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初中物理部分中英文词汇对照表

初中物理部分中英文词汇对照表

初中物理部分中英文词汇对照表Ⅰ、测量(measurement)物理学physics测量measure (vt.)测量工具measuring tool测量范围measuring range最小刻度division value实验experiment实验室laboratory误差error刻度尺meter ruler零刻度线zero graduation line 长度length单位unit面积area千米kilometer米meter平方米square meter立方米cubic meter分米decimeter厘米centimeter毫米millimeter微米micron纳米nanometer时间time小时hour分钟minute秒second毫秒millisecond体积volume升Liter毫升Milliliter天平balance砝码weights游码rider质量mass吨ton 千克kilogram克gram毫克milligram停表stop watch 力force牛顿Newton测力计dynamometer弹簧秤spring balanceⅡ、运动(simple motion)相对运动relative motion方向direction位置position路程path静止rest参照物reference速度velocity平均速度average velocity直线运动rectilinear motion曲线运动curvilinear motion变速直线运动variable rectilinear motion 匀速直线运动uniform rectilinear motionⅡ、热(heat)温度temperature温度计thermometer摄氏度degree centigrade体温计clinical thermometer分子molecules分子运动molecular motion物质substance物体object状态state固体solid液体liquid气体gas物态变化state transformation晶体crystal非晶体noncrystal熔化melting凝固solidification熔点melting point凝固点solidifying point汽化vaporization蒸发evaporation沸腾boiling沸点boiling point液化liquefaction升华sublimation凝华condensation扩散diffusion吸引力attractive force排斥力repulsive force冰箱refrigerator热传递heat transfer热传导heat conduction热对流heat convection热辐射heat radiation吸收absorb(v.)放出release(v.)热量heat比热(容)specific heat (capacity)Ⅳ、光(light)光源light source光的直线传播rectilinear propagation of light均匀介质well-distributed medium光速velocity of light小孔成像image byping hole日食solar eclipse月食lunar eclipse光的色散dispersion of light平面镜plane mirror光的反射reflectionof light反射定律reflection law入射光线incident ray反射光线reflected ray法线normal镜面反射mirror reflection漫反射diffuse reflection入射角incident angle反射角reflection angle海市蜃楼mirage光的折射refractionof light 折射光线refracted ray折射角refraction angle光屏(屏幕)screen照相机camera潜望镜periscope幻灯机slide projector电影放映机film projector空气air真空vacuum蜡烛candle透镜lens凸透镜convex lens凹透镜concave lens会聚converge(v.)发散diverge(v.)焦距focal length焦点focus实像real image虚像virtual image(主)光轴principal optical axis 光心optical centerof lens放大的amplified缩小的reduced正立的erected倒立的inverted放大镜magnifier玻璃glass水waterⅤ、磁(magnetism)磁体magnet小磁针magneticneedle磁场magnetic field天然磁体natural magnet磁极magnetic pole地磁场geomagnetic field人造磁体man-made magnet南极north pole北极South pole电流的磁场magnetic field of electric current条形磁铁bar magnet磁感线magnetic induction line蹄形磁铁horseshoe magnet磁化magnetization电磁铁electromagnetⅥ、声音(sound)振动vibrate声波wave of sound振幅amplitude介质medium音调pitch噪音noise传播travel响度loudness乐音voice声速velocity of sound音色musical quality分贝decibel(dB)回声echo频率frequencyⅦ、力(force)重力gravity惯性inertia动力motive force重心center of gravity平衡equilibrium阻力resistance摩擦力friction force压强pressure动力臂power arm滑动摩擦sliding friction帕斯卡Pascal(Pa)阻力臂resisting arm滚动摩擦rolling friction液体压强hydraulicpressure作用线action-line静摩擦static friction 大气压强atmosphericof pressure滑轮pulley压力pressure force标准大气压standardatmospherepressure 定滑轮fixed pulley浮力buoyancy force气压计barometer动滑轮movable pulley力的图示force diagram托里拆利Torricelli滑轮组pulley block力的大小magnitude of force阿基米德原理Archimedes principle功work力的方向direction of force密度density功率power力的作用点acting point of force潜水艇submarine机械效率mechanical efficiency合力resultant force热气球fire balloon有用功useful work分力component force飞艇airship额外功extra wok力的合成composition of forces简单机械simple mechanics总功total work形变deformation杠杆lever斜面inclined plane牛顿第一定律Newton’s First Law支点pivotⅧ、电(electricity)电荷electric charge正极positive plate电压voltage带电体charged body负极negative plate伏特Volt摩擦起电electrificationby friction 电路electric circuit伏特计voltmeter正电荷positive charge通路closed circuit电阻resistance负电荷negative charge开路open circuit欧姆Ohm导体conductor短路short circuit变阻器rheostat绝缘体insulator电路图circuit map滑动变阻器slide wire rheostat 半导体semiconductor串联series connection欧姆定律Ohm’s law电源power source并联parallel connection电功electric work导线wire电量electric quantity电功率electric power电键key(switch)电流electric current额定电压rated voltage干电池dry cell安培Ampere额定电功率rated power蓄电池storage plate安培计ammeter。

