 made for some really cool shots.
I hope you liked them. Now get out there and do some of your own shooting!
We've covered a lot on how the camera works and what all the different aperture, shutterspeed, and ISO choices are about.
But the TRUTH is that if you don't PRACTICE what you learn then you won't get any better.
In this lesson I'm going to try to motivate you to get out and shoot some photos. I'm going to give you some quick tips and show you some examples. Along the way perhaps I'll hit on a topic that interests you and then you will run out and use all your new technical knowledge to feed your creativity.
So come along with me and let's shoot some photographs!
Children: We love them and we CAN SHOOT THEM!
Get down on their level. Become a part of their world. Capture them being.....themselves. Big goofy smiles are great but having a photo of a little kid engaged in his world can be priceless.
Annoying Teenagers: They NEED to be SHOT!
When I shoot teenagers, I like to use the longest lens I've got. That helps me peek into their world without getting into their space.
Scenic Landscapes: My all-time favorite subject!
My best tip here is to convince you that the best time of day to shoot is at sunrise and sunset. The quality of the light during those times is so much better than during the harsh direct overhead sunshiny part of the day.
Use the rule-of-thirds. That means don't place the dominant elements of the photograph in the center. Move them over or up to the one-third points in the frame. Look for diagonal lines that help draw the eye into the frame.
Flowers and Veggies: Spring is coming and the Botanic Garden could become your favorite place!
Don't just shoot down. Get down on their level. Use what you know about aperture to blur the backgrounds and selective focus on one flower. Remember the rule-of-thirds.
Animals: Shoot the family dog - especially if he barks all night. Capture shots of your kids interacting with their pets. Focus on the animal's eyes - that's where we are drawn when we look at the photo. If you like wild animals, do your homework. Learn what times they are most active. Get into their world.... but be careful. Travel to a National Park or State Park; wild animals are a little less wild there.
I hope you've enjoyed these photos as much as I have. Start a collection of personal favorites. It's great to show them off and it's great to look back and see how your creativity and talent have progressed.
In Lesson #4 I described the tradeoffs involved in your choice of ISO. Increase the ISO and you can shoot at higher shutterspeeds or in low-light conditions. Higher ISO will also get you more digital noise or graininess - that's the tradeoff.
This lesson covers the tradeoffs involved with aperture. You know..... f/stops....... f/numbers!
Remember that the aperture is the hole in the lens through which light travels on its way to the film or sensor. The aperture is adjustable from large f-numbers which correspond to small apertures to small f-numbers which correspond to large apertures.
Confusing? Maybe a definition will help; -- MATH ALERT! -- The f-number (or f/stop) is the ratio of the focal length of the lens to the diameter of the opening in the aperture. An f/stop of 8 means the diameter of the aperture is 1/8th of the focal length of the lens. If you wanted to double the area of the aperture to let in twice as much light, the f/stop would go from 8 to 5.6.
Remember that the area of a circle varies with the SQUARE of the diameter. Go through the math and you'll find that the area of the aperture doubles when you divide the f/stop by 1.414, which of course is the square root of two.
Don't worry about it. That last part was for geeks like me that just MUST UNDERSTAND THE MATH!
Here's the important part: Big aperture = small f-number AND small aperture = big f-number.
So when I say "OPEN up the lens," I mean go to a small f/stop or f-number. When I say "stop down the lens" I mean go to a large f/stop or large f-number.
Stop down the lens to a small aperture (like f/22) and you will increase your depth of field. Open up the lens to a large aperture (like f/2.8) and the depth of field will become shallow.
Depth of field is all about how much of the subject matter in your photograph is in focus. Focus on an object out in front of you and there will be a zone in front of and behind the object that is also in focus. With a small aperture (like f/22) the zone will be large and may extend from a few inches in front of you all the way to infinity. With a wide open aperture (like f/2.8) the zone will be small - perhaps only a few inches in front of and behind your subject. How wide the zone is for a particular lens depends on the size of the aperture you choose.
In landscape photography it is sometimes interesting to have the foreground and the background in focus. Stop down the lens to a small aperture and compose the shot. Now remember, the small aperture lets in less light than a large aperture so it naturally follows that a good exposure will require a longer shutterspeed. The aperture is small so it will need to be open longer. That could be a problem if you are handholding the camera or if your subject is moving.
In portrait photography it is sometimes nice to blur the background so that the subject really stands out. Open up the lens to a wide aperture and compose the shot. Again, the wide aperture means the shutter doesn't have to be open very long. The fast shutterspeed could be great if you need to handhold the camera.
In this shot of the young lady, the ISO was 400, the shutterspeed was 1/200th of a second, and the aperture was at f/2.8. I handheld this shot because the shutterspeed was fast enough to compensate for any camera shake that might have occurred and because I didn't want to set up a tripod on the railroad tracks!
The most important thing to understand is that your choice of aperture affects how much of the photo will be in focus - or how much "depth of field" you have.
Small aperture = large f/stop = lots in focus. Large aperture = small f/stop = very small plane of focus.
If you remember back in Lesson #2 I talked about shooting in Aperture Priority. This is how I shoot about 90 percent of the time. I control the aperture and the ISO and I let the camera pick the shutterspeed. I do this because I want creative control over what is in focus and what is blurry. Even though I'm not controlling the shutterspeed directly, I ALWAYS watch the shutterspeed to make sure it is fast enough for my conditions. If it isn't, then I bump my ISO upward to speed up the shutter. It's all about knowing how the camera works!
Go out and try to shoot with different f/stops and see what effect it has on your photographs.


