Bangladesh has told the UN Security Council it will stop accepting any more Rohingya Muslims who flee from Myanmar.

Bangladesh has told the UN Security Council it will stop accepting any more Rohingya Muslims who flee from Myanmar.

Foreign Secretary Shahidul Haque accused Myanmar of "hollow promises" during negotiations over returns.

More than 740,000 Rohingya are in camps in Bangladesh after they were driven out of Myanmar's Rakhine state during military crackdowns in 2016 and 2017.

The UN describes the crisis as ethnic cleansing. Myanmar denies persecuting the Rohingya, a stateless minority.

What awaits the Rohingya back in Myanmar?
Bangladesh upholds Rohingya marriage ban
Could Aung San Suu Kyi face Rohingya genocide charges?

The latest row comes despite a deal between Bangladesh and Myanmar in January 2018 to repatriate Rohingya refugees.

Myanmar had agreed to accept 1,500 Rohingya each week, Bangladesh said at the time, adding that it aimed to return all of them to Myanmar within two years.

Speaking at Thursday's meeting of the UN Security Council, Mr Haque said his country could not accept more refugees.

"Not a single Rohingya has volunteered to return to Rakhine due to the absence of conducive environment there," he said.

"Is Bangladesh paying the price for being responsive and responsible in showing empathy to a persecuted minority population of a neighbouring country?"

Myanmar's ambassador to the UN, Hau Do Suan, appealed for patience, speaking of "huge physical as well as psychological barriers" in repatriating Rohingya.
Media captionRohingya Muslims displaced from Tula Toli village in Rakhine State gave disturbing accounts to BBC Newsnight

"It takes time and patience as well as courage to build trust and confidence among different communities in Rakhine," the diplomat added.

Meanwhile, the UN envoy to Myanmar, Christine Schraner Burgener said progress in returning Rohyngya to Myanmar was "slow".

Seeing through the official story in Myanmar
What you need to know about the crisis
Is refugee crisis 'textbook ethnic cleansing'?

She also said that Myanmar authorities had given UN agencies "insufficient" access to help repatriate Rohingya.

https://twitter.com/hlamyint1940/status/1105167373680631810

https://twitter.com/hlamyint1940/status/1105167373680631810

BBC News - Brexit: May heads to Strasbourg for last-ditch talks with EU
11:03 AM - 11 Mar 2019

Brexit: May heads to Strasbourg for last-ditch talks with EU

49 minutes ago
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Media captionBig Brexit moment: Will MPs back or bin the PM's deal?

Theresa May is heading to Strasbourg for last-ditch talks with senior EU officials aimed at winning MPs' backing for her Brexit deal.

She will meet European Commission President Jean-Claude Juncker on the eve of the second vote on her deal.

The BBC's Laura Kuenssberg said the trip did not guarantee there is a new deal to be signed by both sides.

But she said sources told her they believe direct talks are the right way to progress at this critical moment.

The EU has said it is now up to MPs to decide the next steps for Brexit and it remains "committed" to agreeing a deal.

But earlier in the Commons, Labour leader Jeremy Corbyn said there had "not been a single change" to the agreement since it was heavily defeated by MPs in January and it was still a "bad deal".

Following speculation the vote could be postponed or downgraded, No 10 said the motion to be debated would be published later on Monday - although it gave no details of what it could contain.

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Downing Street said the PM's focus was "getting on with the work required to allow MPs to support the deal and to bring this stage of the process to an end".
Image Copyright @bbclaurak @bbclaurak
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The UK is due to leave the EU on 29 March but MPs rejected the withdrawal deal on offer in January and demanded major changes.
Media captionJeremy Corbyn, on Brexit negotiations: "This is a government in chaos."
What is the EU saying?

BBC Brussels reporter Adam Fleming said the mood was "bleak" in Brussels after the EU's chief Brexit negotiator, Michel Barnier, briefed EU ambassadors on the state of play earlier.

Adam Fleming said the member states were told that the UK had rejected the EU's proposed solutions on the backstop because "they wouldn't get the support of the Cabinet".

"There is a widely held view that the UK has not been negotiating in good faith over the last few days," he said, adding that at least one diplomat had mentioned planning for a "post-Theresa May government".

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The government has been seeking changes to the Irish backstop, the safety net designed to maintain an open border on the island of Ireland, and only to be used as a last resort.

But the details of it were a sticking point for many MPs when they voted her deal down in January. They worry that - in its current form - the backstop may leave the UK tied to the EU indefinitely.

