A Treatise on Magnetism Designed for the Use of Students in the University |
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Page ix
... momentum impressed on the disturbed magnet . Attractions will be represented in the diagrams by con- tinuous lines , repulsions by interrupted lines · . 15. In the same arrangement , to find the tendency of the action of A to produce a ...
... momentum impressed on the disturbed magnet . Attractions will be represented in the diagrams by con- tinuous lines , repulsions by interrupted lines · . 15. In the same arrangement , to find the tendency of the action of A to produce a ...
Page 24
... momentum impressed on the disturbed magnet . Attractions will be represented in the diagrams by continuous lines , repulsions by interrupted lines . In Figure 9 , suppose that we require the angular Fig . 9 . B momentum which A produces ...
... momentum impressed on the disturbed magnet . Attractions will be represented in the diagrams by continuous lines , repulsions by interrupted lines . In Figure 9 , suppose that we require the angular Fig . 9 . B momentum which A produces ...
Page 25
Sir George Biddell Airy. Fig . 9 . B momentum which A produces on B. The continuous lines denote attraction ; the inter- rupted lines ... momentum which they impress on B is -m- a2 b2 -m - 1 2 243 x ab DISTURBING MAGNET BROADSIDE - ON . 25.
Sir George Biddell Airy. Fig . 9 . B momentum which A produces on B. The continuous lines denote attraction ; the inter- rupted lines ... momentum which they impress on B is -m- a2 b2 -m - 1 2 243 x ab DISTURBING MAGNET BROADSIDE - ON . 25.
Page 26
... momentum obtain- ed from the action of the two poles of A upon the blue pole of B is -m - 1 2b b2 2 24β x ab . -m - 1 x ( 1 + 25+ 2 + 1 ) + ( 1 > с c2 in the same direction as the former . And the whole angular momentum , opposite to ...
... momentum obtain- ed from the action of the two poles of A upon the blue pole of B is -m - 1 2b b2 2 24β x ab . -m - 1 x ( 1 + 25+ 2 + 1 ) + ( 1 > с c2 in the same direction as the former . And the whole angular momentum , opposite to ...
Page 27
... momentum = 2a , ß × ab × [ 2cm − 1 + ( m + 1 ) .c ̄m − 3 { − a2 + ( m + 2 ) . b2 } ] , -m - 3 or = 4aß × ab × [ cm − 1 + m + 1 2 - . cm - 3 { — a23 + ( m + 2 ) .b2 } ] . 15. In the same arrangement , to find the tendency of the ...
... momentum = 2a , ß × ab × [ 2cm − 1 + ( m + 1 ) .c ̄m − 3 { − a2 + ( m + 2 ) . b2 } ] , -m - 3 or = 4aß × ab × [ cm − 1 + m + 1 2 - . cm - 3 { — a23 + ( m + 2 ) .b2 } ] . 15. In the same arrangement , to find the tendency of the ...
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Common terms and phrases
angle angular momentum Astronomical Meridian attraction axis azimuth blue end blue magnetism blue pole broadside-on C₁ Cambridge cloth College compass compass-needle cotan Crown 8vo curves deflexion deviation direction distance disturbed needle disturbing magnet Edition effect elementary end-on equal equations error experiment expression fcap Figure formulæ Greenwich horizontal action horizontal plane investigations latitude Law of Magnetism longitude magnet-power Magnetic Declination magnetic force magnetic meridian Magnetic Pole mass of iron measured moment of inertia netism North Magnetic Pole numerical value observations obtained opposite position produced proportion red end red magnetism red pole remarked represented repulsion rotation Royal Observatory sensibly ship ship's head statical force exerted steel magnet supposed suspension-thread term terrestrial horizontal force terrestrial magnetism theodolite theory tion torsion-power total force treatise vertical force vibration wire
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