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The Idyllic school (also known as the Idyllists) was a 19th-century art movement of British artists—both painters and illustrators—whose depictions of rural landscapes combined elements of social realism and idealism. Van Gogh's well-known admiration for the group was shown in letters to his brother Theo, and in his collection of their work extracted from contemporary British newspapers, such as the Illustrated London News and The Graphic. Nowadays the Idyllist school is seen as one of the earliest manifestation of the social realism movement in art

List of idyllist artists

John William North ARA RWS
Frederick Walker ARA RWS
George John Pinwell RWS
Robert Walker Macbeth RA RWS
George Hemming Mason ARA
Arthur Boyd Houghton
Hubert von Herkomer RA
Richard Jefferies (writer)

See also

Helen Allingham RWS
George Clausen
Alice Mary Havers
Lionel Smythe

References

Further reading

Paul Goldman, Victorian Illustration: The Pre-Raphaelites, the Idyllic School and the High Victorians (Lund Humphries, 1996)
Donato Esposito, Frederick Walker and the Idyllists (London: Lund Humphries, 2017)
Scott Wilcox and Christopher Newall, Victorian Landscape Watercolours (Hudson Hills, 1992), p. 55.

External links

The Idyllists

British art movements


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Malaysia to Give Citizenship to Over 3,400 Permanent Residents of Indian Origin
People celebrating Malaysian Independence Day in Merdeka Square, Kuala Lumpur. [Representational Image]
Over 3,000 people of Indian descent in Malaysia are set to get the country's citizenship after Prime Minister Dr Mahathir Mohamad announced the move this week. The scheme is applicable to Indian-origin persons aged over 60 years, who have already applied for the citizenship status.
The move is in accordance with the election manifesto of the political coalition Pakatan Harapan, which had pledged to extend citizenship status to the 3,407 Indians, who are over the age limit of 60 years and possess red MyKads, Mohamad told the media at the Parliament in Kuala Lumpur on Aug. 14, Malaymail reported.
Red Mykad is a Malaysian identity card given to permanent residents in the country. Citizens of Malaysia, on the other hand, carry Blue Mykad.
The move will not be implemented immediately, since it requires each person to meet several official conditions, such as getting oneself registered at the National Registration Department (NRD).
"If he is a red card holder, 60-years-old and above, he will be given a blue card (MyKad). He has to fill a form at the NRD," Mohamad said, the New Straits Times reported.
People who are under 60 years old will be considered for citizenship only if one parent of the applicant is a Malaysian. The government may also look into cases where the marriage of the parents of the applicant was not registered, he added.
It is mandatory for the applicant to be Malaysia-born and clear a simple Bahasa Malaysia competency test.
"The Bahasa Malaysia competency test will only touch on simple use of the language. If they pass, then we will accept them (as citizen). There will also be a requirement for them to be based in Malaysia for at least 12 years, in which they have actually resided in the country for 10 years, according to the Federal Constitution," Mohamad was quoted as saying by the media.
He added that his 100-day-old pledge was currently restricted to the Indian community, but in future, it will be extended to cover other communities as well.
The Indian community in Malaysia includes Hindus, Buddhists, Sikhs, Christians and Muslims, according to a survey conducted in 2017 by the NGO MyDaftar. People of Indian origin in the country are mainly Tamil-speaking while a significant number speak Telugu, Malayalam, Hindi and Punjabi, it added.
Indian identity issues were in the spotlight in Malaysian general election in 2018, when Mohamad himself was targeted for his Indian roots.
The 93-year-old politician, who happens to be the world's oldest serving prime minister, was born in Malaysia but shares his roots with India, which was an issue used by his opponents to target him during the election campaign earlier this year.
Categories: NRI, Politics
Tags: Diaspora, Mahathir Mohamad, Malaysia