高中物理功和能(功是能量转化的量度)公式大全

高中物理功和能(功是能量转化的量度)公式大全

高中物理功和能(功是能量转化的量度)公式大全功和能(功是能量转化的量度)1.功:W=Fscosα(定义式){W:功(J),F:恒力(N),s:位移(m),α:F、s间的夹角}2.电功:W=UIt(普适式) {U:电压(V),I:电流(A),t:通电时间(s)}3.重力做功:Wab=mghab {m:物体的质量,g=9.8m/s2≈10m/s2,hab:a与b高度差(hab=ha-hb)}4.电场力做功:Wab=qUab {q:电量(C),Uab:a与b之间电势差(V)即Uab=φa-φb}5.功率:P=W/t(定义式) {P:功率[瓦(W)],W:t时间内所做的功(J),t:做功所用时间(s)}6.电功率:P=UI(普适式) {U:电路电压(V),I:电路电流(A)}7.汽车牵引力的功率:P=Fv;P平=Fv平 {P:瞬时功率,P平:平均功率}8.汽车以恒定功率启动、以恒定加速度启动、汽车最大行驶速度(vmax=P额/f)9.动能:Ek=mv2/2 {Ek:动能(J),m:物体质量(kg),v:物体瞬时速度(m/s)}10.重力势能:EP=mgh {EP :重力势能(J),g:重力加速度,h:竖直高度(m)(从零势能面起)}11.电势能:EA=qφA {EA:带电体在A点的电势能(J),q:电量(C),φA:A点的电势(V)(从零势能面起)}12.焦耳定律:Q=I2Rt {Q:电热(J),I:电流强度(A),R:电阻值(Ω),t:通电时间(s)}13.纯电阻电路中I=U/R;P=UI=U2/R=I2R;Q=W=UIt=U2t/R=I2Rt14.动能定理(对物体做正功,物体的动能增加):W合=mvt2/2-mvo2/2或W合=ΔEK{W合:外力对物体做的总功,ΔEK:动能变化ΔEK=(mvt2/2-mvo2/2)}15.机械能守恒定律:ΔE=0或EK1+EP1=EK2+EP2也可以是mv12/2+mgh1=mv22/2+mgh216.重力做功与重力势能的变化(重力做功等于物体重力势能增量的负值)WG=-ΔEP注:(1)重力做功和电场力做功均与路径无关(见2、3两式);(2)功率大小表示做功快慢,做功多少表示能量转化多少;(3)重力(弹力、电场力、分子力)做正功,则重力(弹性、电、分子)势能减少(4)O0≤α<90O 做正功;90O<α≤180O做负功;α=90o不做功(力的方向与位移(速度)方向垂直时该力不做功);(5)机械能守恒成立条件:除重力(弹力)外其它力不做功,只是动能和势能之间的转化;(6)能的其它单位换算:1kWh(度)=3.6×106J,1eV=1.60×10-19J;。

大学物理第4章 功与能work and energy(1)

大学物理第4章  功与能work and energy(1)

2.动能的性质: 瞬时性;相对性
问题:
铅直下落的冰雹,质量为 m,某时刻的速率为v,试问从地 面上以速率v水平运动的车上观察,该冰雹的动能是多少?
(答案:mv2)
3.动能与动量的关系:
v v
v v
u
二 、动能定理 1. 质点的动能定理
合外力对质点所作的功, 等于质点动能的增量 .
质点运动的动能定理 合外力对质点所做的功等于质点动能的增量
典型的保守力: 重力、万有引力、弹性力 与保守力相对应的是非保守力,如摩擦力。
若质点沿任意闭合路径运动一周,保守力 对质点所做的功为零。



