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A marble moves along the x-axis. Its potential energy function U(x) is shown in the figure.! !"##$%&'&#()#*%&#+,'-&#,.#*%&#/!'01&',3# 0"##4*!01&#&56(1(0'(76/"7!"3# -"##8.)*!01&#&56(1(0'(76/"!3# !"#$% &'()*+(,%% !"###0#!.9#9#)(.-&#+,'-&#()# .&:!;<&#,+#*%&#=#9&'(<!;<&## 0"###0#)(.-&#>,*&.;!1#&.&':?# (.-'&!)&)#!',6.9#(*@#/&!.)# A(.&;-#&.&':?#9&-'&!)&)@# *&.9)#*,#)*!?#B-!1/CD## -"#9#96&#*,#(.-'&!)&#,+#E(.&;-#&.&':?@#%&.-&#-!.#&!)(1?#'6.#!F!?D# -% CURVEBALL on the Definition of Conservative Forces! .*/011,%!"%0%23+/*%4(%/3'(*+5065*7%#$%&%)3+8%93'*%:;%<=*%23+/*%013'>% 0%/13(*9%?0<=%4'%(?0/*%4(%@*+37%% A=*%/3'<+0?3(465*%32%<=4(%(<0<*B*'<%"C$7%)=4/=%!"%13>4/011;% *DE4501*'<%<3%4<%4(%<=0<% !"%<=*%)3+8%93'*%:;%0%23+/*%0+3E'9%0%/13(*9%?0<=%4(%FGA%@*+3% #$%&%<=*%23+/*%4(%FGFH/3'(*+5065*I' The reverse of this statement is NOT TRUE!! !"')3+8%93'*%:;%<=*%23+/*%013'>%0%/13(*9%?0<=%4'%(?0/*%4(% @*+37%#$%&%0%23+/*%4(%/3'(*+5065*% Moral: Only if the work done around every possible closed path is zero could we say that a force is conservative J% (impossible to demonstrate!).! An example which serves as a warning (i.e. an example where the converse is false)! Suppose a variable force acting on an object moving in the plane is given by:! = xy xˆ + 2xyˆ The work done by F in moving it around the closed loop (0,0)->(3,0)->(3,2)->(0,0) is! ! But this force is in fact non-conservative: move it around the unit square: (0,0)->(1,0)->(1,1)->(0,1)->(0,0)! K% Power under Constant Force ! ":*13)7%0B0@4'>%=3+(*?3)*+L$% M3'(49*+%0%/3'(<0'<%23+/*7%N7%0/6'>%3'%0%:39;% !! !! A=*%?3)*+%32%<=4(%23+/*%4(,% power = Work Done F"s = = Fv "t "t (v is mean velocity) O% power = Work Done F"s = = Fv "t "t (v is mean velocity) Implications:! (a) Power increases when the velocity of the object it acts on increases.! ! (b) Suppose your car maxes out at 550 Horsepower in your new BMW, by this relationship, the faster you travel (average velocity), the smaller the force it generate ---" smaller acceleration -" it is hard to increase velocity further (i.e., hard to accelerate more on a high way when you are already fast!) ! PQ%!'4<,%%RS(%T%U%"U0V$% W% Instantaneous Power! #-%!.:(.:#+,'-&)# !! !! G,.)(9&'#!#+,'-&@#H@#F%(-%#!-*)#,.#!#0,9?D#I6'(.:#!#)%,'*#;/& #J*#*%�,9?#/,<&)#!#)%,'*#9()*!.-&#J=D#K+#*%&#;/&#(.*&'<!1#() #)%,'*#&.,6:%#H#()#!>>',=(/!*&1?#-,.)*!.*#+,'#*%&#>&'(,9# "# "' !x% !!L%&#F,'A#9,.�?#*%&#+,'-&#(.#*%()#>&'(,9#()M# "W = F"x cos# !! N,F#*%&#>,F&'#,+#*%&#+,'-`'(.:#*%()#>&'(,9#()#)(/>1?#*%& #!/,6.*#,+#F,'A#9,.	(<(9&9#0?#*%&#;/&#(*#*!A&)#*,#9,#(* #),DDD# ! P= "W F"x cos# = "t "t X% K.#*%(/(*#*%!*#*%&#;/&#-%!.:&#)%'(.A)#*,#O&',@#F&#%!<&% #x dx = F cos " = Fv cos " #t dt dW ! ! Instantaneous Power P = = F •v dt P = F cos" ! Example: P#!'/?#*!.A#%!)#!#>,F&'#,+#QRRR@RRR#$D##K+#*%&#/!))# ,+#*%&#*!.A#()#SRR#*,.)D##N&:1&-*#+'(-;,.@#F%!*#()#*%&#!--&1&'!;,.# !,+#*%&#*!.A#F%&.#(*#()#*'!<&11(.:#!*#7S"#TU#A/V%,6'###7Q"##WQ#A/V%3% Solution: (a) 4*!'*#F(*%#!#>,F&'#&56!;,.#F%(-%#()#'&1!*&9#*,#+,'-&% P = Fv cos0 36 km "1000 m/sec = 10F 1 hour " 3600 sec/hour F = 200,000 N 2000000 = F " N,F#6)&#N&F*,.#KK#*,#),1<&#+,'#!--&1&'!;,.