% dr. dm d 2 r dt 2 = F g + F P,t + F P,b !"#$%&'()*+(,-%&'./'0(/1(2%#'0( !"#$%&'()*+(,-%&'./'0(/1(2%#'0( !"#$%&'()*+(,-%&'.
|
|
- Edmund Black
- 5 years ago
- Views:
Transcription
1 /-.3&'(#(456.-3'.4#6(7/689&(/(:#(.-(%&( #%9/$&'&(/(#(%#'(;.%(8'#4&(#'&#<(<(#%(#( '#3.8('/9(4&-%&'(/(%#'<('<(6&-:%(3'<#-3(;.%( 3&-.%5<(+( dm d 2 r dt 2 F g + F P,t + F P,b >-65(/'4&(#4?-:(/-(456.-3&'(#'&(:'#7.%5(#-3( $'&8'&(@;.4(.(#6;#5(-/'9#6(%/(%&(8'#4&A( F P,t ( F P,b + df P ) P F A df P A F G G M rdm dm d 2 r dt G M rdm A 2 E/'4&(#%(%&(%/$(&F8#6(%&(/'4&(#%(%&(D/G/9( #-3(#(4/''&4?/-(%&'9(%#%(#44/8-%(/'(%&( '&384?/-(.-(%&('#3.#6(3.'&4?/-H( I'#7.%#?/-#6(/'4&( #$%&$'()*%+,-./$2324*25( dm Adr Adr d 2 r dt GA M dr r A 2 *( d 2 r dt G M r 2 dr dr G M r g J53'/%#?4(&F8.6.D'.89(K( #44&6&'#?/-(.(L&'/( MF-(/(53'/%#?4(&F8.6.D'.89(K(.-(/'3&'( /'(#(%#'(%/(D&(%#?4<(%&'&(98%(&C.%(#( $'&8'&(:'#3.&-%(%#%(D#6#-4&(:'#7.%5H( B'&8'&(.-4'&#&(;.%(3&4'&#.-:('#3.8H( $+.5-,$,'$7*++*$-,$,'$/#,*$%&$-$+,-*$%&$%#$ 9 :;< $%#$> :;< $)#+2,($?@?A$BC$5 DE F$ dr P s P c R s P c R s P c G M s# s R s 2.7 $ 4 Nm 2 P c R % c GM P c r #(r) % dr P s R s N/8:(&?9#%&(/(4&-%'#6( $'&8'&( O/'&('.:/'/8(4#6486#?/-(3&9#-3( 8-4?/-#6(/'9(/'(O ' (#-3(@'A<(-/%( :&-&'#665(#7#.6#D6&H( /9$8%&'(9/3&6.-:(5.&63(#(4&-%'#6( $'&8'&(/+(( PHQR(C()* )S (T9 KP (U(PHQ(C()* )) (#%9((
2 #$%&$5-++$/%#+*G-.%#( 2$&'.4#665(599&%'.4#6(&66(/(9#(3O<(;.%(%.4V-&(3'<(#%( 3.%#-4&('('/9(%&(4&-%&'(/(%&(%#'+( dm r ( 4 dr) H*++*$#$%&$+,-,( O#4'/4/$.4($'&8'&(4/9&('/9(%&(&F8#?/-(/(%#%&(/( %&(9#%&'.#6(@.3(:#(6#;AH( PV NkT dm r dr 4 r2 O#(4/-&'7#?/-( &F8#?/-( W.4%#%&(/;(%&(.-%&'./'(9#(/(#(%#'( 98%(4#-:&(;.%(3.%#-4&('/9(%&( 4&-%&'H( V N k T X/689&( T89D&'(/($#'?46&( Y/6%L9#--Z(4/-%#-%( [&9$&'#%8'&( H*++*$#$%&$+,-,( H*++*$#$%&$+,-,( /-.3&'(:#(4/-%#.-&3(.-(#(456.-3&'(/( 6&-:%(C(;.%($#'?46&(7&6/4.?&(7 C ( f ma dp dt ft p 2p xˆ i t 2 x v x f 2p x t p xv x x &(U(E/'4&($&'($#'?46&(,9$86&('/9( 4/66../-( [.9&(D&%;&&-(4/66../-( f p xv x x p x v x v 2 v x 2 + v y 2 + v z 2 v x 2 v y 2 v z 2 v 2 p x v x 3 pv O/9&-%89($'/$/'?/-#6(%/( 7&6/4.%5( 3 2$&&3(.(%&(F8#3'#%8'&(89( /(7&6/4.?&(.-((3.'&4?/-( T/($'&&''&3(7&6/4.%5( 3.'&4?/-( [&($'/384%(/(9/9&-%89(#-3( 7&6/4.%5(.-(%&(C(3.'&4?/-(.()\Q( %&(%/%#6(7&4%/'($'/384%(
3 H*++*$#$%&$+,-,( f ( p) p v 3 x N # N p dp H*++*$#$%&$+,-,( W.7.3&(D/%(.3&(D5(#'&#+( F A 3 # N p Ax v pdp df( p) f (p)n p dp 3 N p x pvdp n p dp N p V dp T89D&'(/($#'?46&(;.%( 9/9&-%89($($&'(8-.%(7/689&( [/%#6(/'4&(&C&'%&3(D5( $#'?46&(4/66../-+( F 3 # N p x pvdp B'&8'&(.-%&:'#6( P # n p pvdp 3 #6486#%&($'&8'&<(:.7&-(%&(3.%'.D8?/-( 8-4?/-<(- $ 3$( I-+$7*++*$-#)$9-#$9%3/3-*$ J2C',( pdp mv 2 dv P n v mv 2 dv 3 28D?%8?-:(.-%/(%&($'&8'&(.-%&:'#6( I-+$H*++*$-#)$9-#$9%3/3-*$ J2C',( P g nkt kt µ m H I#($'&8'&(.H%H/H(9&#-( 9/6&486#'(;&.:%( n v dv n p dp $ m ' n v dv n& ) % 2#kT ( n ndv 3 / 2 e *mv 2 / 2kT 4# 2 dv B#'?46&(-89D&'(3.%'.D8?/-( O#C;&66KY/6%L9#--(7&6/4.%5( 3.%'.D8?/-( 2.-4&+( n m µ m m H O&#-(9/6&486#'(;&.:%(
4 9-#$9%3/3-*$J2C',( K%*$-$/%573,3($#,*-3$C-+8( O&#-(9/6&486#'(;&.:%(3&$&-3(/-(4/9$/.?/-(/( &F8#?/-AH(( E'&&(&6&4%'/-(98%(D&(.-4683&3(.-(%&(#7&'#:&(9#( $&'($#'?46&H( m n N m N m n µ n N m N N A N A m m H µ m /m H #$%&'()$*+#$#,'$-(..$ /&(2$/&$'(,$3(&4'$ K%*$-$/%573,3($#,*-3$C-+8( K%*$-$/%573,3($#,*-3$C-+8( µ i N A N ( + z ) )]L^(#44/8-%(/'(%&(-846&8($68(%&(-89D&'(/( '&&(&6&4%'/-(%#%('&86%('/9(4/9$6&%&65(./-.L.-:(#-(#%/9(/(%5$&(^H( µ n m H N N m number particles from mass particle from :(/7&'($#'?46&(;.%( 3._&'&-%(9#&( mass particle from total mass of gas µ n m H N N m,-7&'%(%&(&c$'&./-(/'(#7&'#:&($#'?46&(9#( #-3('&;'.%&((.-(%&'9(/(%&(9#('#4?/-H( N N A m H A m H X X L M $.(%&(9#('#4?/-(/(#%/9( /(%5$&(M( %/%#6(-89D&'(/($#'?46&( ((((%/%#6(9#(/(:#( µ n X A µ n X + 4 Y + A n Z ;&.:%&3(#7&'#:&(/(#66(&6&9&-%(.-(:#( .&'(%#-(53'/:&-(#-3(&6.89H(
5 K%*$-#$2%#2N)$C-+8( µ i + z A X 2X + 3 µ i 4 Y + + z A i Z E/'(&6&9&-%(.&'(%#%(J(#-3(J&+( [/%#6(-89D&'(/($#'?46&(.-4683&3+(/-(J( 4/-%'.D8%&()(&6&4%'/-($68(-846&8<(/-&(J&( 4/-%'.D8%&(P(&6&4%'/-($68(-846&8( + z A i 2 >G2O8( dr G M r g P n p pvdp 3 P g nkt kt µ m H dm r dr 4 r2 µ m m H µ n X + 4 Y + A n Z 2X + 3 µ i 4 Y + + z Z + z A i A i 2 O&#-(9/6&486#'(;&.:%(@-&8%'#6( :#A(( B'&8'&(,-%&:'#6( O#(4/-&'7#?/-(&F-( O&#-(9/6&486#'(;&.:%(@/'( 4/9$6&%&65(./-.L&3(:#A( O&#-(9/6&486#'(;&.:%( I#($'&8'&(&F-( MF-(/(53'/%#?4(&F8.6.D'.89( PG*-C$#*C($7*$7-*./38( K*52DQ2*-/$G+$R%+D2#+,2#( nkt mn v v 2 dv 3 n n v v 2 dv 3kT m v 2 3kT 2 2 mv kt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