Save time. Save energy. Save frustration.
is available from Amazon.com as a Kindle book (US$4.40) — no Kindle required. This is the first Kindle ebook from MacTips.info.
The 22 Tips and techniques in this ebook are sure to save you time as you use your Mac. Whether you're a raw beginner or an experienced user you will find tips here for work and play with your Mac.
You don't need a Kindle device to read this ebook — you can read it on your Mac, iPhone or iPad using the free Kindle software — search the App Store for your device for Kindle.
I've drawn on Tips from the website and written extra Tips too. Each Tip in this book is complete in itself, but where the website has more information that could help, well, I've added a link right there in the book for you.
22 Tempting Timesavers for Mac Users.
Find quick ways to name files or save them to the right place. Find out how to quickly move around in the Finder or call up web browser bookmarks. Find out how to clean up your workspace with the press of a key, or how to have your Mac read you stories. Looking for one particular thing on a long web page? This books shows you how to find it in an instant. Trouble reading tiny print? This book shows you how to zoom in for a better look.
If you read MacTips, please buy this ebook. You'll like the Tips, I'm sure, but you're also helping to support the site. It's only the price of a coffee. In fact, why not read it with a coffee (or my preferred beverage, green tea)?
And please, leave a review at Amazon after you've read the book. Reviews help sales. Sales help me. And that means I can get on with the job of writing more free Tips for you all.
Thanks for reading MacTips, and for telling others about the Tips.
Now, don't you have something you're supposed to be doing?


In this post I'll focus on the privacy aspect of secure websites only —the extent to which communication is protected from eavesdroppers. Issues of trust are just as important, but I'll have to discuss those in a future post.
As you can see, there are five different encryption protocols listed, in increasing order of strength. Generally speaking, TLS is better than SSL and more recent versions of TLS are better still. Published attacks on these protocols typically enable someone who can view network traffic to decrypt some or even all of the information passing over the 'secure connection'. This type of scenario is called a 'man in the middle attack' because the eavesdropper stands in between your browser and the website it is communicating with.
If your browser always chooses the best encryption available, why would you want to configure the specific protocols it supports? Unfortunately, the very first part of the communication between your browser and the website is more vulnerable. The two systems have to agree on an encryption protocol to use before they can be truly private. In some special cases it is possible for a man in the middle to intervene and force a weaker protocol to be negotiated. By configuring your browser to support only stronger protocols, you can ensure that your browser is never tricked this way.
Here at Questionmark, we care about your security too! If a protocol like SSLv3 is considered vulnerable to interception, shouldn't the server refuse to use it as well? Yes, it should. In fact, we don't support SSL versions 2 and 3 for this very reason.
For this blog post I've focused on the most visible aspect of the security protocol. In practice, there lots of subtle differences in the way each protocol can be configured. If you use Google's Chrome browser you can click on the padlock to reveal information about connection security.
Notice that this connection uses TLS 1.2, but there is even more detail reported concerning the specific cryptographic algorithms used. Sites like www.ssllabs.com have almost 50 separate check points that they can report on for a public-facing secure website! Staying on top of all this configuration complexity is critical to keeping websites secure.
Unfortunately, sometimes we have to strengthen security in such a way that compatibility with older browsers is sacrificed. For example, according to the latest simulation results, Internet Explorer version 6 (running on Windows XP) is no longer able to successfully negotiate a secure connection with our OnDemand service.
In practice, an overwhelming majority of users use more modern browsers (or have access to one), so the web remains both secure and usable. Perhaps a greater cause of concern is older applications that are integrated with our APIs. It is just as important to keep these applications up to date. For example, applications that use older versions of Java, such as Java 6 or have their Java runtime configuration options set inappropriately might have problems communicating to the same high standards. If you are running a custom integration and are concerned about future compatibility, please get in touch.
This is a developing field. New ways of exploiting older protocols and cryptographic algorithms are being found by security researchers all the time, and the bad guys aren't far behind. Our security specialists at Questionmark constantly monitor best practice and update the configuration of our OnDemand service to keep your communications safe.