In a statement, the Commission said it had put forward proposals to try to reassure MPs the backstop "if used will apply temporarily".

A spokesman said the EU was willing to meet UK negotiators at any time.

He added: "We are committed to using our best endeavours to find a subsequent agreement that replaces the backstop... We are committed to ratifying this deal before 29 March."
Media captionIs the UK actually in a crisis over leaving the EU?
How have MPs reacted?

Brexit minister Robin Walker has been updating MPs in response to an urgent question from Labour.

He said the government "absolutely stood by" its commitment to hold Tuesday's vote and, if the PM's deal was defeated, subsequent votes by Thursday at the latest on a no-deal exit and extending talks.

Details of Tuesday's "meaningful vote" motion will be published by the end of Commons business, expected to be about 22.00 GMT, while Brexit Secretary Stephen Barclay will be making a statement before that.

Labour MP Pat McFadden said any vote had to be on the Brexit deal, as currently constituted, and not a version of the deal ministers might hope to end up with after further talks with the EU.

And Tory Brexiteer Peter Bone urged the government to delay the vote until MPs had had enough time to scrutinise any changes to the deal.
What could happen this week?

Theresa May's deal to face a "meaningful vote" in Parliament on Tuesday
If it's rejected, a further vote has been promised for Wednesday on whether the UK should leave without a deal
If that no-deal option is rejected, MPs could get a vote on Thursday on whether to request a delay to Brexit from the EU.

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aung naing moe/ satire about tuitions/ 9 march 2019

Aung Naing Moe
32 mins ·

ဆယ္​တန္​း​ေက်ာင္​းသား​ေတြ စာ​ေမးပြဲ​ေျဖခ်ိန္​ဆို​ေတာ့ ကံခြၽန္​ရဲ႕​"​ေခတ္​​ေက်ာင္​းသား"ဆိုတဲ့ လုံးခ်င္း​ဝတၳဳ​တပုဒ္​ကို သတိရမိတယ္​။ ဆယ္​တန္​းကို တဘုံးဘုံးက်ၿပီး က်ဴ႐ွင္​တက္​ရင္​း အျပင္​က​ေန ​ေျဖဆို​ေနၾကတဲ့ ​ေက်ာင္း​သား​ေတြ ဘဝကို ​ေရးဖြဲ႔ထားတာ။ က်ဴ႐ွင္​ဆရာ​ေတြရဲ႕ သဘာဝ၊ ​ေက်ာင္​းသား​ေတြရဲ႕ဓ​ေလ့စ႐ိုက္​ ပီျပင္​တယ္​။

ဇာတ္ဝင္ခန္းတခုမွာ ​​​ဇာတ္​​ေကာင္​ဆယ္​တန္​း​ေက်ာင္​းသားက လက္​ဖက္​ရည္​ဆိုင္​သြားဖို႔ သူ႔သူငယ္​ခ်င္​းအိမ္​ဆီ ထြက္​လာတယ္​။ အိမ္​နားနီးလာ​ေတာ့ အိမ္​အ​ေပၚထပ္​မွာ ဟို​ေကာင္​ ​ေရနံ​ေျမသပိတ္​အ​ေၾကာင္​း ​ေအာ္​က်က္​​ေနသံ ၾကားရတယ္​။ ​ေအာ္​က်က္​ရင္​း တ​ေနရာ​ေရာက္​​ေတာ့ "သခင္​... သခင္​... သခင္​... သခင္​..." ဆိုၿပီး ထစ္​​ေနတယ္​။ အဲ့ဒီမွာ အိမ္​​ေအာက္​ထပ္​မွာ စက္​ဘီးျပင္​​ေနတဲ့ သူ႔အ​ေဖ ဦးတိုးက "ဘိုးလွႀကီး" ဆိုၿပီး ၾကံဳး​ေအာ္​လိုက္​သတဲ့။

ၿပီး​ေတာ့​ေျပာ​ေသးသတဲ့။ "မင္​းသူငယ္​ခ်င္​း အဲ့ဒီ​ေရနံ​ေျမသပိတ္​ကို က်က္​လာတာ ​ေလးႏွစ္​​ေလာက္​ ႐ွိၿပီ။ အခုထိအလြတ္​မရ​ေသးဘူး။ ​ေဘးပတ္​လည္​အိမ္​​ေတြက က​ေလး​ေတြ​ေတာင္​ သူ႔စာက်က္​သံနား​ေထာင္​ၿပီး ဆယ္​တန္​းကို တ​ေယာက္​ၿပီးတ​ေယာက္​ ​ေအာင္​ကုန္​ၾကၿပီ" တဲ့။

