state Fleming's left hand rule
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Fleming's left hand rule is used to determine the direction of force exerted on a current carrying wire placed in a magnetic field.
Fleming's left-hand rule states that “When a current-carrying conductor is placed in an external magnetic field, the conductor experiences a force perpendicular to both the field and to the direction of the current flow.” It was invented by John Ambrose Fleming.
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state Fleming's left hand rule
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sᴛᴀᴛᴇ ғʟᴇᴍɪɴɢ's ʟᴇғᴛ-ʜᴀɴᴅ ʀᴜʟᴇ
ғʟᴇᴍɪɴɢ's ʟᴇғᴛ-ʜᴀɴᴅ ʀᴜʟᴇ sᴛᴀᴛᴇs ᴛʜᴀᴛ “ᴡʜᴇɴ ᴀ ᴄᴜʀʀᴇɴᴛ-ᴄᴀʀʀʏɪɴɢ ᴄᴏɴᴅᴜᴄᴛᴏʀ ɪs ᴘʟᴀᴄᴇᴅ ɪɴ ᴀɴ ᴇxᴛᴇʀɴᴀʟ ᴍᴀɢɴᴇᴛɪᴄ ғɪᴇʟᴅ, ᴛʜᴇ ᴄᴏɴᴅᴜᴄᴛᴏʀ ᴇxᴘᴇʀɪᴇɴᴄᴇs ᴀ ғᴏʀᴄᴇ ᴘᴇʀᴘᴇɴᴅɪᴄᴜʟᴀʀ ᴛᴏ ʙᴏᴛʜ ᴛʜᴇ ғɪᴇʟᴅ ᴀɴᴅ ᴛᴏ ᴛʜᴇ ᴅɪʀᴇᴄᴛɪᴏɴ ᴏғ ᴛʜᴇ ᴄᴜʀʀᴇɴᴛ ғʟᴏᴡ.” ɪᴛ ᴡᴀs ɪɴᴠᴇɴᴛᴇᴅ ʙʏ ᴊᴏʜɴ ᴀᴍʙʀᴏsᴇ ғʟᴇᴍɪɴɢ.
ғʟᴇᴍɪɴɢ's ʟᴇғᴛ-ʜᴀɴᴅ ʀᴜʟᴇ ғᴏʀ ᴇʟᴇᴄᴛʀɪᴄ ᴍᴏᴛᴏʀs ɪs ᴏɴᴇ ᴏғ ᴀ ᴘᴀɪʀ ᴏғ ᴠɪsᴜᴀʟ ᴍɴᴇᴍᴏɴɪᴄs, ᴛʜᴇ ᴏᴛʜᴇʀ ʙᴇɪɴɢ ғʟᴇᴍɪɴɢ's ʀɪɢʜᴛ-ʜᴀɴᴅ ʀᴜʟᴇ[1] (ғᴏʀ ɢᴇɴᴇʀᴀᴛᴏʀs). ᴛʜᴇʏ ᴡᴇʀᴇ ᴏʀɪɢɪɴᴀᴛᴇᴅ ʙʏ ᴊᴏʜɴ ᴀᴍʙʀᴏsᴇ ғʟᴇᴍɪɴɢ, ɪɴ ᴛʜᴇ ʟᴀᴛᴇ 19ᴛʜ ᴄᴇɴᴛᴜʀʏ, ᴀs ᴀ sɪᴍᴘʟᴇ ᴡᴀʏ ᴏғ ᴡᴏʀᴋɪɴɢ ᴏᴜᴛ ᴛʜᴇ ᴅɪʀᴇᴄᴛɪᴏɴ ᴏғ ᴍᴏᴛɪᴏɴ ɪɴ ᴀɴ ᴇʟᴇᴄᴛʀɪᴄ ᴍᴏᴛᴏʀ, ᴏʀ ᴛʜᴇ ᴅɪʀᴇᴄᴛɪᴏɴ ᴏғ ᴇʟᴇᴄᴛʀɪᴄ ᴄᴜʀʀᴇɴᴛ ɪɴ ᴀɴ ᴇʟᴇᴄᴛʀɪᴄ ɢᴇɴᴇʀᴀᴛᴏʀ.
ᴡʜᴇɴ ᴄᴜʀʀᴇɴᴛ ғʟᴏᴡs ᴛʜʀᴏᴜɢʜ ᴀ ᴄᴏɴᴅᴜᴄᴛɪɴɢ ᴡɪʀᴇ, ᴀɴᴅ ᴀɴ ᴇxᴛᴇʀɴᴀʟ ᴍᴀɢɴᴇᴛɪᴄ ғɪᴇʟᴅ ɪs ᴀᴘᴘʟɪᴇᴅ ᴀᴄʀᴏss ᴛʜᴀᴛ ғʟᴏᴡ, ᴛʜᴇ ᴄᴏɴᴅᴜᴄᴛɪɴɢ ᴡɪʀᴇ ᴇxᴘᴇʀɪᴇɴᴄᴇs ᴀ ғᴏʀᴄᴇ ᴘᴇʀᴘᴇɴᴅɪᴄᴜʟᴀʀ ʙᴏᴛʜ ᴛᴏ ᴛʜᴀᴛ ғɪᴇʟᴅ ᴀɴᴅ ᴛᴏ ᴛʜᴇ ᴅɪʀᴇᴄᴛɪᴏɴ ᴏғ ᴛʜᴇ ᴄᴜʀʀᴇɴᴛ ғʟᴏᴡ (ɪ.ᴇ ᴛʜᴇʏ ᴀʀᴇ ᴍᴜᴛᴜᴀʟʟʏ ᴘᴇʀᴘᴇɴᴅɪᴄᴜʟᴀʀ). ᴀ ʟᴇғᴛ ʜᴀɴᴅ ᴄᴀɴ ʙᴇ ʜᴇʟᴅ, ᴀs sʜᴏᴡɴ ɪɴ ᴛʜᴇ ɪʟʟᴜsᴛʀᴀᴛɪᴏɴ, sᴏ ᴀs ᴛᴏ ʀᴇᴘʀᴇsᴇɴᴛ ᴛʜʀᴇᴇ ᴍᴜᴛᴜᴀʟʟʏ ᴏʀᴛʜᴏɢᴏɴᴀʟ ᴀxᴇs ᴏɴ ᴛʜᴇ ᴛʜᴜᴍʙ, ғᴏʀᴇ ғɪɴɢᴇʀ ᴀɴᴅ ᴍɪᴅᴅʟᴇ ғɪɴɢᴇʀ. ᴇᴀᴄʜ ғɪɴɢᴇʀ ɪs ᴛʜᴇɴ ᴀssɪɢɴᴇᴅ ᴛᴏ ᴀ ϙᴜᴀɴᴛɪᴛʏ (ᴍᴇᴄʜᴀɴɪᴄᴀʟ ғᴏʀᴄᴇ, ᴍᴀɢɴᴇᴛɪᴄ ғɪᴇʟᴅ ᴀɴᴅ ᴇʟᴇᴄᴛʀɪᴄ ᴄᴜʀʀᴇɴᴛ). ᴛʜᴇ ʀɪɢʜᴛ ᴀɴᴅ ʟᴇғᴛ ʜᴀɴᴅ ᴀʀᴇ ᴜsᴇᴅ ғᴏʀ ɢᴇɴᴇʀᴀᴛᴏʀs ᴀɴᴅ ᴍᴏᴛᴏʀs ʀᴇsᴘᴇᴄᴛɪᴠᴇʟʏ.
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