% ! F = ma ! 200,000 = 100,000 " a a = 2 m/s2 Q##% ! (b) G!''?#,6*#)(/(1!'#-!1-61!;,.@#+,'#<XWQ#A/V%@##F&#:&*#!XS#/V) Y% ! ! ! Y,'!1M###7!"#$(*%,6*#+'(-;,.@#!--&1&'!;,.#9&-'&!)&)#!)#)>&&9#(.-'&!)&)# % %%%%70"#$(*%,6*#+'(-;,.#*%&#!--&1&'!;,.#()#.&<&'#RZ# We should be thankful that friction keeps us from getting that speeding ticket! ! Why is Power a limiting factor???! !!N&&9#*,#'&/&/0&'#*%!*#*%&#F,'A #9,.�?#*%&#+,'-&#()#-,.<&'*&9#(.*, #E(.&;-#[.&':?#F%&'&M# Kinetic Energy = !! 1 2 mv 2 Q &.&':?#()#>',>,';,.!1#*,#< @#.,*#<# G,.)(9&'#*%&#F,'A#9,.�?#*%&#+,'-&# !! ! Work Done W = W =m ! (v + v 0 ) (v " v 0 ) 2 1 2 1 1 2 mv " mv 0 = m(v + v 0 )(v " v 0 ) 2 2 2 W = mv "v Z% What does the following equation tell us?! W = mv "v Suppose mass of a remote-control toy car is 1 kg, moving with an average speed of 10 m/s on the road, to make a 2 m/s change in speed, what is the required work by the engine? What happens when the average speed is 20 m/s? Case 1! !# 2 = 20J W = mv "v = 1#10 Case 2! W = mv "v = 1# 20 # 2 = 40J A lot more work needs to spent to bring the same speed change when the toy car moves with faster average speed.! ! Power is work over time, so need more power as well!! ! Energy Conversion: Energy cannot be created or destroyed in a closed system (careful: mechanical energy of an object can be lost due to frictional heating), but can be converted from one form to another.! [% \'*+>;%.*10<*9%M01/E1063'(% The fastest steam engine in the world is the Mallard which achieved a speed of 126mph (202 km/h) on 3rd July 1938 over a 5000 m stretch of track! !! !! The current electric trains operating on the same line today have a maximum speed of 225 km/h! ! Based on the following info, what was the power of the engine and the amount of coal burnt during the speed trial?! !! !! !! !! Coal contains 30MJ/kg chemical energy! The burning and heat extraction efficiencies were 80% and 50% respectively! The six coaches pulled gave a frictional force of 10000 N! -]% ! Power of the engine:! 1000 = 561 kW 3600 !!To calculate the coal burned we need to know the energy required! !! Work = Power x time ! 5000 W = 561,000 " " 3600 = 50 MJ 202,000 Now the conversion efficiency of the heat energy into mechanical work is 50% ! 50MJ Heat Energy Needed = = 100 MJ ! 50% The conversion efficiency of coal’s chemical energy into heat is 80% ! 100MJ Chem Energy Needed = = 125 MJ 80% ! So the total number of kg of coal needed:! 125MJ Chem Energy Needed = = 4.2 kg --% 30MJ/kg ! Power = Force " velocity = 10,000 " 202 " ! ! Forces and Potential Energy in 2D & 3D Partial derivatives (Math interlude) (and the differential criterion for determining whether a 2D/3D force is conservative) Suppose we have a function U of two variables x and y. Then we can ask “how fast” does U change in the x-direction and how fast does U change in the y-direction. So there are two natural rates of change, or two partial derivatives we can take: In practice, we compute partial derivatives exactly as you would an ordinary derivative except that you treat every variable as a constant except the one you are differentiating with respect to. "U = 2# y "y 1) Examples 2) 3) ! -J%