ကံခြၽန္​ဝတၳဳကို က်​ေနာ္​မွတ္​မိသ​ေလာက္​ ျပန္​​ေရးျပတာပါ။ က်​ေနာ္​ ဆယ္​တန္​းတုန္​းက အင္​းစိန္​၊ မင္​းႀကီးလမ္​းက ဆရာဦးတင္​့စိန္​ဖူးက်ဴ႐ွင္​နဲ႔ ဆရာဦးစံသိန္​းက်ဴ႐ွင္​​ေတြ တက္​ခဲ့တာ ျပန္​​ေျပာင္​းသတိရမိပါတယ္​။ ဆရာ​ေတြ ​ေတာ္​ၾကပါတယ္​။ အထူးသျဖင္​့ ဆရာဦးတင္​့စိန္​ဖူးဟာ အသင္​အျပလည္​း​ေကာင္​း၊ ​ေစတနာလည္​း​ေကာင္​း၊ ​ရယ္​စရာလည္​း​ေျပာတတ္​တဲ့ ဆရာတ​ေယာက္​ပါ။ အဲ့သည္​တုန္​းက ညဦးပိုင္​းက်ဴ႐ွင္​ခ်ိန္​​ေတြဟာ ​ေပ်ာ္​စရာကာလမ်ားပါ။
9You, Nyan Gyi, Soe Nilar Aung and 6 others
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Aung Naing Moe
2 hrs ·

ေရႊခ်ထား​သင္​့​ေသာ
===========

- ​အ​ေမြစုဟာ အဘ​ေတြ​ ခ်မွတ္​ခဲ့တဲ့ လမ္​းျပ​ေျမပုံ ၇ ခ်က္​ကို ၿပီး​ေျမာက္​​ေအာင္​ အိမ္​ဝင္​ျဖည္​့​ေပးခဲ့တယ္​။

- အ​ေမြစုဟာ အဘ​ေတြ​ ​ေရးဆြဲအတည္​ျပဳခဲ့တဲ့ ၂၀၀၈ ​ေျခဥကို ကာကြယ္​​ေစာင္​့​ေ႐ွာက္​ပါမည္​လို႔လည္​း က်မ္​းသစၥာက်ိန္​ဆိုခဲ့တယ္​။

- အ​ေမြစုဟာ အဘ​ေတြနဲ႔ ရင္​ၾကား​ေစ့ဖို႔ကိုလည္​း အခ်ိန္​႐ွိသမ်ွ လူသိ႐ွင္​ၾကား တြင္​တြင္​​ေျပာၾကားတယ္​။

- အ​ေမြစုဟာ အဘ​ေတြကို သူမရဲ႕အစိုးရအဖြဲ႔ထဲမွာ ​ေနရာ​ေတြ​ေပးတယ္​။

- အ​ေမြစုဟာ အဘ​ေတြနဲ႔ အႀကိမ္​ႀကိမ္​​ေတြ႔ဆုံၿပီး ဘာ​ေျပာခဲ့ၾကသလဲဆိုတာကို ၿမံဳထားတယ္​။

- ​အ​ေမြစုဟာ အဘ​ေတြနဲ႔ခ႐ုိနီ​ေတြအက်ိဳးစီးပြားကို ကာကြယ္​​ေစာင္​့​ေ႐ွာက္​တယ္​။

​အဲ့သလို​ လုပ္ရပ္​ေ​​တြအတြက္ ​အ​ေမြစုကို ​ေဝဖန္​တဲ့အခါ အ​ေမြစု​ေထာက္​ခံသူ​ေတြက ​ေဝဖန္​သူကို အဘ​ေဘာမလို႔ တံဆိပ္​ကပ္​ၾကတယ္​။ အႏွီ အ​ေမြစု​ေထာက္​ခံသူ​ေတြဟာ ​ေရႊခ်ထားရမယ္​့ ဦး​ေႏွာက္​ပိုင္​႐ွင္​​ေတြျဖစ္​တယ္​။

Learning physics Faraday's law 6 march 2019.

Learning physics Faraday's law 6 march 2019.
Qualitative statement

The most widespread version of Faraday's law states:

The electromotive force around a closed path is equal to the negative of the time rate of change of the magnetic flux enclosed by the path.[13][14]

The closed path here is, in fact, conductive.
Quantitative
The definition of surface integral relies on splitting the surface Σ into small surface elements. Each element is associated with a vector dA of magnitude equal to the area of the element and with direction normal to the element and pointing "outward" (with respect to the orientation of the surface).