A保
Fdr l
Fdr ACB
F dr
BDA
F d r F d r
ACB
ADB
A C
解:(1)选择地球惯性系建立坐标系; (2)确定研究对象: 链条 设经时间 t 秒,链条下落 x (3)分析所受的力;重力和摩擦力 摩擦力:
f LL-- ax o
xa
(4)链条离开桌面过程中摩擦力所做的功
X
(5)下落过程重力做的功: (6)应用动能原理列方程解方程
链条刚刚离开桌面时的速率:
f L- x o x
例 一轻弹簧, 其一端 系在铅直放置的圆环的顶 点P,另一端系一质量为m 的小球, 小球穿过圆环并在 环上运动(μ =0).开始球 静止于点 A, 弹簧处于自然 状态,其长为环半径R; 当球运动到环的底端点B时,球对环没有压 力.求弹簧的劲度系数.
解 以弹簧、小球和 地球为一系统
只有保守内力做功 系统
P.229 4.15
一质量为 m 的物体,从质量为M的圆弧形槽顶由静止滑下, 圆弧形槽的半径为R,张角为 900 。如果所有摩擦可以忽略。

高中物理常用公式功和能转化公式

高中物理常用公式功和能转化公式

2019年高中物理常用公式功和能转化公式1.功:W=Fscos(定义式){W:功(J),F:恒力(N),s:位移(m),:F、s 间的夹角}2.重力做功:Wab=mghab {m:物体的质量,g=9.8m/s210m/s2,hab:a 与b高度差(hab=ha-hb)}3.电场力做功:Wab=qUab {q:电量(C),Uab:a与b之间电势差(V)即Uab=b}4.电功:W=UIt(普适式) {U:电压(V),I:电流(A),t:通电时间(s)}5.功率:P=W/t(定义式) {P:功率[瓦(W)],W:t时间内所做的功(J),t:做功所用时间(s)}6.汽车牵引力的功率:P=Fv;P平=Fv平{P:瞬时功率,P平:平均功率}7.汽车以恒定功率启动、以恒定加速度启动、汽车最大行驶速度(vmax=P额/f)8.电功率:P=UI(普适式) {U:电路电压(V),I:电路电流(A)}9.焦耳定律:Q=I2Rt {Q:电热(J),I:电流强度(A),R:电阻值(),t:通电时间(s)}10.纯电阻电路中I=U/R;P=UI=U2/R=I2R;Q=W=UIt=U2t/R=I2Rt11.动能:Ek=mv2/2 {Ek:动能(J),m:物体质量(kg),v:物体瞬时速度(m/s)}12.重力势能:EP=mgh {EP :重力势能(J),g:重力加速度,h:竖直高度(m)(从零势能面起)}13.电势能:EA=qA {EA:带电体在A点的电势能(J),q:电量(C),A:A点的电势(V)(从零势能面起)}14.动能定理(对物体做正功,物体的动能增加):W合=mvt2/2-mvo2/2或W合=EK{W合:外力对物体做的总功,EK:动能变化EK=(mvt2/2-mvo2/2)}15.机械能守恒定律:E=0或EK1+EP1=EK2+EP2也可以是mv12/2+mgh1=mv22/2+mgh216.重力做功与重力势能的变化(重力做功等于物体重力势能增量的负值)WG=-EP注:(1)功率大小表示做功快慢,做功多少表示能量转化多少;(2)O090O 做正功;90O180O做负功;=90o不做功(力的方向与位移(速度)方向垂直时该力不做功);(3)重力(弹力、电场力、分子力)做正功,则重力(弹性、电、分子)势能减少(4)重力做功和电场力做功均与路径无关(见2、3两式);(5)机械能守恒成立条件:除重力(弹力)外其它力不做功,只是动能和势能之间的转化;(6)能的其它单位换算:1kWh(度)=3.6106J,1eV=1.6010-19J;*(7)弹簧弹性势能E=kx2/2,与劲度系数和形变量有关。