6 >-)2-.%#$H*++*( P rad 3 u 3 at 4 >-)2-.%#$H*++*( T/;<(4&4V(%/(&&(;&%&'(.%(;#('&#/-#D6&(%/(-&:6&4%('#3.#?/-( $'&8'&(.-(%&(4/'&(;.%(/8'(3&'.7&3(4/'&(%&9$&'#%8'&+(( P tot kt µm H + 3 at 4 [/%#6($'&8'&(38&(%/(:#( #-3('#3.#?/-(( P tot kt µm H + 3 at 4 #6486#%&(%&(%&9$&'#%8'&(.-(%&(4/'&(/(%&(28-H(,:-/'&('#3.#?/-($'&8'&+( P rad.53 3 Nm #2.65% P gas T c P cµm H k.44 # 7 K 2%#-3#'3(/6#'(9/3&6+( [ 4/'& U)H`aC)* a b( sun 4kg m 3 µ ioninzed.62 P central 2.34 # 6 Nm 2 29#66(4/-%'.D8?/-('/9('#3.#?/-($'&8'&<(/( %#%(#89$?/-(;#('&#/-#D6&H( :,33-*$#*C($+%*/+( :,33-*$#*C($:%*/+( I'#7.%#?/-#6(B/%&-?#6(M-&':5+( U G Mm r E'/9(%&(X.'.#6(%&/'&9(@MF-(PHRa(.-(5/8'(D//VA<(#6(/(%&(4#-:&(.-(:'#7.%#?/-#6(BHMH(.(#7#.6#D6&(%/(D&('#3.#%&3(#;#5(K(%&(/%&'(#6( 8$$6.&(%&'9#6(&-&':5(%#%(&#%(%&(%#'H((( [&(:'#7.%#?/-#6(/'4&(/-(#($#'?46&(/(9#()5 2 (/8%.3&(#( $&'.4#665(599&%'.4(9#<(9(.+((( df g,i G M rdm i du g,i G M rdm i r G M r 4 # dr r R U grav 4G $ M r # rdr # ~ # M 4 3 R3 M R ~ 4 3 r3 # U grav ~ G# 2 R 5 ~ 3 GM 2 5 R E ~ 3 GM 2 R [/%#6(:'#7.%#?/-#6(BHMH( 89&(4/-%#-%(3&-.%5(U(9&#-(3&-.%5( $$'/C.9#%&(%&(9#(.H%H/H(9&#-(3&-.%5( [&-<(&?9#%&(%&(:'#7.%#?/-#6(BHM(( E'/9(%&(X.'.#6(%&/'&9<(%&(%/%#6( 9&4#-.4#6(&-&':5(.(#6(%&( :'#7.%#?/-#6(BHMH(
7 (cc(n A<( /;(984(&-&':5(;/863(#7&(D&&-(6.D&'#%&3('/9(:'#7.%#?/-#6( 4/66#$&d(( E grav (E f E i ) # E f ~ 3 t KH E grav L sun ~ 7 yr 2 GM sun R sun ~.$ 4 J 89.-:(-&#'65(4/-%#-%(689.-/.%5<(/;(6/-:(4/863(%&( 8-(&9.%(&-&':5(#%(%.('#%&d( b&67.-kj&69/6%l(?9&4#6&(k(d#&3(/-('#3./#4?7&(./%/$&(3#?-:<(%&(9//-(#-3(9&%&/'.%&(#'&(/63&'( %#-(%.<(%&'&/'&(:'#7.%#?/-#6(4/-%'#4?/-(4#--/%( #44/8-%(/'(&-&':5(/8%$8%(/(%&(28-H( :,33-*$#*C($:%*/+( &9.4#6('?/-d( [5$.4#6(#9/8-%(/(&-&':5($&'(#%/9(-/%(6.V&65(%/(D&(9/'&(%#-()K)*(&XH(( I.7&-(%&(-89D&'(/(#%/9($'&&-%(.-(#(%#'<(%&(#9/8-%(/(4&9.4#6( &-&':5(.(#6/(#'(%//(6/;(%/(#44/8-%(/'(/6#'(689.-/.%5(/7&'(#('&#/-#D6&( $&'./3(/(?9&H(( M sun 2 3 kg M hydrogen.7 27 kg ~ 57 ev.6 8 J L sun W t E tot L sun T $#'?46& (@89&(8-(.()**e( 53'/:&-A( M-&':5($&'($#'?46&( f89.-/.%5(/(%&(8-( T/%(6/-:(&-/8:(%/(D&( 6*6 * 24 * 365 s/ yr 573 yr 4/-.%&-%(;.%(./%/$.4( 3#?-:(/(9//-(#-3( 9&%&/'.%&( </3-*$.5+/-3+( T846&#'('?/-($'/384&(&-&':5(@O&X($&'( 'C-A( </3-*$.5+/-3( 89&(%&(28-(;#(/'.:.-#665()**e(53'/:&-(#-3(/-65(%&(.--&'( )*e(/(%&(28-z(9#(d&4/9&(/%(&-/8:(%/(8&(53'/:&-(%/( &6.89H(J/;(984(-846&#'(&-&':5(.(#7#.6#D6&(.-(%&(28-d( E nuclear..7 M sun c J 2/9&(9#(.(4/-7&'%&3(.-%/(&-&':5(@MU94 P AH(E/'(( '?/-+( t nuclear E nuclear L sun ~ yr T846&#'(8./-($'/7.3&(#-(&-&':5(/8'4&( %#%(.(4/-.%&-%(;.%(689.-/.%5(/(%&( 8-(#-3(#:&(/(9//-(#-3(9&%&/'.%&H( 9(U(*H*PgSha@9&#-(9/6&486#'(;&.:%A( 9(U(*Hae(
8 S-#,5$9/'-#2/-3$T##32#C( N&4#66(%#%(%&(/-65(7.#D6&(/8'4&(/(&-&':5(%/($'/7.3&( /D&'7&3(%&66#'(689.-/.%5(/'($'&89&3(6.&?9&(/( %&(28-(.(-846&#'(8./-H(( 89&(%#%(&-&':5('&F8.'&3(%/(/7&'4/9&(/86/9D( $/%&-?#6(.(:.7&-(D5(%&'9#6(&-&':5+( 2 mv kt classical Z Z 2 e 2 4 r T classical Z Z 2 e2 6 kr # K J/;&7&'<(4#6486#%&3(%&9$&'#%8'&(/(/6#'(4/'&(.(/-65()* a b( S-#,5$9/'-#2/-3$T##32#C( M7&-(;.%(%&(OY(7&6(3.%'.D8?/-<(?66(-/%(&-/8:(&-&':5(%/(#7&( #(.:-.i4#-%(8./-('#%&h((j/;&7&'(o(%8--&6.-:(#66/;($#'?46&(%/( 9#V&(46/&'(#$$'/#4H(( M?9#%&(%&($#'?46&(;#7&6&-:%(#(%&(3&Y'/:6.&(;#7&6&-:%+(( 2 µ v 2 m p2 Z Z 2 e 2 2µ m 4 # 4 # h Z Z 2 e 2 2µ m T quantum Z 2 Z 2 2 e 4 µ m h 2 k $7 K ( h /#)2 2µ m 2/67&(/'(%&(3&Y'/:6.&(;#7&6&-:%(#-3( 8D?%8%&(/'('(.-(%&($'&7./8(&F8#?/-( h p </3-*$>6#$*-,+$-#)$,'$I-5%O$H-B( </3-*$/*%++$+/.%#( O/'&(4#'&86(4#6486#?/-+('C-('#%&($&'(&-&':5(.-%&'7#6(.-(%&'9( /(%&(-89D&'(3&-.%5(/($#'?46&(;.%(&-&':5(.-($&4.i&3( '#-:&(4/9D.-&3(;.%(%&(%8--&6.-:($'/D#D.6.%5+( '/K&4?/-(.(%&(-89D&'(/('?/-($&'(%#':&%(-846&8($&'( 8-.%(?9&(3.7.3&3(D5(%&(k8C(/(.-4.3&-%($#'?46&H( KE E µ mv 2 2 ( E ) number of rxn /nucleus/time number incident particles/ area / time n E de 2n 2 / 2 kt ( ) 3 / 2 E/ 2 e E / kt de f&%(6$3&-/%&(#(%#':&%($#'?46&(#-3(2(3&-/%&(#-(.-4.3&-%($#'?46&h([&( -89D&'(/('C-<()< <(.(%&(-89D&'(/($#'?46&(%#%(4#-(%'.V&(C(.-(?9&(.-%&'7#6(3%(;.%(#(7&6/4.%5+( v E ( ) 2E /µ m
9 </3-*$/*%++$+/.%#( dn E ( E )v( E )n i,e dedt n i,e de n i n n EdE, n i n i,e de rxns per nucleus dt # [&(-89D&'(/(.-4.3&-%($#'?46&(.(%&( -89D&'(4/-%#.-&3(.-(#(456.-3&'(/(7/689&( UV$GUV$),F(( dn dt ( E )v ( E ) n i n n EdE T89D&'(/(.-4.3&-%($#'?46&(;.%(%&( #$$'/$'.#%&(7&6/4.%5(@.H&H<(&-&':5A(.(#( '#4?/-(/(%&(%/%#6(-89D&'(/($#'?46&H( #5*-,%*( # )(4/9&('/9(%&($'&7./8(OY(3.%'.D8?/-H(T'$ #54*$%&$*6#+$7*$#/3+$7*$.5$2#,*G-3$O2,'$ #*C($4,O#$$-#)$$W$)F( </3-*$/*%++$+/.%#( r i,x E # n x n i ( E )v ( E ) n E n de ' ( ) $% & 2 $% ) h p ( E ) $e -2% 2 U c / E ( 2 *, $ + E U c E Z Z 2 e 2 /4%. r Z Z 2 e 2 µ m v 2 /2 2%. hv ( ) $e -be /2 b / %µ / 2 m Z Z 2 e 2 E 2 / 2. h E/'(# 6 (%#':&%<(%&(%/%#6(-89D&'(/('C-($&'(8-.%( 7/689&(.(/8-3(D5(.-%&:'#?-:(/7&'(#66($/.D6&( &-&':.&( [&(8-4?/-#6(/'9(/(%&(4'/K&4?/-(.(4/9$6.4#%&3H((#(.9$6.i4#?/-<(%.-V(/(.%(#(%&($5.4#6(4'/K&4?/-<(4#6&3( D5(%&(3&(Y'/:6.&(;#7&6&-:%( [&(%8--&6.-:($'/D#D.6.%5(.(&C$/-&-?#6<(:/.-:(%/(L&'/( #(%&(/86/9D($/%&-?#6(:/&(%/(.-i-.%5( /86/9D($/%&-?#6(&-&':5(( D(3&$&-3(/-(9#<(&6&4%'.4(4#':&( </3-*$/*%++$+/.%#( /9D.-.-:(%&(3&$&-3&-4.&(/'(%&(4'/K&4?/-+( r i,x 2 $ # & kt % ( ) S( E ) E 3 / 2 E n i n x µ m ' /2 ebe * ) S E ( ) / 2 ( )e (be (/2 e (E / kt de E'/9(%&(%8--&6.-:( $'/D#D.6.%5( E'/9(%&(OY(%&'9( I-5%O$H-B( [&($'/384%(/(%&(%;/(&C$/-&?#6(#4%/'($'/384&(#( %'/-:65($&#V&3(48'7&+( T846&#'('C-($'/D#D.6.%5(3&$&-3(/-(%&(V.-&?4( &-&':5(/(%&(4/66../-H([&(I#9/;($&#V( #'.&('/9(%&(OY(.:(&-&':5(%#.6(#-3(%&( /86/9D(D#''.&'(%&'9H( [.($6/%('&$'&&-%(4/66../-(/(%;/($'/%/-(#%( %&(4&-%'#6(%&9$&'#%8'&(/(%&(28-H(,(:UV(.(6/;65(7#'5.-:<(.%(4#-(D&(%'&#%&3(#(#( 4/-%#-%(#-3($866&3(/8%(/(%&(.-%&:'#6H((