Faraday's law of induction makes use of the magnetic flux ΦB through a hypothetical surface Σ whose boundary is a wire loop. Since the wire loop may be moving, we write Σ(t) for the surface. The magnetic flux is defined by a surface integral:

Φ B = ∬ Σ ( t ) B ( r , t ) ⋅ d A , {\displaystyle \Phi _{B}=\iint \limits _{\Sigma (t)}\mathbf {B} (\mathbf {r} ,t)\cdot \mathrm {d} \mathbf {A} \,,} {\displaystyle \Phi _{B}=\iint \limits _{\Sigma (t)}\mathbf {B} (\mathbf {r} ,t)\cdot \mathrm {d} \mathbf {A} \,,}

where dA is an element of surface area of the moving surface Σ(t), B is the magnetic field (also called "magnetic flux density"), and B·dA is a vector dot product (the infinitesimal amount of magnetic flux through the infinitesimal area element dA). In more visual terms, the magnetic flux through the wire loop is proportional to the number of magnetic flux lines that pass through the loop.

When the flux changes—because B changes, or because the wire loop is moved or deformed, or both—Faraday's law of induction says that the wire loop acquires an EMF, E, defined as the energy available from a unit charge that has travelled once around the wire loop.[15][16][17] (Note that different textbooks may give different definitions. The set of equations used throughout the text was chosen to be compatible with the special relativity theory.) Equivalently, it is the voltage that would be measured by cutting the wire to create an open circuit, and attaching a voltmeter to the leads.

Faraday's law states that the EMF is also given by the rate of change of the magnetic flux:

E = − d Φ B d t , {\displaystyle {\mathcal {E}}=-{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}},} {\displaystyle {\mathcal {E}}=-{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}},}

where E is the electromotive force (EMF) and ΦB is the magnetic flux.

The direction of the electromotive force is given by Lenz's law.

The laws of induction of electric currents in mathematical form was established by Franz Ernst Neumann in 1845.[18]

Faraday's law contains the information about the relationships between both the magnitudes and the directions of its variables. However, the relationships between the directions are not explicit; they are hidden in the mathematical formula.
A Left Hand Rule for Faraday's Law. The sign of ΔΦB, the change in flux, is found based on the relationship between the magnetic field B, the area of the loop A, and the normal n to that area, as represented by the fingers of the left hand. If ΔΦB is positive, the direction of the EMF is the same as that of the curved fingers (yellow arrowheads). If ΔΦB is negative, the direction of the EMF is against the arrowheads.[19]

It is possible to find out the direction of the electromotive force (EMF) directly from Faraday’s law, without invoking Lenz's law. A left hand rule helps doing that, as follows:[19][20]

Align the curved fingers of the left hand with the loop (yellow line).
Stretch your thumb. The stretched thumb indicates the direction of n (brown), the normal to the area enclosed by the loop.
Find the sign of ΔΦB, the change in flux. Determine the initial and final fluxes (whose difference is ΔΦB) with respect to the normal n, as indicated by the stretched thumb.
If the change in flux, ΔΦB, is positive, the curved fingers show the direction of the electromotive force (yellow arrowheads).
If ΔΦB is negative, the direction of the electromotive force is opposite to the direction of the curved fingers (opposite to the yellow arrowheads).

For a tightly wound coil of wire, composed of N identical turns, each with the same ΦB, Faraday's law of induction states that[21][22]

E = − N d Φ B d t {\displaystyle {\mathcal {E}}=-N{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}} {\displaystyle {\mathcal {E}}=-N{\frac {\mathrm {d} \Phi _{B}}{\mathrm {d} t}}}

where N is the number of turns of wire and ΦB is the magnetic flux through a single loop.
Maxwell–Faraday equation
An illustration of the Kelvin–Stokes theorem with surface Σ, its boundary ∂Σ, and orientation n set by the right-hand rule.

The Maxwell–Faraday equation states that a time-varying magnetic field always accompanies a spatially varying (also possibly time-varying), non-conservative electric field, and vice versa. The Maxwell–Faraday equation is

∇ × E = − ∂ B ∂ t {\displaystyle \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}} \nabla \times \mathbf {E} =-{\frac {\partial \mathbf {B} }{\partial t}}

(in SI units) where ∇ × is the curl operator and again E(r, t) is the electric field and B(r, t) is the magnetic field. These fields can generally be functions of position r and time t.

