Electric field

ELECTRIC FIELD

The concept of the electric field was introduced by Michael Faraday. An electric field is created by a charged body in the space that surrounds it, and results in a force exerted on any other charges placed within the field. The electric field acts between two charges in a similar manner to the way that the gravitational field acts between two masses, and like it, extendsΒ  towards infinity and shows an inverse square relationship with distance. However, there is an important difference. Gravity always acts in attraction, drawing two masses together, while the electric field can result in either attraction or repulsion. Since large bodies such as planets generally carry no net charge, the electric field at a distance is usually zero. Thus gravity is the dominant force at distance in the universe, despite being much weaker. An electric field generally varies in space, and its strength at any one point is defined as the force (per unit charge) that would be felt by a stationary, negligible charge if placed at that point. As the electric field is defined in terms of force, and force is a vector, so it follows that an electric field is also a vector, having both magnitude and direction. Specifically, it is a vector field.1000 The study of electric fields created by stationary charges is called electrostatics. The field may be visualized by a set of imaginary lines whose direction at any 117point is the same as that of the field. This concept was introduced by Faraday, whose term 'lines of force' still sometimes sees use. The field lines are the paths that a point positive charge would seek to make as it was forced to move within the field; they are however an imaginary concept with no physical existence and the field permeates all the intervening space between the lines. Field lines emanating from stationary charges have several key properties: first, that they originate at positive charges and terminate at negative charges; second, that they must enter any good conductor at right angles, and third, that they may never cross nor close in on themselves.Β  The principles of electrostatics are important when designing items of high-voltage equipment. There is a finite limit to the electric field strength that may withstood by any medium. Beyond this point, electrical breakdown occurs and an electric arc causes flashover between the charged parts. Air, for example, tends to arc at electric field strengths which exceed 30 kV per centimetre (ΠΊΠ’/см) across small gaps. Over larger gaps, its breakdown strength is weaker, perhaps 1 kV per centimetre. 2000The most visible natural occurrence of this is lightning, caused when charge becomes separated in the clouds by rising columns of air, and raises the electric field in the air to greater than it can withstand. The voltage of a large lightning cloud may be as high as 100 MV and have discharge energies as great as 250 kWh. The field strength is greatly affected by nearby conducting objects, and it is particularly intense when it is forced to curve around sharply pointed objects. This principle is exploited in the lightning conductor, the sharp spike of which acts to encourage the lightning stroke to develop there, rather than to the building it serves to protect.