10 9%)2X/-.%#+$,%$</3-*$*6#$*-,+8(,(%&'&(.(#('&/-#-4&(D&%;&&-(%&( &-&':5(/(%&(.-4/9.-:($#'?46&(#-3(( %&(/'D.%#6(&-&':5(6&7&6(/(%&( $&#V.-:(#%($&4.i4(&-&':.&H(( H%O*$3-O$&%*$*6#$*-,+( NC-('#%&(4#-(D&(;'.G&-(#($/;&'(6#;(4&-%&'&3(#%(#( $#'?486#'(%&9$&'#%8'&H(( r i,x r X i X x #' T $,%(.(#6/($/.D6&(%/(6/;&'(%&(/86/9D($/%&-?#6(D#''.&'(D5( 3/,*%#$+/*#2#C<(;.4(/448'(;.%(%&'&(#'&(9#-5('&&( &6&4%'/-(@./-.L&3(#%/9(#%(.:(4&-%'#6(%&66#'(%&9$&'#%8'&A( X i X x #' 2 $ O#('#4?/-(/(.-4.3&-%(#-3( %#':&%($#'?46&( B/;&'(6#;(&C$#-./-(/('C-('#%&(&F-( Z(lP(/'(%;/KD/35(4/66../-<((4#-('#-:&( '/9()(%/(#D/8%(R*H( H%O*$3-O$&%*$*6#$*-,+( /9D.-&(%&('C-('#%&(;.%(%&(&-&':5($&'('C-(%/(:&%(%&( #9/8-%(/(&-&':5($&'(&4/-3($&'(V:+( Y52#%+2,($C*-)2#,( [/%#6(689.-/.%5(.(%&(89(/(#66(&-&':5(@-846&#'<( 4&9.4#6<(:'#7.%#?/-#6A(:&-&'#%&3(D5(%&66#'(9#%&'.#6H( # i,x & % ( r i,x $ ' ' i,x X i X x ) T * [ W kg + ] ) )'+ M-&':5($&'(V:(?9&(%&('C-('#%&( [&(89(/(&-&':5('&6&#&3($&'( &4/-3($&'(V:(.(%&(%/%#6(-846&#'( &-&':5(:&-&'#?/-('#%&( dl dm nuclear + grav dl r dr 4r2 # [/%#6(&-&':5($&'(V:($&'(&4/-3(D5(#66( -846&#'('C-Z(#-3(D5(:'#7.%5( f89.-/.%5(38&(%/(&-&':5(:&-&'#%&3(;.%.-( %#'(.-%&'./'<(/8%(%/(%&('#3.8<('H(
11 </3%+(#,'+2+$-#)$/%#+*G-.%#$3-O+( T846&/5-%&.('?/-(4/-&'7&(4#':&<(-846&/-( -&8%'.-/<(-FBF-F$32C',$,'2#C+A( R*-#/'2#C$>-.%+( ' pp ~,pp X 2 4 f pp # pp C pp T 6 ~.8 $ %2 W m 3 kg %2 E.'%(%&$(.(%&(6/;&%(K(.-7/67&(%&(3&4#5(/(#( $'/%/-(.-%/(#(-&8%'/-( e + e + 2# M6&4%'/-($68(#($/.%'/-(5.&63(%;/(@.:( &-&':5A($/%/-( #$%&'()#*+*,%-.#$/** -89D&'(/(9#G&'(6&$%/-(K(-89D&'(/(#-?9#G&'(6&$%/-( 5+,$4$/%#+,-#,(.()#/( A Z X L(.(%&(&6&9&-%<(Z(.(%&(-89D&'(/($'/%/-<(P(.(%&(-89D&'(/(-846&/-(@$'/%/-(](-&8%'/-A( M#4(%&$(/(%&($K$( 4#.-(#(#(3._&'&-%( 'C-('#%&(D&4#8&( 3._&'&-%(/86/9D( D#''.&'(#-3(4'/K &4?/-(#'&(.-7/67&3H( [&&('C-('#%&(#'&(/'( %&(4&-%'#6( %&9$&'#%8'&(/(%&( 28-H( [<\$[(/3( [<\$[(/3( 4 2He+ 4 2 He 8 4 Be 8 4 Be+ 4 2 He 2 6 C + # 3$ ~ #',3$ % 2 Y 3 f 3$ T 8 4 E#9/8(m%'.$6&(#6$#($'/4&n(4/-7&'%( &6.89(.-%/(4#'D/-H(( T/%&(%&(3'#9#?4(&-.?7.%5(%/( %&9$&'#%8'&(.-(%&($/;&'(6#;('C-('#%&H( E/'(#(-846&8(;.%((-846&/-<( :(p( $'/%/-<(%&(D.-3.-:(&-&':5($&'(-846&/-+( M D U94 P Uqp9 $ ]@KpA9 - (K9-846&8 r4 P ( 2 6C+ 4 2 He 6 8 O + 6 8O+ 4 2 He 2 Ne + E/'9#?/-(/(.&'( &6&9&-%(%'/8:(%&( #33.?/-(/(#6$#( $#'?46&o<T<><T&<O:<( 2.<(E&( 2.9$65(%&(3._&'&-4&(D&%;&&-(%&(9#(/( Kp+(T89D&'(/(-&8%'/-( '&&($'/%/-(#-3(-&8%'/-(#-3(%&(9#(/( %&(D/8-3(-846&8H( %(%&(#%/9.4(9#(/(E&<(%&(D.-3.-:(&-&':5(.((((
12 #*C($T*-#+7%*,( dr G M r g dm r dr 4 r2 dl r dr 4r2 # M-&':5(%'#-$/'%+( )A PA QA 5&%(/'([@'AH(( N#3.#?/-H(N#-3/9(;#6V(D5($/%/-<(#D/'D&3<(4#G&'&3<('&K&9.G&3H( /-7&4?/-H(J/%(D/85#-%(9#(&6&9&-%(4#''5(&-&':5( /-384?/-H(['#-$/'%(D5(4/66../-(@:&-&'#665(-/%(.9$/'%#-%(.-(%#'AH(( >-)2-.G$T57*-,*$I*-)2#,( rad dr # c F rad 4 3 at 3 dr dr 3 # 4ac T F 3 rad F rad L 4$ dr 3 # L 4ac T 3 4$ N#3.#?7&(k8C('/9(%&(2%&#-K Y/6%L9#--('&6#?/-( N#3.#?/-($'&8'&(:'#3.&-%( N#3.#?7&(%&9$&'#%8'&(:'#3.&-%+(#(&.%&'( %&(689.-/.%5(/'(/$#4.%5(.-4'&#&<(%&( %&9$&'#%8'&(:'#3.&-%(D&4/9&(%&&$&'<H( 2%&&$&'(:'#3.&-%($'/9/%&(4/-7&4?/-H( H*++*$:/-3$]2C',8$/'-*-/,*2+./$3#C,'$+/-3$&%*$/%#G/.%#( K2*+,$Y-O$%&$T'*5%)(#-52/+( H P dr B'&8'&(4#6&(&.:%( du dq dw #-:&(.-(.-%&'-#6(&-&':5(U(&#%(#33&3(@3A( 9.-8(;/'V(3/-&(@3tAH( dr P H P lnp r H P U 3 k % $ ' T 3 2# µm H & 2 nrt,-%&'-#6(&-&':5(.(%&(#7&'#:&(%&'9#6(&-&':5( $&'(9#(&6&9&-%H(;$.(#(m%#%&n(8-4?/-(K(/-65( 3&$&-3(/-(48''&-%(4/-3.?/-(/(%&(:#<(-/%( /-(.%/'5H(,%(.(#(8-4?/-(/(4/9$/.?/-<(<( #-3(%&9$&'#%8'&( P P o e r / H P dr g J B (.(%&(3.%#-4&(;&'&(%&( $'&8'&(3'/$(D5()\B( 28D?%8%&(%&('#3.#?7&($'&8'&(:'#3.&-%(.-%/( &C$'&./-(/'(%&($'&8'&(4#6&(&.:%( nr k #(.(%&(-89D&'(/(9/6&((( µm H NUgHQ)RRaPs(9/6& K) (b K) (U(8-.7&'#6(:#(4/-%#-%( H P P g ~ R Sun
13 :7/2X/$]-,( :7/2X/$]-,$[^( C P Q P C V Q V #-:&(.-(@3A(.(88#665(&C$'&&3(.H%H/H(%&( $&4.i4(&#%<([ H $U+7/2X/$'-,$-,$/%#+,-#,$ 7*++*V$%*$[^$U+7/2X/$'-,$-,$/%#+,-#,$ G%35V( dw F $ # & dr PA $ # & dr PdV m% m % du dq ' PdV I#(&C&'%(#(/'4&<(EUB(/-(%&( &-3(/(#(456.-3&'<(#-3(3/&( ;/'V(9/7.-:(%&($.%/-(#( 3.%#-4&(3'+(tUE3'( %(4/-%#-%(7/689&+( dv ( du du V dq V du )Q )T V C V du C V,-3&$&-3&-%(/(%&( %&'9/35-#9.4($'/4&( E/'(#(9/-#%/9.4(:#+( du 3nR $ # & 2 % C V 3 2 nr :7/2X/$]-,$[ H ( du Q T P P V T P PV nrt PdV + V RTdn + nr P)2-4-./8$)S_A( du dq PdV PdV + V nr du C V du C V PdV C V %(4/-%#-%($'&8'&+( PdV nr P dv nr du C V C V Q T P nr C V C P nr C P C V + nr #6;#5o( C V 3 2 nr C P 5 2 nr C P C V 5 3 # PdV + V nr & % ( PdV $ ' C V PdV + V 2 3 PdV 5 PdV V 3 ) dv V P PV K u.-:(%&(.3(:#(6#;+( ( ) P K'T