The Maxwell–Faraday equation is one of the four Maxwell's equations, and therefore plays a fundamental role in the theory of classical electromagnetism. It can also be written in an integral form by the Kelvin–Stokes theorem:[23]

∮ ∂ Σ ⁡ E ⋅ d l = − ∫ Σ ∂ B ∂ t ⋅ d A {\displaystyle \oint _{\partial \Sigma }\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-\int _{\Sigma }{\frac {\partial \mathbf {B} }{\partial t}}\cdot \mathrm {d} \mathbf {A} } {\displaystyle \oint _{\partial \Sigma }\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-\int _{\Sigma }{\frac {\partial \mathbf {B} }{\partial t}}\cdot \mathrm {d} \mathbf {A} }

where, as indicated in the figure:

Σ is a surface bounded by the closed contour ∂Σ,
E is the electric field, B is the magnetic field.
dl is an infinitesimal vector element of the contour ∂Σ,
dA is an infinitesimal vector element of surface Σ. If its direction is orthogonal to that surface patch, the magnitude is the area of an infinitesimal patch of surface.

Both dl and dA have a sign ambiguity; to get the correct sign, the right-hand rule is used, as explained in the article Kelvin–Stokes theorem. For a planar surface Σ, a positive path element dl of curve ∂Σ is defined by the right-hand rule as one that points with the fingers of the right hand when the thumb points in the direction of the normal n to the surface Σ.

The integral around ∂Σ is called a path integral or line integral.

Notice that a nonzero path integral for E is different from the behavior of the electric field generated by charges. A charge-generated E-field can be expressed as the gradient of a scalar field that is a solution to Poisson's equation, and has a zero path integral. See gradient theorem.

The integral equation is true for any path ∂Σ through space, and any surface Σ for which that path is a boundary.

If the surface Σ is not changing in time, the equation can be rewritten:

∮ ∂ Σ ⁡ E ⋅ d l = − d d t ∫ Σ B ⋅ d A . {\displaystyle \oint _{\partial \Sigma }\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-{\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma }\mathbf {B} \cdot \mathrm {d} \mathbf {A} .} {\displaystyle \oint _{\partial \Sigma }\mathbf {E} \cdot \mathrm {d} \mathbf {l} =-{\frac {\mathrm {d} }{\mathrm {d} t}}\int _{\Sigma }\mathbf {B} \cdot \mathrm {d} \mathbf {A} .}

The surface integral at the right-hand side is the explicit expression for the magnetic flux ΦB through Σ.

Learning physics. 6 march .2019 Newton's law of universal gravitation.

6 march 2019

Learning physics.
14 feb.2019 thurs.


Newton's law of universal gravitation
states that every particle attracts every other particle in the universe with a force which is directly proportional to the product of their masses and inversely proportional to the square of the distance between their centers.[note 1] This is a general physical law derived from empirical observations by what Isaac Newton called inductive reasoning.[1]

It is a part of classical mechanics and was formulated in Newton's work Philosophiæ Naturalis Principia Mathematica ("the Principia"), first published on 5 July 1687. When Newton presented Book 1 of the unpublished text in April 1686 to the Royal Society, Robert Hooke made a claim that Newton had obtained the inverse square law from him.


In today's language, the law states that every point mass attracts every other point mass by a force acting along the line intersecting the two points.
The force is proportional to the product of the two masses, and inversely proportional to the square of the distance between them.[2]


The equation for universal gravitation thus takes the form:
F = G m 1 m 2 r 2 {\displaystyle F=G{\frac {m_{1}m_{2}}{r^{2}}}\ }
where F is the gravitational force acting between two objects, m1 and m2 are the masses of the objects, r is the distance between the centers of their masses, and G is the gravitational constant.



The first test of Newton's theory of gravitation between masses in the laboratory was the Cavendish experiment conducted by the British scientist Henry Cavendish in 1798.[3]

It took place 111 years after the publication of Newton's Principia and approximately 71 years after his death.
Newton's law of gravitation resembles Coulomb's law of electrical forces, which is used to calculate the magnitude of the electrical force arising between two charged bodies.

Both are inverse-square laws, where force is inversely proportional to the square of the distance between the bodies.
Coulomb's law has the product of two charges in place of the product of the masses, and the electrostatic constant in place of the gravitational constant.
Newton's law has since been superseded by Albert Einstein's theory of general relativity, but it continues to be used as an excellent approximation of the effects of gravity in most applications.
Relativity is required only when there is a need for extreme accuracy, or when dealing with very strong gravitational fields, such as those found near extremely massive and dense objects, or at very close distances (such as Mercury's orbit around the Sun).