Β  An electric field is zero inside a conductor. This is because the net charge on a conductor only exists on the surface. External electrostatic fields are always perpendicular to the conductors surface. Otherwise this would produce a force on the charge carriers inside the conductor and so the field would not be static as we assume.Β 
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ΠŸΠΎΠ½ΡΡ‚ΠΈΠ΅ элСктричСского поля Π±Ρ‹Π»ΠΎ Π²Π²Π΅Π΄Π΅Π½ΠΎΒ ΠœΠ°ΠΉΠΊΠ»ΠΎΠΌΒ Π€Π°Ρ€Π°Π΄Π΅Π΅ΠΌ. ЭлСктричСскоС полС создано заряТСнным Ρ‚Π΅Π»ΠΎΠΌ Π² космосС, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ ΠΎΠΊΡ€ΡƒΠΆΠ°Π΅Ρ‚ Π΅Π³ΠΎ, ΠΈ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ силС, проявлСнной ΠΏΠΎ Π»ΡŽΠ±Ρ‹ΠΌ Π΄Ρ€ΡƒΠ³ΠΈΠΌ обвинСниям, ΠΏΠΎΠΌΠ΅Ρ‰Π΅Π½Π½Ρ‹ΠΌ Π² области. ЭлСктричСскоС ΠΏΠΎΠ»Π΅ дСйствуСт ΠΌΠ΅ΠΆΠ΄Ρƒ двумя обвинСниями ΠΏΠΎΠ΄ΠΎΠ±Π½Ρ‹ΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ ΠΊ ΠΏΡƒΡ‚ΠΈ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ дСйствия поля тяготСния ΠΌΠ΅ΠΆΠ΄Ρƒ двумя массами, ΠΈ ΠΊΠ°ΠΊ ΠΎΠ½ΠΎ, простираСтся ΠΊ бСсконСчности ΠΈ ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°Π΅Ρ‚ ΠΎΠ±Ρ€Π°Ρ‚Π½Ρ‹Π΅ ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚Π½Ρ‹Π΅ ΠΎΡ‚Π½ΠΎΡˆΠ΅Π½ΠΈΡ с расстояниСм. Однако, Π΅ΡΡ‚ΡŒ Π²Π°ΠΆΠ½ΠΎΠ΅ Ρ€Π°Π·Π»ΠΈΡ‡ΠΈΠ΅. Π‘ΠΈΠ»Π° тяТСсти всСгда дСйствуСт Π² ΠΏΡ€ΠΈΠ²Π»Π΅ΠΊΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ, соСдиняя Π΄Π²Π΅ массы, Π² Ρ‚ΠΎ врСмя ΠΊΠ°ΠΊ элСктричСскоС ΠΏΠΎΠ»Π΅ ΠΌΠΎΠΆΠ΅Ρ‚ привСсти ΠΈΠ»ΠΈ ΠΊ ΠΏΡ€ΠΈΠ²Π»Π΅ΠΊΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ ΠΈΠ»ΠΈ ΠΊ ΠΎΡ‚Π²Ρ€Π°Ρ‰Π΅Π½ΠΈΡŽ. Π’Π°ΠΊ ΠΊΠ°ΠΊ большиС Ρ‚Π΅Π»Π°, Ρ‚Π°ΠΊΠΈΠ΅ ΠΊΠ°ΠΊ ΠΏΠ»Π°Π½Π΅Ρ‚Ρ‹ Π²ΠΎΠΎΠ±Ρ‰Π΅ Π½Π΅ нСсут чистого обвинСния, элСктричСскоС ΠΏΠΎΠ»Π΅ Π½Π° расстоянии ΠΎΠ±Ρ‹Ρ‡Π½ΠΎ - ноль. Π’Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ сила тяТСсти - Π΄ΠΎΠΌΠΈΠ½ΠΈΡ€ΡƒΡŽΡ‰Π°Ρ сила Π½Π° расстоянии Π²ΠΎ всСлСнной, нСсмотря Π½Π° Ρ‚ΠΎ, Ρ‡Ρ‚ΠΎΠ±Ρ‹ Π±Ρ‹Ρ‚ΡŒ Π½Π°ΠΌΠ½ΠΎΠ³ΠΎ Π±ΠΎΠ»Π΅Π΅ слабым. ЭлСктричСскоС ΠΏΠΎΠ»Π΅ Π²ΠΎΠΎΠ±Ρ‰Π΅ измСняСтся ΠΏΠΎ пространству, ΠΈ Π΅Π³ΠΎ сила Π² любом ΠΏΡƒΠ½ΠΊΡ‚Π΅ ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Π° ΠΊΠ°ΠΊ сила (Π·Π° ΠΎΠ±Π²ΠΈΠ½Π΅Π½ΠΈΠ΅ Π² Ρ€Π°Π·Π΄Π΅Π»Π΅), ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ чувствовало Π±Ρ‹ постоянноС, Π½Π΅Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ΅ ΠΎΠ±Π²ΠΈΠ½Π΅Π½ΠΈΠ΅ Ссли ΠΏΠΎΠΌΠ΅Ρ‰Π΅Π½ΠΎ Π² Ρ‚ΠΎΡ‚ ΠΏΡƒΠ½ΠΊΡ‚. ΠŸΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ элСктричСскоС ΠΏΠΎΠ»Π΅ ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΎ с Ρ‚ΠΎΡ‡ΠΊΠΈ зрСния силы, ΠΈ сила - Π²Π΅ΠΊΡ‚ΠΎΡ€, Ρ‚Π°ΠΊ, ΠΈΠ· этого слСдуСт, Ρ‡Ρ‚ΠΎ элСктричСскоС ΠΏΠΎΠ»Π΅ - Ρ‚Π°ΠΊΠΆΠ΅ Π²Π΅ΠΊΡ‚ΠΎΡ€, имСя ΠΈ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρƒ ΠΈ руководство. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Π½ΠΎ, это - вСкторная ΠΎΠ±Π»Π°ΡΡ‚ΡŒ. ИсслСдованиС элСктричСских ΠΏΠΎΠ»Π΅ΠΉ, созданных постоянными обвинСниями, Π½Π°Π·Ρ‹Π²Π°ΡŽΡ‚ electrostatics. ΠžΠ±Π»Π°ΡΡ‚ΡŒ ΠΌΠΎΠΆΠ΅Ρ‚ Π²ΠΈΠ·ΡƒΠ°Π»ΠΈΠ·ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒΡΡ рядом Π²ΠΎΠΎΠ±Ρ€Π°ΠΆΠ°Π΅ΠΌΡ‹Ρ… Π»ΠΈΠ½ΠΈΠΉ, руководство ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π² любом 117point являСтся Ρ‚Π΅ΠΌ ΠΆΠ΅ самым ΠΊΠ°ΠΊ Ρ‚ΠΎΠΉ ΠΈΠ· области. Π­Ρ‚ΠΎ понятиС Π±Ρ‹Π»ΠΎ Π²Π²Π΅Π΄Π΅Π½ΠΎ Π€Π°Ρ€Π°Π΄Π΅Π΅ΠΌ, Ρ‚Π΅Ρ€ΠΌΠΈΠ½ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ 'Π»ΠΈΠ½ΠΈΠΈ силы' всС Π΅Ρ‰Π΅ ΠΈΠ½ΠΎΠ³Π΄Π° Π²ΠΈΠ΄ΠΈΡ‚ использованиС. ΠŸΠΎΠ»Π΅Π²Ρ‹Π΅ Π»ΠΈΠ½ΠΈΠΈ - ΠΏΡƒΡ‚ΠΈ, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ заряд ΠΏΡƒΠ½ΠΊΡ‚Π° стрСмился Π±Ρ‹ ΡΠ΄Π΅Π»Π°Ρ‚ΡŒ, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ ΠΎΠ½ Π±Ρ‹Π» Π²Ρ‹Π½ΡƒΠΆΠ΄Π΅Π½ ΠΏΠ΅Ρ€Π΅ΠΌΠ΅ΡΡ‚ΠΈΡ‚ΡŒΡΡ Π² области; ΠΎΠ½ΠΈ - ΠΎΠ΄Π½Π°ΠΊΠΎ Π²ΠΎΠΎΠ±Ρ€Π°ΠΆΠ°Π΅ΠΌΠΎΠ΅ понятиС Π±Π΅Π· физичСского сущСствования, ΠΈ ΠΎΠ±Π»Π°ΡΡ‚ΡŒ ΠΏΡ€ΠΎΠ½ΠΈΠΊΠ°Π΅Ρ‚ Π²ΠΎ всСм ΠΏΡ€ΠΎΡˆΠ΅Π΄ΡˆΠ΅ΠΌ пространствС ΠΌΠ΅ΠΆΠ΄Ρƒ линиями. Π£ ΠΏΠΎΠ»Π΅Π²Ρ‹Ρ… Π»ΠΈΠ½ΠΈΠΉ, происходящих ΠΎΡ‚ постоянных ΠΎΠ±Π²ΠΈΠ½Π΅Π½ΠΈΠΉ, Π΅ΡΡ‚ΡŒ нСсколько ΠΊΠ»ΡŽΡ‡Π΅Π²Ρ‹Ρ… свойств: Π²ΠΎ-ΠΏΠ΅Ρ€Π²Ρ‹Ρ…, Ρ‚ΠΎ, Ρ‡Ρ‚ΠΎ ΠΎΠ½ΠΈ происходят Π² ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… зарядах ΠΈ ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹ΠΉ Π² ΠΎΡ‚Ρ€ΠΈΡ†Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… зарядах; Π²ΠΎ-Π²Ρ‚ΠΎΡ€Ρ‹Ρ…, Ρ‚ΠΎ, Ρ‡Ρ‚ΠΎ ΠΎΠ½ΠΈ Π΄ΠΎΠ»ΠΆΠ½Ρ‹ Π²ΠΎΠΉΡ‚ΠΈ Π² любого Ρ…ΠΎΡ€ΠΎΡˆΠ΅Π³ΠΎ ΠΏΡ€ΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠ° ΠΏΠΎΠ΄ прямым ΡƒΠ³Π»ΠΎΠΌ, ΠΈ Π²-Ρ‚Ρ€Π΅Ρ‚ΡŒΠΈΡ…, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ ΠΎΠ½ΠΈ Π½ΠΈΠΊΠΎΠ³Π΄Π°, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ, Π½Π΅ ΠΏΠ΅Ρ€Π΅ΡΠ΅ΠΊΠ°ΡŽΡ‚, Π½ΠΈ ΠΏΡ€ΠΈΠ±Π»ΠΈΠΆΠ°ΡŽΡ‚ΡΡ ΡΠ°ΠΌΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½ΠΎ. ΠŸΡ€ΠΈΠ½Ρ†ΠΈΠΏΡ‹ electrostatics Π²Π°ΠΆΠ½Ρ‹, проСктируя ΠΏΡƒΠ½ΠΊΡ‚Ρ‹ оборудования высокого напряТСния. Π•ΡΡ‚ΡŒ ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹ΠΉ ΠΏΡ€Π΅Π΄Π΅Π» силС элСктричСского поля, которая ΠΌΠΎΠΆΠ΅Ρ‚ ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΡΡ‚ΠΎΡΠ²ΡˆΠΈΠΉ любой срСдой. Π’Π½Π΅ этого ΠΏΡƒΠ½ΠΊΡ‚Π° происходит элСктричСскоС расстройство, ΠΈ элСктричСская Π΄ΡƒΠ³Π° Π²Ρ‹Π·Ρ‹Π²Π°Π΅Ρ‚ flashover ΠΌΠ΅ΠΆΠ΄Ρƒ заряТСнными частями. Π’ΠΎΠ·Π΄ΡƒΡ…, Π½Π°ΠΏΡ€ΠΈΠΌΠ΅Ρ€, ΠΈΠΌΠ΅Π΅Ρ‚ Ρ‚Π΅Π½Π΄Π΅Π½Ρ†ΠΈΡŽ ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Ρ‹Π²Π°Ρ‚ΡŒ Π΄ΡƒΠ³Ρƒ Π² силах элСктричСского поля, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΡ€Π΅Π²Ρ‹ΡˆΠ°ΡŽΡ‚ 30 ΠΊΠ’ Π·Π° сантимСтр (ΠΊΠ’/см) Ρ‡Π΅Ρ€Π΅Π· малСнькиС пропуски. По большим пропускам Π΅Π³ΠΎ элСктричСская ΠΏΡ€ΠΎΡ‡Π½ΠΎΡΡ‚ΡŒ Π±ΠΎΠ»Π΅Π΅ слаба, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎ 1 ΠΊΠ’ Π·Π° сантимСтр.

Electric field