14 P)2-4-./$+%#)$+7)8( P)2-4-./$,57*-,*$C*-)2#,8( v sound B [&($&&3(/(/8-3(.('&6#%&3(%/(%&( 4/9$'&.D.6.%5(/(#(:#( P g kt µm H W._&'&-?#?-:(%.(/'9(/(%&(.3(:#(6#;( B V #P #V [&(D86V(9/3868(/;(/;(984(%&(7/689&(/(%&( :#(4#-:&(;&-(.%(.(4/9$'&&3H( dr P dµ µ dr + P d dr + P T dr V # $ P K% W&i-.?/-(/'(X/689&+()\$&4.i4(3&-.%5( v sound $P 3.#D#?4(/8-3($&&3( dr % P d dr W._&'&-?#?-:(%&(#3.#D#?4(:#(6#;( P)2-4-./$,57*-,*$C*-)2#,8( P)2-4-./$,57*-,*$C*-)2#,8( dr P d dr + P T dr P d dr P d dr + P T dr $ # ' & ) T dr adiabatic % ( P dr dr #G M r P g kt µm H 89&(4/-%#-%(( P)2-4-./$,57*-,*$C*-)2#,8$ /%#G/.%#$ # & % ( µm H GM r dr adiabatic $ ' k g C P [&(4/-7&4?7&(4&66(98%('&9#.-(D8/5#-%(#%(&7&'5(6&7&6(.(.%(.(%/(4/-?-8&('..-:H(,(%&(3&-.%5(/(%&(D8DD6&(.(6&( %#-(%&(3&-.%5(/(%&(8''/8-3.-:(:#(.-(%&(%#'<(%&-( %&(D8DD6&(;.66('.&H(( /-3.?/-(/'(4/-7&4?/-+( > dr star dr adiabatic bubble N#3.#?7&(%'#-$/'%(;.66(#6;#5(D&($'&&-%v((/-7&4?/-(4#-( %8'-(/-(/'(/_(3&$&-3.-:(/-($5.4#6(3&$%(.-%/(%&(%#'<( &7/68?/-#'5(%#:&(&%4H( f#':&(%&9$&'#%8'&(:'#3.&-%(#'&(4#8&3(d5(.:(/$#4.%5h(( J.:65(/$#F8&(6#5&'(4/-%'.4%(%&(k/;(/(&#%('/9(D&6/;(K( %&(%#'(4#-(&C$#-3<(/'(8&(4/-7&4?/-(#(#(m#&%5(7#67&Hn(
15 :,33-*$/%#G/.%#$ [%#)2.%#$&%*$/%#G/.%#8( E/'(#(9/-#%/9.4(:#<(%.(4/-3.?/-(/'(%&( %&66#'(#%9/$&'&(4#-(D&('&K;'.G&-+( d lnp dlnt < # 2.5 t&-()$6-h$`$)$6-t(c(ph`<(%&(%#'(.(%#d6&(#:#.-%( 4/-7&4?/-H(,-(:&-&'#6<(4/-7&4?/-(/448'(;&-+(@)A(%&66#'(/$#4.%5(.( 6#':&<(@PA(./-.L#?/-(4#8&(#(6#':&($&4.i4(&#%(#-3(6/;( #3.#D#?4(%&9$&'#%8'&(:'#3.&-%(@QA(%&(%&9$&'#%8'&( 3&$&-3&-4&(/(-846&#'(&-&':5('#%&(.(6#':&(@T>(4546&A( 9262#C$3#C,'$,'%*($%&$+7*-)2-4-./$/%#G/.%#8( 9262#C$3#C,'$,'%*($%&$+7*-)2-4-./$/%#G/.%#8( E8-3#9&-%#6(4'.%&'.#(/'(4/-7&4?/-+(3&-.%5(/(%&('..-:(D8DD6&(.( 6&(%#-(3&-.%5(/(%&(8''/8-3.-:(:#H( > dr star dr adiabatic bubble f&%(%&(d8dd6&(d&(#3.#d#?4<(#-3(%&(%&9$&'#%8'&(:'#3.&-%(/(%&( 8''/8-3.-:(D&(%&(%&9$&'#%8'&(:'#3.&-%(/(%&(%#'+( # T % $ dr ad dr star & # ( dr & % ( dr ' $ dr ' 2.-4&(%&9$&'#%8'&(:'#3.&-%(#'&(#6;#5(-&:#?7&+( l )H P 3(.(%&(9.C.-:(6&-:%<(] H (.(%&($'&8'&(4#6&( &.:%H(([&('#?/(/(%&&(%;/(6&-:%<(<( #(7#68&(D&%;&&-(*H`(#-3(QH( > dr bubble dr star q C P T ( )* MC4&(&#%(k/;($&'(8-.%( 7/689&('/9(%&(D8DD6&(%/(%&( 8''/8-3.-:(:#(
16 :,33-*$9%)3$R23)2#C( dr G M r g ]()*%+,-./$2324*258$7*++*$G+$C*-G2,($ :,33-*$9%)3$R23)2#C( dr G M r g ]()*%+,-./$2324*258$7*++*$G+$C*-G2,($ dm r dr 4 r2 9-++$/%#+*G-.%#$ dm r dr 4 r2 9-++$/%#+*G-.%#$ dl r dr 4r2 # Y52#%+2,($C*-)2#,$ dl r dr 4r2 # Y52#%+2,($C*-)2#,$ dr 3 # L 4ac T 3 4$ T57*-,*$C*-)2#,$U*-)2-.GV$ dr 3 # L 4ac T 3 4$ T57*-,*$C*-)2#,$U*-)2-.GV$ # & % ( µm H dr adiabatic $ ' k GM r g C P T57*-,*$C*-)2#,$U/%#G/.%#V( # & % ( µm H dr adiabatic $ ' k GM r g C P T57*-,*$C*-)2#,$U/%#G/.%#V(,(%&(%#'(.(%#?4(&-&':5(4/9&('/9(-846&#'('?/-( :,33-*$9%)3$R23)2#C( (9/3&6(#%9/$&'&(4/-.%(/(#(%#D6&(/(-89D&'(:.7.-:(%&(/8'4&( 8-4?/-(@/'(%&(%&9$&'#%8'&A<(#-3($'&8'&(#(#(8-4?/-(/(/$?4#6(3&$%H(( W&$&-3.-:(/-(%&(#$$6.4#?/-<(#(9/3&6(9.:%(#6/($&4.5+$$ w$q#+2,($ w$i%5,*2/-3$)7,'$ w$p4+%*7.%#$/%a/2#,$ w$3/,*%#$7*++*$ w$9-#$2#,#+2,($ w$^3%/2,($ w$9-c#./$7*%7*.+$$ E'/9(%&(9/3&6<(%&(8'#4&(k8C(4#-(D&(4#6486#%&3+(.H&H<(%&(6.:%(&4#$.-:( %&(8'#4&($&'(8-.%(#'&#H(,-(/'3&'(%/(4#6486#%&(%&(689.-/.%5<(-&&3(%&(.-3&$&-3&-%65(3&%&'9.-&3(%&66#'('#3.8H( :,33-*$9%)3$R23)2#C(,-(#33.?/-(%/(%&(i7&(D#.4(%&66#'(&F8#?/-(@;.4(5/8Z66( -&&3(%/(9&9/'.L&A<(.-/'9#?/-(.(-&&3&3(#D/8%(%&( 4/9$/.?/-(/(%&(%#'(.-((6#5&'H$ P P(,T,composition) (,T,composition) # #(,T,composition) $$'/C.9#%&(;.%(.3(:#(#-3( '#3.#?/-($'&8'&( #6486#%&(&C$6.4.%65(D5(.-%&'$/6#?-:(#( :'.3(/(T( u&($/;&'(6#;(/'(%&($$(4#.-(/'( T>(4546&(K(K(38%5<( 4/9$8%#?/-#6('?/-(-&%;/'V( /9$/.?/-(4#-:&(;.%(?9&(#(.&'(&6&9&-%(/'9H(NC-Z(%#V&($6#4&(.-(%&(4/'&( /(%&(%#'(;&'&($'&8'&(.(.:&%H( >D^&4%(;.%(9#(x(*H*aP(O 2uT (3/(-/%(#7&(.:(&-/8:(%&9$&'#%8'&\$'&8'&(/'($$( 4#.-H(2%#'(;.%(9#(:'&#%&'(%#-(h*(O 2uT (#'&(8-%#D6&(%/(%&'9#6(/4.66#?/-H((
17 :,33-*$9%)3$R23)2#C( 6/(8&(D/8-3#'5(4/-3.?/-(%/(D8.63(%&66#'(9/3&6+$ M r L r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i'%(&%(/( D/8-3#'5(4/-3.?/-H( :,33-*$9%)3$R23)2#C8$P#-3(./-3$P77*%-/'( f#-&km93&-(&f8#?/-(:.7&(#-(#-#65?4#6(/68?/-(/'(%&66#'(%'84%8'&h( J5$/%&?4#6(%&66#'(9/3&6(.-(;.4(%&($'&8'&(3&$&-3(/-(3&-.%5(.-(%&( /'9(H$_$b (V-/;-(#($/65%'/$&H( d % $ ' (G dm r dr # dr & dr d % $ ' (G( 4) ) dr # dr & % $ ' (4)G # dr & d d* % dr r2 g $ ' 4)G # dr & * g U g m B/./-Z(&F8#?/-(/'($&'.4#665( 599&%'.4#6(:'#7.%#?/-#6($/%&-?#6( &-&':5( :,33-*$9%)3$R23)2#C8$P#-3(./-3$P77*%-/'( K d $ % & #2 d dr r2 dr ' ( ) #4*G + n +. - K d $, n / dr r2 (#n )/ n d ' % & dr ( ) #4*G ( ) c [ D n ( r) ] n r $ + ( n +) K #n c & - %, 4*G $ + n & n + - %, ( ) / n ( ) K c.' ) /( ( N ) / n 4*G d $ dd n ' dr % & r2 dr ( ) #D n n.' ) /( / 2 :4+.,,8$$H$_$b Y,8$$$_U?W#V$`$#$$ 67*++$$2#$,*5+$%&$+/-32#C$&-/,%*$Q # $-#)$,'$/#,*-3$)#+2,($ / N&$'&&-%(%&(3.%#-4&(%&'9(D5((