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Dhaval Jayantilal Gada, popularly known as DG, is an Indian film and TV producer. He is a young businessperson who is quickly turning into a power figure within the Hindi film industry and the television industry. Born to Hansa Gada and Hindi film maker Jayantilal Gada, Dhaval is an acclaimed producer and establisher of the famous PEN India Ltd, which is a movie production banner. He has a sister and a brother. He was born in Mumbai. He did his education from Pinewood International (Panchgani) and then finished his further studies in Mumbai.
As enthusiastic as he is about film making, Dhaval is also interested in Formula 1 and has pursued it since he was very young. He sought after his enthusiasm for auto racing and kept on making his imprint in the sector by winning many laurels. When he was 12 years old, he won the JK Tire first runner-up place in the Indian National Championship in F4 (Go-kart) racing. Dhaval Gada's role model is his dad Jayantilal and who was the motivation for him to start his very own production house. Dhaval Jayantilal Gada assumed control over PEN India Ltd on November 3, 2014, turning into the youngest filmmaker in the Bollywood film industry.
Dhaval has, from that point forward, delivered and co-created a few well-understood films under the PEN India Ltd. pennant, including ' Kahaani' and ' Entertainment', setting up himself as a maker in the film business. Other than assuming the responsibility of PEN India Ltd, Dhaval additionally shaped his organization, Dhaval and Gurudev Productions that produces TV drama series. He entered the TV business in 2014 with 'Udaan Sapnon Ki', which recorded the most elevated TRPs.
Prominently known as Udaan Sapnon Ki, the Indian TV dramatization show premiered on August 18, 2014, and is aired on Colors, an Indian TV channel. Together created by Bollywood filmmaker Mahesh Bhatt, the drama is meant to highlight the issue of reinforced work in Indian towns and conveys an essential social message.
Gada's other TV endeavor is ' Dil Ki Baatein Dil Hi Jaane', featuring well-known TV stars Ram Kapoor and Gurdeep Kohli that premiered March 23, 2015, which aired on Sony Entertainment Television. Bhatt conceptualized the show. He has also produced other movies like 'Singh Is Bliing', and the famous television series ' Mahabharat'.


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Q: Why is my subdomain returning a 403 status? I have a Wordpress installation at www.mysite.com. Wordpress is installed in /public_html/
I created a sub domain test.mysite.com. cPanel asks for the directory in my file system. I pointed it to /public_html/wp-content/themes/mytheme/test/. When I do this, I get a 403 error. When I point it to /public_html/, it works - displays main page of my website.
How do I get test.mysite.com to show what I have in /public_html/wp-content/themes/mytheme/test/

A: There are some questions I have but cannot add a comment so will do my best to help clarify the steps to set up a subdomain network: http://codex.wordpress.org/Create_A_Network.
First, the multisite feature of WordPress needs to be enabled. Did you do the steps required to enable multisite?
Second, the same wordpress files are used for the main site and any network enabled site. In other words, if you have public_html/wordpress for the domain.com then in cpanel you also point the subdomain to public_html/wordpress for a sub.domain.com. You do not create a directory public_html/wordpress/sub. The directory does not exist but the multisite feature enabled will recognize to render the WP files when sub.domain.com is requested in the browser.

A: Check if your router dns settings, are set for the isp dns server.


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The government's protection of the wealthy is bad news for the average property investor
By now it should be overwhelmingly clear – the government has no interest in housing affordability and they will not take any measure to lower land values. If the budget didn't paint the picture, no doubt the forthcoming Senate inquiry into housing will.
'The age of entitlement' is not over – it has been protected at the expense of 'the age of opportunity'.
The current administration has surgically set about reducing living standards of the poor, making cuts to heath, education, and employing harsh means testing measures which will fall most heavily on the old, young, unemployed and a broad sector of low to middle income families with dependant children.
They have done this to studiously protect the interests of the wealthy, refusing to lay a finger on the licensed resource monopolies, the mineral wealth of which increased more than $55 billion in 2012-13 alone.
Clawing back just a fraction of the tax exemptions granted on capital gains, or placing a levy per ton of exported minerals, would not only have gone a long way to covering the budget short fall, but would also have lifted the burden from the poorest onto the richest. But in a political system where major parties sell themselves to the highest bidder (which as current ICAC investigations suggest happen to be property developers and large land holders), their failure to do so should come as no surprise.
It walks hand-in-hand with the diabolical decision by "Australia's premier real estate industry education and training provider", AREC, to employ an ex convict who defrauded clients out of more than $200 million to educate real estate agents at the biggest industry training event of the year. Despite protests from various participants, the event has sold out and clearly not prickled the conscience of the other speakers who are happy to stand alongside 'The Wolf of Wall Street', Jordan Belfort.
The above measures, along with Tony Abbott's desire to be knighted the 'infrastructure Prime Minister' will drive investment into housing – albeit, of the speculative kind.
Infrastructure intensifies the use and demand for residential land as the population grows and no doubt, we need more of it. However, it also has the effect of rising land values, which taken alone, should be a 'good' thing for our country (or at least it would be, if those gains truly benefitted the community).
Instead those gains will be pocketed, leaving the government to scrape future funding from elsewhere.
Story continues on page 2. Please click below.


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