ဗင္နီဇြဲလားျပည္သူေတြ တနလၤာေန႔ ဆႏၵျပဖို႔ Guaido ပန္ၾကား 04 မတ္၊ 2019

https://gdb.voanews.com/231A05B2-BA18-48F4-9A7C-A4A892CAFD25_w650_r1_s.jpg


ဗင္နီဇြဲလားျပည္သူေတြ တနလၤာေန႔ ဆႏၵျပဖို႔ Guaido ပန္ၾကား
04 မတ္၊ 2019

ဗြီအိုေအ (ျမန္မာပုိင္း)

ဗင္နီဇြဲလား အတိုက္အခံ ေခါင္းေဆာင္ Juan Guaido
ဗင္နီဇြဲလား အတိုက္အခံ ေခါင္းေဆာင္ Juan Guaido
မွ်ေ၀ပါ

ဗင္နီဇြဲလား အတိုက္အခံ ေခါင္းေဆာင္ Juan Guaido က လက္တင္ အေမရိက မဟာမိတ္ ႏုိင္ငံေတြကို သြားေရာက္ၿပီးေနာက္ ႏုိင္ငံကို ျပန္လာဖို႔ စီစဥ္ထားခ်ိန္နဲ႔ တၿပိဳင္တည္း ဒီကေန႔ တနလာၤေန႔မွာ ျပည္သူေတြ လမ္းမေပၚထြက္ၾကဖို႔ တိုက္တြန္းထားပါတယ္။ ႏုိင္ငံကို ျပန္လာမယ့္ အေၾကာင္း အသိေပးေၾကာင္း၊ ေနာက္ တနလာၤေန႔ မနက္ ၁၁ နာရီမွာ ဗင္နီဇြဲလား ျပည္သူေတြ ႏုိင္ငံတ၀န္းမွာ စုရံုးၾကဖို႔ တိုက္တြန္းတယ္လို႔ Guaido က တြစ္တာ လူမႈကြန္ယက္မွာ ေရးသားထားတာပါ။




ႏိုင္ငံေပါင္း ၅၀ နဲ႔ အေမရိကန္တို႔က ဗင္နီဇြဲလားရဲ႕ ယာယီေခါင္းေဆာင္ အျဖစ္ အသိအမွတ္ျပဳထားတဲ႔ Guaido ဟာ လႊတ္ေတာ္ဥကၠဌ ျဖစ္ပါတယ္။ အေျခခံ ဥပေဒကို က်င့္သံုးႏုိင္တဲ႔ သူ႔ရဲ႕ အခြင့္အာဏာကို သံုးၿပီး လႊတ္ေတာ္ အႀကီးအကဲ Guaido က သမၼတ Nicolas Maduro ေခါင္းေဆာင္မႈကို ေရြးေကာက္ပြဲ မသမာမႈေတြေၾကာင့္ ဆိုၿပီး တရားမ၀င္အျဖစ္ ေၾကညာၿပီး သူ႔ကိုယ္သူ ၾကားျဖတ္သမၼတ အျဖစ္ ေၾကညာခဲ႔တာပါ။

Maduro ႏုတ္ထြက္ေရး ဖိအား တိုးေပးႏိုင္ေရး အတြက္ လက္တင္ အေမရိကတိုက္ ႏုိင္ငံေတြကို ခရီးသြားေနတဲ႔ Guaido က ၿပီးခဲ႔တဲ႔ စေနေန႔ တုန္းကေတာ့ အီေကြေဒါ ႏုိင္ငံမွာ ေရာက္ေနပါတယ္။ ၿပီးခဲ႔တဲ႔ သီတင္းပတ္ကေတာ့ အေမရိကန္ ဒုတိယ သမၼတ Mike Pence ၊ ေနာက္ ေဒသတြင္း ေခါင္းေဆာင္ေတြနဲ႔ ေတြ႔ဆံုခဲ႔ၿပီးေနာက္ အေမရိကန္ အသိအမွတ္ျပဳထားတဲ႔ ဗင္နီဇြဲလား ၾကားျဖတ္ သမၼတက ဘရာဇီလ္းနဲ႔ Prague ႏုိင္ငံေတြကို သြားေရာက္ခဲ႔ပါတယ္။