18 :,33-*$9%)3$R23)2#C8$ P#-3(./-3$P77*%-/'( [&-<(;.%($ r n # I&%(%&(.-#9/8(f#-&KM93&-(&F8#?/-+( d 2 d dd 2 n % n $ ' (D n # d & ))2#C,%#$Y52#%+2,($Y252,( P t rad dr kt µm H + 3 at 4 c F L rad c 4# [&($'&8'&(.-(#(%#'(.(-/'9#665(3/9.-#%&3(D5(%&(:#( $'&8'&(%&'9H(Y8%<(/'(%&(.:&%(9#(@.:&%( %&9$&'#%8'&A(%#'<('&:./-(/(6/;(3&-.%5(4#-(D&4/9&( 3/9.-#%&3(D5('#3.#?/-($'&8'&H$ N#3.#?/-($'&8'&(:'#3.&-%(,9$/&(D/8-3#'5(4/-3.?/-(@4/-%#-%(/(.-%&:'#?/-A(K(%&-<( /68?/-(/(%.(WHMH(.-(%&'9(/((/'(#($&4.i4($/65%'/$.4(.-3&C<(-<( :.7&(#(3&-.%5($'/i6&(#(#(8-4?/-(/('#3.8H(( J/;&7&'<(%&(8&86-&(/(%.(#$$'/#4(.(6.9.%&3(K(/-65(#-#65?4#6( /68?/-(/'(%'&&($/65%'/$&+(-U*<)<`H((( O/-/%/9.4(.3(:#+(-U)H`( W&:&-&'#%&(%#'+(-U)H`( M33.-:%/-(%#-3#'3(9/3&6+(-UQ( 5-3+#'&.$&6777$ dr $G M L Ed 4#Gc M E/'(%&(4/-3.?/-(/(53'/%#?4(&F8.6.D'.89<(&%(%&( &C$&'./-(/'(%&($'&8'&(:'#3.&-%(&F8#6(%/((/%&'(#-3( /67&(/'(%&(899:2;#2$<+-:2.:#H( ))2#C,%#$Y52#%+2,($Y252,( 9-++DY52#%+2,($*3-.%#( E/'(%#'(/-(%&(8$$&'(9#.-(&F8&-4&(;.%([l(`*<***b(@/(./-.L&3(K(;#%(.(%&($'.9#'5(/$#4.%5(/8'4&dA+( L Ed ~.5 3 M M sun L Ed M ~ L sun M sun [&(9#K689.-/.%5('&6#?/-(4#-(D&( 4#6486#%&3(/'(%#'H((( t.6&(%&(689.-/.%5('#-:&($#-('/9( )* KR (f 2uT (%/()* S( f 2uT <(%&(9#('#-:&(.( /-65(#(#4%/'(/(l)***H(( J.:(9#(%#'(#'(/8%$#4&(%&(&-&':5( $'/384?/-(/(6/;(9#(%#'<(#-3(%8( #7&(984(/'%&'(6.&?9&H( L Ed ~ L sun E/'(#(h*(O 2uT (%#'<(%&(M33.-:%/-(689.-/.%5(&C4&&3( %&(/D&'7&3(689.-/.%5(D5(#(#4%/'(/(Qo((%&(%#'(.(.-( 53'/%#?4(&F8.6.D'.89<(D8%(-/%(&C4&.7&65(/v(
to Highbury via Massey University, Constellation Station, Smales Farm Station, Akoranga Station and Northcote
b v Nc, g, F, C Uv Hgb p (p 4030) F g (p 4063) F (p 3353) L D (p 3848) 6.00 6.0 6.2 6.20 6.30 6.45 6.50 6.30 6.40 6.42 6.50 7.00 7.5 7.20 7.00 7.0 7.2 7.20 7.30 7.45 7.50 7.30 7.40 7.42 7.50 8.00 8.5 8.20
More informationParts Manual. EPIC II Critical Care Bed REF 2031
EPIC II Critical Care Bed REF 2031 Parts Manual For parts or technical assistance call: USA: 1-800-327-0770 2013/05 B.0 2031-109-006 REV B www.stryker.com Table of Contents English Product Labels... 4
More informationOutline Review Example Problem 1 Example Problem 2. Thermodynamics. Review and Example Problems. X Bai. SDSMT, Physics. Fall 2013
Review and Example Problems SDSMT, Physics Fall 013 1 Review Example Problem 1 Exponents of phase transformation 3 Example Problem Application of Thermodynamic Identity : contents 1 Basic Concepts: Temperature,
More informationt a serial T p c o y o d c b m ii y f t s u d W y p ii a p l u R O f l T h k s m me t er y d n y ad v o t b c t t t w j i t M ua T n a a o t U t n i a
= = W # = A G 1 P S 1 A R 2 R Sg 19 C C 1 R A 6 g (M, C S H S y 3 C F 4! U M y 1 D D ( 6 W B C D C 7 W T 6 E S S 4 W S 1 v E T 2 g y - F P C C 1 L 8 - d M S N 2 d O k4 C S 5 y D O 4 y? 4! 7 ~ S y C R Md
More information-$! " #$%&! ' () * +,,,)* -./ ( 01! 6 %&! +,,.: - 1?* 'F! %&! '3*4 -$ ):7 +,,
((((( +,-. ()* $%&' "#! : :!, %& ' ()*+ $ " -$! " #$%&! ' () * +,,,)* -. ( 01! '% 6):7 -$'1& '*6 )78 %&! +,, 79.& 2* '3*4 0 (A 6>* & ' BC D$!E.?@$* '*! ;4 6 %&! +,,.: - 1?* 'F! %&! '3*4 -$ ):7
More informationStellar Interiors. Hydrostatic Equilibrium. PHY stellar-structures - J. Hedberg
Stellar Interiors. Hydrostatic Equilibrium 2. Mass continuity 3. Equation of State. The pressure integral 4. Stellar Energy Sources. Where does it come from? 5. Intro to Nuclear Reactions. Fission 2. Fusion
More informationSpecific Heat of Diatomic Gases and. The Adiabatic Process
Specific Heat of Diatomic Gases and Solids The Adiabatic Process Ron Reifenberger Birck Nanotechnology Center Purdue University February 22, 2012 Lecture 7 1 Specific Heat for Solids and Diatomic i Gasses
More informationTrade Patterns, Production networks, and Trade and employment in the Asia-US region
Trade Patterns, Production networks, and Trade and employment in the Asia-U region atoshi Inomata Institute of Developing Economies ETRO Development of cross-national production linkages, 1985-2005 1985
More informationChapter 14 Kinetic Theory
Chapter 14 Kinetic Theory Kinetic Theory of Gases A remarkable triumph of molecular theory was showing that the macroscopic properties of an ideal gas are related to the molecular properties. This is the
More informationME 501. Exam #2 2 December 2009 Prof. Lucht. Choose two (2) of problems 1, 2, and 3: Problem #1 50 points Problem #2 50 points Problem #3 50 points
1 Name ME 501 Exam # December 009 Prof. Lucht 1. POINT DISTRIBUTION Choose two () of problems 1,, and 3: Problem #1 50 points Problem # 50 points Problem #3 50 points You are required to do two of the
More informationwhere R = universal gas constant R = PV/nT R = atm L mol R = atm dm 3 mol 1 K 1 R = J mol 1 K 1 (SI unit)
Ideal Gas Law PV = nrt where R = universal gas constant R = PV/nT R = 0.0821 atm L mol 1 K 1 R = 0.0821 atm dm 3 mol 1 K 1 R = 8.314 J mol 1 K 1 (SI unit) Standard molar volume = 22.4 L mol 1 at 0 C and
More informationHeat and Thermodynamics. February. 2, Solution of Recitation 2. Consider the first case when air is allowed to expand isothermally.
Heat and Thermodynamics. February., 0 Solution of Recitation Answer : We have given that, Initial volume of air = = 0.4 m 3 Initial pressure of air = P = 04 kpa = 04 0 3 Pa Final pressure of air = P =
More informationOutline Review Example Problem 1. Thermodynamics. Review and Example Problems: Part-2. X Bai. SDSMT, Physics. Fall 2014
Review and Example Problems: Part- SDSMT, Physics Fall 014 1 Review Example Problem 1 Exponents of phase transformation : contents 1 Basic Concepts: Temperature, Work, Energy, Thermal systems, Ideal Gas,
More informationChemistry. Lecture 10 Maxwell Relations. NC State University
Chemistry Lecture 10 Maxwell Relations NC State University Thermodynamic state functions expressed in differential form We have seen that the internal energy is conserved and depends on mechanical (dw)
More informationHelp us transform the Central Suburbs bus network Tell us what you think
Hv F p p 1 p 2 p 3 b pp cg p f vc pg 5 6 Cc f vc f pg 3 T v: Fp fbc f pg 8, fbc f AT.gv.z/NN c f AT.gv.z/NN? C v ( pg 4) c (09) 366 6400. Hp f C Sbb b T Fbc p f 1 Ocb 10 Dcb 2015 vg pbc p f Ac f fg Ac
More information(7) CALAMINTHA NEPETA 'WHITE CLOUD' (15) RUDBECKIA FULGIDA VAR.SULLIVANTII 'GOLDSTURM' (2) SPIRAEA JAPONICA 'ANTHONY WATERER'
XD DC D D ; () C ' COUD' () UDCK FUGD VUV 'GODU' () JOC 'OY ' () CGO X CUFO 'K FO' C f d Dpm f ub K DVO C-Cu ud, u u K, J vd O x d, - OV DG D VC Gp f CO OJC: F K DVO D UY DCG CUO XG CC COCO QUD O DGD U
More informationChapter 3 - First Law of Thermodynamics
Chapter 3 - dynamics The ideal gas law is a combination of three intuitive relationships between pressure, volume, temp and moles. David J. Starling Penn State Hazleton Fall 2013 When a gas expands, it
More informationIntroduction. Statistical physics: microscopic foundation of thermodynamics degrees of freedom 2 3 state variables!
Introduction Thermodynamics: phenomenological description of equilibrium bulk properties of matter in terms of only a few state variables and thermodynamical laws. Statistical physics: microscopic foundation
More informationYou MUST sign the honor pledge:
Chemistry 3411 MWF 9:00AM Spring 2009 Physical Chemistry I Final Exam, Version A (Dated: April 30, 2009 Name: GT-ID: NOTE: Partial Credit will be awarded! However, full credit will be awarded only if the
More informationYou MUST sign the honor pledge:
CHEM 3411 MWF 9:00AM Spring 2012 Physical Chemistry I Final Exam, Version A (Dated: May 4, 2012 Name: GT-ID: NOTE: Partial Credit will be awarded! However, full credit will be awarded only if the correct
More informationConnectJuly Heartily Congratulations
cjy 2017 Oy F h Mmb f F Lc S Gp Awd f FL Id - B Hy M. Ahk Km A G, mmc Hd Id f h cb whch d h c d h wd. I h h mk cmp whch v-ch; h chvm vy dcv. I mm cb d hw h cmmm wk h pd ff d h j h b. W cfd w m, d m dp
More informationTHE GRACE MESSENGER
G Ev L C 1326 S 26 S O, NE 68105-2380 402-341-7730 E: @. W S:.. Lk Fk :.fk./ R Sv Rqd Dd M REGULAR SUNDAY EVENTS 9:30.. C Ed 11:00.. W Sv P - Rv. D. D D. Lk Ed/C Sy - Bd S O - C Jffy Sx - A Lz L V C -
More informationceducate. SCIENCE
d f K K K v G v G W f f d v K G G G W f G W f d K v d K k b d d K v G G G f W b d dw f v d K d K v G v G G W G f b W d w d f d d v f d M M d k b d G f - 2016 2015 v bb w.. f d. www.kwb. d f Pd, M 1 Pd,
More informationAdvanced Placement. Chemistry. Integrated Rates
Advanced Placement Chemistry Integrated Rates 204 47.90 9.22 78.49 (26) 50.94 92.9 80.95 (262) 52.00 93.94 83.85 (263) 54.938 (98) 86.2 (262) 55.85 0. 90.2 (265) 58.93 02.9 92.2 (266) H Li Na K Rb Cs Fr
More informationNetworking Management system Protocol. User s Manual
wk M U M Id hp : I : dw : fw : w hp : w h : h : h : h h pwd : f. M p f. d h p : h : 7: f M-MU. h f d dp f d. h f d dp f b- d. h f d dp f * d. h f d dp f d. h f d dp f Y d. h f d dp f. d 7. h f d dp f V
More informationFIITJEE JEE(Main)
AITS-FT-II-PCM-Sol.-JEE(Main)/7 In JEE Advanced 06, FIITJEE Students bag 6 in Top 00 AIR, 75 in Top 00 AIR, 8 in Top 500 AIR. 54 Students from Long Term Classroom/ Integrated School Program & 44 Students
More information2016 FALL PARKS DIVISION AND WATER UTILITY LANDSCAPING
- - - - - - - - - - - - - - - - - DU F O K CD G K CUC G K D K FD K GY GOF COU O K G O K GD O K KGO-OYX K O CK K G K COD K K K (KG O) UY O G CK KY UY F D UY CY OF DO D OF UC OK U O: --; --; --; --; ---
More informationInternal Energy (example)
Internal Energy (example) A bucket of water KEs: translational: rotational: vibrational: PEs: within molecules: between molecules: @ rest on the table molecular bonds dipole-dipole interactions Internal
More informationHarold s AP Physics Cheat Sheet 23 February Electricity / Magnetism
Harold s AP Physics Cheat Sheet 23 February 206 Kinematics Position (m) (rad) Translation Horizontal: x = x 0 + v x0 t + 2 at2 Vertical: y = y 0 + v y0 t 2 gt2 x = x 0 + vt s = rθ x = v / Rotational Motion
More informationnd A L T O SOLO LOWELL. MICHIGAN. THURSDAY. APRIL Spring Activities Heads Up and Forward (Editorial By " T h e Committee'')
- 6 7 8 9 3-6 7 8 9 3 G UDY 3 93 VU XXXV U XY F K FD D j V K D V FY G F D Y X K X DD Y j \ V F \ VD GD D U Y 78 K U D Y U Y 484?35 V 93 7 4 U x K 77 - D :3 F K > 6 D x F 5 - - x - G 7 43 8 D $35 K F $5
More informationLOWELL STORES SERVE THRONGS OF LOV PEOPLE ON FRIDAY NIGHT
J p M 879 61 p 260 M G W j p : b p pp M M K p b J M G * p P p b p p D W P p b G 14 b p qp j b p p p J p z M- K W W G Gbb Wb M J W W K G J D D b b P P M p p b p p b b p J W ; p jb b p x b p p b b W Pp pp
More informationP a g e 3 6 of R e p o r t P B 4 / 0 9
P a g e 3 6 of R e p o r t P B 4 / 0 9 p r o t e c t h um a n h e a l t h a n d p r o p e r t y fr om t h e d a n g e rs i n h e r e n t i n m i n i n g o p e r a t i o n s s u c h a s a q u a r r y. J
More informationPrayer. Volume III, Issue 17 January 11, Martin Luther King Jr. Prayer. Assumption Catholic School 1
Vm III, I 17 J 11, 2017 TROJAN NEW W Rpb Cz, E Cmm, L L L, d A Ch wh bd mm d mk p. P M Lh K J. P Gd h h h Am d A h wd, W w h h hh w; w whh M w h bh. A w whh h h wd w B h wd pwh, Ad h p p hk. A w whh m
More informationYou MUST sign the honor pledge:
CHEM 3411 MWF 9:00AM Fall 2010 Physical Chemistry I Exam #2, Version B (Dated: October 15, 2010) Name: GT-ID: NOTE: Partial Credit will be awarded! However, full credit will be awarded only if the correct
More informationEntropy in Macroscopic Systems
Lecture 15 Heat Engines Review & Examples p p b b Hot reservoir at T h p a a c adiabats Heat leak Heat pump Q h Q c W d V 1 V 2 V Cold reservoir at T c Lecture 15, p 1 Review Entropy in Macroscopic Systems
More informationIdeal Gas Law. Deduced from Combination of Gas Relationships: PV = nrt. where R = universal gas constant
Ideal Gas Law Deduced from Combination of Gas Relationships: V 1/P, Boyle's Law V T, Charles's Law V n, Avogadro's Law Therefore, V nt/p or PV nt PV = nrt where R = universal gas constant The empirical
More information35H MPa Hydraulic Cylinder 3.5 MPa Hydraulic Cylinder 35H-3
- - - - ff ff - - - - - - B B BB f f f f f f f 6 96 f f f f f f f 6 f LF LZ f 6 MM f 9 P D RR DD M6 M6 M6 M. M. M. M. M. SL. E 6 6 9 ZB Z EE RC/ RC/ RC/ RC/ RC/ ZM 6 F FP 6 K KK M. M. M. M. M M M M f f
More informationHelp parents get their kids settled in with this fun, easy-to-supervise coloring activity. A Fun Family Portrait... 3
K u R C d C! m m m k m u y g H p u R Cd C g d g b u d yu g p m d fu g f pg m g w Tk yu C g p D Ng kd pg u bk! T y g b fm dy m d md g g p By pvdg ud d ug yu u f D Ng Cg v, yu b pg up g u d g v bf W v pvdd
More informationLecture 3 Clausius Inequality
Lecture 3 Clausius Inequality Rudolf Julius Emanuel Clausius 2 January 1822 24 August 1888 Defined Entropy Greek, en+tropein content transformative or transformation content The energy of the universe
More informationT h e C S E T I P r o j e c t
T h e P r o j e c t T H E P R O J E C T T A B L E O F C O N T E N T S A r t i c l e P a g e C o m p r e h e n s i v e A s s es s m e n t o f t h e U F O / E T I P h e n o m e n o n M a y 1 9 9 1 1 E T
More informationOddn ENTRIES. Two New Buildings For County 4-H Fair
D G N H V G NNG \VH FYXH Y N $40000 b U v v 000 v b vv v vb v v b b x b z b v b b b & K b K G DH F H H /\U F b 80 K b z b bb v $40000 b v x v b bb 8 v b 30 K b b v v b v b b? x v z v b H D N G N H H Fz
More informationC e. Negative. In a clockwise cycle, the work done on the gas is negative. Or for the cycle Qnet = +600 J and U = 0 so W = Q = 600 J
AP Physics Free Response Practice Thermodynamics ANSWERS 1983B4 Since T is constant, pbv B = p 0 V 0 and V B = 2V 0 gives p B = ½ p0 U = Q + W, since AB is isothermal, U = 0 and W = Q = 1000 J c. The entropy
More informationSection 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow
Section 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow Anderson: Chapter 2 pp. 41-54 1 Equation of State: Section 1 Review p = R g T " > R g = R u M w - R u = 8314.4126
More informationLecture 4 Clausius Inequality
Lecture 4 Clausius Inequality Entropy distinguishes between irreversible and reversible processes. irrev S > 0 rev In a spontaneous process, there should be a net increase in the entropy of the system
More information4. All questions are NOT ofequal value. Marks available for each question are shown in the examination paper.
THE UNIVERSITY OF NEW SOUTH WALES SCHOOL OF PHYSICS \1111~11\llllllllllllftllll~flrllllllllll\11111111111111111 >014407892 PHYS2060 THER1\1AL PHYSICS FINAL EXAMINATION SESSION 2 - NOVEMBER 2010 I. Time
More information6 Physical transformations of pure substances
6 Physical transformations of pure substances E6.b E6.2b E6.3b E6.4b Solutions to exercises Discussion questions Refer to Fig. 6.8. The white lines represent the regions of superheating and supercooling.
More informationThe first law of thermodynamics continued
Lecture 7 The first law of thermodynamics continued Pre-reading: 19.5 Where we are The pressure p, volume V, and temperature T are related by an equation of state. For an ideal gas, pv = nrt = NkT For
More information176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s
A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps
More informationThe Evolution of Outsourcing
Uvy f R I DCmm@URI S H Pj H Pm Uvy f R I 2009 T Ev f O M L. V Uvy f R I, V99@m.m Fw wk : ://mm../ P f B Cmm Rmm C V, M L., "T Ev f O" (2009). S H Pj. P 144. ://mm..//144://mm..//144 T A b y f f by H Pm
More informationHomework: 13, 14, 18, 20, 24 (p )
Homework: 13, 14, 18, 0, 4 (p. 531-53) 13. A sample of an ideal gas is taken through the cyclic process abca shown in the figure below; at point a, T=00 K. (a) How many moles of gas are in the sample?
More informationChapter 18 Thermal Properties of Matter
Chapter 18 Thermal Properties of Matter In this section we define the thermodynamic state variables and their relationship to each other, called the equation of state. The system of interest (most of the
More informationYou don t need a better car, you need to learn how to drive
O h Imp f Cyb-Df L Am Y d d b, y d hw dv E Lv, F Hm, Phpp Lwk m AG 2017 m.m Wh w? m AG 2017 Pg 3 Y d d b, y d hw dv Wh h k b Wh w dd Wh w h p Wh h k NOT b C p-by-p hw fx hg Cd Vd bhg A mk
More informationMultivariable Calculus
Multivariable Calculus In thermodynamics, we will frequently deal with functions of more than one variable e.g., P PT, V, n, U UT, V, n, U UT, P, n U = energy n = # moles etensive variable: depends on
More informationAn Elephantine Misunderstanding: A miscommunication between researchers and their subjects
P S d C R hr J hkd AE h M d d g: AM mm b w R h dt h S bj R 1 7 A 2 1 P S d C U v y f M h g I f S R h A Eh Mddg: A mmm bw h d h bj Jh Kd Uvy f Mhg P Sd C Rh R 1-7 A 21 Akwdgm: Th h b d f d dd vm D h Fd
More informationINSTALLATION INSTRUCTIONS
U 18 D V p y p & d 2-5 - 410 208~230 V. 1. 60 z. Md: YD024GM18M2 YD036GM18M2 YD048GM18M2 YD060GM18M2 : pp f y vy. GZ YMB D M Y M G dd d qfd d v p f pp, dj d p f. d gy bf pg p. fw y pp, dj, v pby g f, k,
More informationl l s n t f G A p p l i V d s I y r a U t n i a e v o t b c n a p e c o n s
G A 2 g R S 2 A R 2 S I g 3 C C 2 S S 5 C S G 6 S 4 C S 5 S y 1 D O A 1 S R d G 1 d 1 E T S & T 2 Vg y F P 4 2? M I 2 J H W 1 W B C L D 1 2 L W 4 M T 5 M S N 2 O I 4 P 7, P S 1 8 R I y y w Y f If f K f
More informationVECTORS ADDITIONS OF VECTORS
VECTORS 1. ADDITION OF VECTORS. SCALAR PRODUCT OF VECTORS 3. VECTOR PRODUCT OF VECTORS 4. SCALAR TRIPLE PRODUCT 5. VECTOR TRIPLE PRODUCT 6. PRODUCT OF FOUR VECTORS ADDITIONS OF VECTORS Definitions and
More informationEffect of adding an ideal inert gas, M
Effect of adding an ideal inert gas, M Add gas M If there is no change in volume, then the partial pressures of each of the ideal gas components remains unchanged by the addition of M. If the reaction
More informationLecture 4 Clausius Inequality
Lecture 4 Clausius Inequality We know: Heat flows from higher temperature to lower temperature. T A V A U A + U B = constant V A, V B constant S = S A + S B T B V B Diathermic The wall insulating, impermeable
More informationWhitney Grummon. She kick started a fire in my soul Teaching me a tool to cleanse my mind That ll last a life time. That s how I will remember
W Gmm S kk f m T m m m T f m T I mmb N m p f p f f G L A f b k, b k v M k b p:, bb m, m f m, v. A b m, f mm mm f v b G p. S m m z pp pv pm f, k mk, f v M. I m, I m, fm k p x. S f 45 m m CMS, I p mf,. B
More informationLions 202L News and Views Week Commencing 2 nd May ISSUE 586. Like us on facebook/noozletta Please address all items to
L 0L Nw d Vw W Cg d My ISSUE 86 L fb/nz P dd z@b.g.z Gg fw L I p y d g w d wd. I v d g w y b R E g f R Ad L M. w pg Sf Cy Ld w wd b f. b by pj, d g g pp w pfg dd v- ' L vg f d w dg g y v D' fg Off g g
More informationCoolsicles. Chicken Tenders. Hearty Beef Stew
Cck T M B Cck P Cc Hy B Sw D Ec, Ec pp y y cc y w C F K TM c p b y by N Fz R F Ac (NFRA) pp w cc pc Y M Ip (YMI). T p y cc w $50 pp y c ( ). C F K TM p c b cc, p c, b pyc cvy. I w y wk b pv w v w pc w
More informationRESOURCE, SUPPORT, AND DEVELOPMENT, INC
RESOURCE, SUPPORT, AND DEVELOPMENT, INC BOARD OF DIRECTORS Pd Pk E. K V-Pd B R S L Bd-Sw Ld Tk Nk Edwd A DB Dv S ADMINISTRATIVE TEAM Pvd v dvd w db B, Hd, Lww, d Rd Ld, M A Pb R.S.D., I Smm 2006 Vm 5 CEO
More informationtc'h~ Tenese Invasin YClS tf'i man through Allatoona Pass.-Resaca held, but Hood takes Dalton, and, avoiding a Battle, re- th
x -Pd 311 d Rd g -d g W--d dg g D k WT- p M- d P d 2161 T p -F dd d Ad E-A N--d W P Rd d g g 3 -T K- A-T B A - d: dn T p k d1)k 4 g d d pd-d d - Pd pddl314lx Y g A P-R d d k D d dg B - 1 ge %;- 0 1 - dd-
More informationChair Susan Pilkington called the meeting to order.
PGE PRK D RECREO DVOR COMMEE REGUR MEEG MUE MOD, JU, Ru M h P P d R d Cmm hd : m Ju,, h Cu Chmb C H P, z Ch u P dd, Mmb B C, Gm Cu D W Bd mmb b: m D, d Md z ud mmb : C M, J C P Cmmu Dm D, Km Jh Pub W M,
More informationPhysics 408 Final Exam
Physics 408 Final Exam Name You are graded on your work (with partial credit where it is deserved) so please do not just write down answers with no explanation (or skip important steps)! Please give clear,
More information(EccL HUt, Mosheim, p. 40.) AGC3. Rgnres. We shall now proceed to show two things:
P K K P / P V -K VX - x K D K GFF G D G DKX X P P F D K 8 6 Y X X X P 9 ] K V Y 0 - D 00 D P F G K K PXVK P > G K K V v v v v PK P v D > v Y v D P > P v v - v x V D - ()zx q - & 9 K x K > % x v - - P x
More informationers The Extraordinary Boogie and Swing Festival MUNICH GERMANY 9
W!!! C, E p, C J 95 RT H v D L T BI 10 N P f B 70 5 z V D AY b T Ex B Fv 28.02. - 04.03. MUNICH 1 GERMANY 9 R O C KT H AT W I N G. C O M WING ENT F O LD DLY PRE R WO PROU 14 5 DAY HT G I N UIC M E LIV
More informationAdiabatic Expansion/Compression
Adiabatic Expansion/Compression Calculate the cooling in a the reversible adiabatic expansion of an ideal gas. P P 1, 1, T 1 A du q w First Law: Since the process is adiabatic, q = 0. Also w = -p ex d
More informationAnalysis of Collaborative Learning Behaviors and the Roles of Collaborative Learning Agent
A v L Bhv h v L A Ik L (Sj Uv, S. K, @j..k) J H L (Uv Ih, S. K, jh@h..k) Sh J (S N Uv, S. K, v712@..k) E M S (S N Uv, S. K, 04@..k) K A M (E T h I, S. K, k@..k) H J S (E T h I, S. K, hjh@..k) A: v h h
More informationABCD42BEF F2 F8 5 4D6589 CC8 9
ABCD BEF F F D CC Vetri Velan GSI, Physics 7B Midterm 1: Problem 3 3. a) Since the collisions with the walls are all elastic, for each given wall, only one component of the velocity matters. Consider
More informationThe Standard Gibbs Energy Change, G
The Standard Gibbs Energy Change, G S univ = S surr + S sys S univ = H sys + S sys T S univ = H sys TS sys G sys = H sys TS sys Spontaneous reaction: S univ >0 G sys < 0 More observations on G and Gº I.
More informationDiscovery Guide. Beautiful, mysterious woman pursued by gunmen. Sounds like a spy story...
Dv G W C T Gp, A T Af Hk T 39 Sp. M Mx Hk p j p v, f M P v...(!) Af Hk T 39 Sp, B,,, UNMISSABLE! T - f 4 p v 150 f-p f x v. Bf, k 4 p v 150. H k f f x? D,,,, v? W k, pf p f p? W f f f? W k k p? T p xp
More informationČasopis pro pěstování matematiky
Časopis pro pěstování matematiky Alois Švec Determination of a surface by its mean curvature Časopis pro pěstování matematiky, Vol. 103 (1978), No. 2, 175--180 Persistent URL: http://dml.cz/dmlcz/108617
More informationThermodynamic Variables and Relations
MME 231: Lecture 10 Thermodynamic Variables and Relations A. K. M. B. Rashid Professor, Department of MME BUET, Dhaka Today s Topics Thermodynamic relations derived from the Laws of Thermodynamics Definitions
More informationT098. c Dr. Md. Zahurul Haq (BUET) First Law of Thermodynamics ME 201 (2012) 2 / 26
Conservation of Energy for a Closed System Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET Dhaka-, Bangladesh zahurul@me.buet.ac.bd
More informationDetails on the Carnot Cycle
Details on the Carnot Cycle he isothermal expansion (ab) and compression (cd): 0 ( is constant and U() is a function U isothermal of only for an Ideal Gas.) V b QH Wab nrh ln Va (ab : isothermal expansion)
More informationCAT. NO /irtl,417~ S- ~ I ';, A RIDER PUBLICATION BY H. A. MIDDLETON
CAT. NO. 139-3 THIRD SUPPLEMENT I /irtl,417~ S- ~ I ';,... 0 f? BY H. A. MIDDLETON.. A RIDER PUBLICATION B36 B65 B152 B309 B319 B329 B719 D63 D77 D152 DA90 DAC32 DAF96 DC70 DC80 DCC90 DD6 DD7 DF62 DF91
More informationPotential Concept Questions
Potential Concept Questions Phase Diagrams Equations of State Reversible Processes Molecular Basis of Heat Capacity State Functions & Variables Temperature Joules Experiment for conversion of one form
More informationThermodynamics of solids 5. Unary systems. Kwangheon Park Kyung Hee University Department of Nuclear Engineering
Thermodynamics of solids 5. Unary systems Kwangheon ark Kyung Hee University Department of Nuclear Engineering 5.1. Unary heterogeneous system definition Unary system: one component system. Unary heterogeneous
More informationConcentrating on the system
Concentrating on the system Entropy is the basic concept for discussing the direction of natural change, but to use it we have to analyze changes in both the system and its surroundings. We have seen that
More informationNuclear Binding Energy
Nuclear Energy Nuclei contain Z number of protons and (A - Z) number of neutrons, with A the number of nucleons (mass number) Isotopes have a common Z and different A The masses of the nucleons and the
More informationY'* C 0!),.1 / ; ')/ Y 0!)& 1 0R NK& A Y'. 1 ^. ]'Q 1 I1 )H ;". D* 1 = Z)& ^. H N[Qt C =
(-) 393 F!/ $5 $% T K&L =>-? J (&A )/>2 I B!" GH 393/05/07 :K 393/07/23 :7b +B 0 )NO M / Y'* C a23 N/ * = = Z)& ^. ;$ 0'* Y'2 8 OI 53 = ;" ~" O* Y.b ;" ; ')/ Y'* C 0!),. / ; ')/ Y 0!)& 0R NK& A Y'. ^.
More informationand A I L j T O S O L O LOWELL, MICHIGAN, THURSDAY, AUG. 1, 1935
Y D D Y 5 VD D Y D D - ( D K D ( > Kz j K D x j ; K D D K x z ( D K D ( ; ) ( ) V DY - j! ) : x x x j K D K j DY 95 Y-D Y D D j 5 4 V 89 j j j j 89 j 4998 9 j K 8 j V x j K x x 5 x x x j - K 4- -D K 4-
More informationOIL & GAS EQUIPMENT RENTAL SOLUTIONS
I A EQUIE EA UI by.c YE Eqp Wh v 65% f h w v 40% f h w v h E. W hv cy p p c h c q. y Eqp w f h UAE h y 1990 c h h w bc f h p qp cp h E. Wh 15 p b cv h UAE KA Kw Q h w hv f f v 10000 f p f v 800 pp. W ff
More informationLecture 7: Kinetic Theory of Gases, Part 2. ! = mn v x
Lecture 7: Kinetic Theory of Gases, Part 2 Last lecture, we began to explore the behavior of an ideal gas in terms of the molecules in it We found that the pressure of the gas was: P = N 2 mv x,i! = mn
More information" W I T H IvIALIGE T O W A R D ISTPISTE A N D O H A R I T Y F O R A L L LOWELL PEOPLE. A Fine Time with Mr. and Krs. Geo. W. Parker.
V - > >- VBz FB B DB j B DB&B G R D P D R Y F R V K CY C PR 9 2 B $200 3 G R G V C: C Y B B V F C F B $00 PC C VR CQ D P C x R q» G C R B BY B P Y P P J C CP F FRR D DRKR GD J B R D PC R P D < C x F B
More informationPhysics 607 Final Exam
Physics 67 Final Exam Please be well-organized, and show all significant steps clearly in all problems. You are graded on your work, so please do not just write down answers with no explanation! Do all
More informationPhysics 2 week 7. Chapter 3 The Kinetic Theory of Gases
Physics week 7 Chapter 3 The Kinetic Theory of Gases 3.1. Ideal Gases 3.1.1. Experimental Laws and the Equation of State 3.1.. Molecular Model of an Ideal Gas 3.. Mean Free Path 3.3. The Boltzmann Distribution
More information! 94
! 94 4 : - : : / : : : : ( :) : : : - : / : / : : - 4 : -4 : : : : : -5 () ( ) : -6 : - - : : : () : : : :4 : -7. : : -8. (. : ( : -9 : ( ( ( (5 (4 4 : -0! : ( : ( :. : (. (. (. (4. ( ( ( : ( 4 : - : :
More informationModule 5 : Electrochemistry Lecture 21 : Review Of Thermodynamics
Module 5 : Electrochemistry Lecture 21 : Review Of Thermodynamics Objectives In this Lecture you will learn the following The need for studying thermodynamics to understand chemical and biological processes.
More informationPreliminary Examination - Day 2 August 16, 2013
UNL - Department of Physics and Astronomy Preliminary Examination - Day August 16, 13 This test covers the topics of Quantum Mechanics (Topic 1) and Thermodynamics and Statistical Mechanics (Topic ). Each
More informationThermal Physics. 1) Thermodynamics: Relates heat + work with empirical (observed, not derived) properties of materials (e.g. ideal gas: PV = nrt).
Thermal Physics 1) Thermodynamics: Relates heat + work with empirical (observed, not derived) properties of materials (e.g. ideal gas: PV = nrt). 2) Statistical Mechanics: Uses models (can be more complicated)
More informationUNIVERSITY OF SOUTHAMPTON VERY IMPORTANT NOTE. Section A answers MUST BE in a separate blue answer book. If any blue
UNIVERSITY OF SOUTHAMPTON PHYS1013W1 SEMESTER 2 EXAMINATION 2011/12 ENERGY AND MATTER SOLUTIONS Duration: 120 MINS VERY IMPORTANT NOTE Section A answers MUST BE in a separate blue answer book. If any blue
More informationSuperior protection that you can count on.
M y p v wh cmp f f vcc F vcc 1 v p L LV (H V L (AL (K ph h c p K jv ( y k * m v k LV m c b Rh B C N Ch L R P fc ch 1% pc cfm 2 p.1,2 1-y vcc Expm gp P gm/ vm Pvb fc F-O-Vx Lv-K 1% Nbvc F 2-FLV 1% LEUKOCELL
More informationTABLES AND INFORMATION RETRIEVAL
Ch 9 TABLES AND INFORMATION RETRIEVAL 1. Id: Bkg h lg B 2. Rgl Ay 3. Tbl f V Sh 4. Tbl: A Nw Ab D Ty 5. Al: Rdx S 6. Hhg 7. Aly f Hhg 8. Cl: Cm f Mhd 9. Al: Th Lf Gm Rvd Ol D S d Pgm Dg I C++ T. 1, Ch
More informationAugust 30, 2013 Volume 85 Issue 2 echo.snu.edu 6612 NW 42nd St. Bethany, OK (405)
B S B OKC w TE Ag 30, 2013 V 85 I 2 d 6612 NW 42d S B, OK 73008 (405) 491-6382 R f v j xd P b K Rb K Rb, Ed--f E, v d f bdg vg f d d b d d f Of, b f g j, d Bd j g w d d g, SNU d g- j w fw T w d vd bdg
More informationKinetic Theory of Gases
Kinetic Theory of Gases Modern Physics September 7 and 12, 2016 1 Intro In this section, we will relate macroscopic properties of gases (like Pressure, Temperature) to the behavior of the microscopic components
More informationMolar Specific Heat of Ideal Gases
Molar Specific Heat of Ideal Gases Since Q depends on process, C dq/dt also depends on process. Define a) molar specific heat at constant volume: C V (1/n) dq/dt for constant V process. b) molar specific
More informationChapter 3. Property Relations The essence of macroscopic thermodynamics Dependence of U, H, S, G, and F on T, P, V, etc.
Chapter 3 Property Relations The essence of macroscopic thermodynamics Dependence of U, H, S, G, and F on T, P, V, etc. Concepts Energy functions F and G Chemical potential, µ Partial Molar properties
More information