大学物理英文版PPT

大学物理英文版PPT

4.Units 单位
International System of Units SI: Syst me International d’Unit s 法语 is used in China
mass
m
kg:千克 kilogram
length
L m:米 meter
Time
t s:秒 second
5. Scalar and vector 标量和矢量 : Two types of physical quantities 量 :
主要讲授内容:
经典力学 相对论
电磁学
振动与波动 日常生活
波动光学
热学
量子论简介
puter 计算机科学
Medicine 医学
Physics
Chemistry 化学
Mechanics 机械学
Biology 生物学
Physics: fundamentals and methods.
References 参考书
主要贡献: •发明了望远镜,维护、坚持和发展了哥白尼学说, 发现木星的四个卫星; •摆的等时性、惯性定律、落体运动定律; •运动的合成原理和独立性原理,相对性原理; •方法:实验科学。
§1-1 Frame of Reference Particle 质点
1. Frame of Reference 参照系
C=A+B B
A
B C
A
In Cartesi an coordinate system 直角坐标系 :
A A xiA yjA zk
i,jankd are unit vectors along OX,OY,OZ Y
O
X
Z

功与能的转换关系

功与能的转换关系

功与能的转换关系人们常常谈论“得到的回报与所做的付出成正比”,这句话其实道出了功与能的转换关系。

功和能量是物理学中重要的概念,二者之间存在着密不可分的联系和相互转换的关系。

本文将围绕功与能的转换关系展开论述。

一、什么是功和能首先,我们来阐述功和能的概念。

在物理学中,功(Work)是指力在物体上产生的作用,可以理解为力对物体的改变。

功的大小等于力乘以移动的距离。

例如,我们抬起一本书并将其放在书架上,这一过程中我们所施加的力对书做了功。

能量(Energy)则是物体存储的做功的能力。

它是物体的固有属性,可以进行传递、转换和储存。

物体的能量可以分为多种形式,包括动能、势能、热能等。

二、接下来,我们来探讨功与能的转换关系。

功与能之间的转换关系可以归结为两个方面:能转化为功,功也能转化为能。

首先是能转化为功的过程。

当物体具有能量时,可以将这种能量用于对其他物体做功。

例如,我们把一颗弹簧拉到一定距离,这时弹簧具有弹性势能。

如果释放弹簧,它会向前弹起,将潜在能转化为动能,对其他物体做功。

再比如,我们把一个球球扔到空中,球球上升的过程中动能逐渐减小,而高度增加,最终转化为势能。

球球下落时,势能又逐渐转化为动能,对地面做功。

其次是功转化为能的过程。

当力对物体做功时,物体获得了能量。

比如,我们用力推动自行车,这时我们对自行车做功,把化学能转化为机械能。

同样,我们给手机充电时,电源对手机做功,将电能转化为储存在电池中的化学能。

三、功与能的守恒与转化此外,我们还需要了解功与能的守恒与转化。

根据能量守恒定律,能量在任何情况下都是守恒的,即能量不会凭空消失或产生。

在物体间的相互转化过程中,总能量保持不变。

功与能的转化也反映了能量保存定律。

当物体之间进行能量转化时,总的能量是不变的。

功和能量可以在不同形式之间相互转换,但总的能量守恒。

四、功与能的应用功与能的转换关系在生活和科学研究中有着广泛的应用。

能量转化的过程也是许多工具和装置的基础原理。

高三物理《功和能转化》公式总结

高三物理《功和能转化》公式总结

高三物理《功和能转化》公式总结功:=Fscosα{:功,F:恒力,s:位移,α:F、s间的夹角}重力做功:ab=ghab{:物体的质量,g=9.8/s2≈10/s2,hab:a与b高度差}电场力做功:ab=qUab{q:电量,Uab:a与b之间电势差即Uab=φa-φb}电功:=UIt{U:电压,I:电流,t:通电时间}功率:P=/t{P:功率[瓦],:t时间内所做的功,t:做功所用时间}汽车牵引力的功率:P=Fv;P平=Fv平{P:瞬时功率,P平:平均功率}汽车以恒定功率启动、以恒定加速度启动、汽车最大行驶速度电功率:P=UI{U:电路电压,I:电路电流}焦耳定律:Q=I2Rt{Q:电热,I:电流强度,R:电阻值,t:通电时间}0.纯电阻电路中I=U/R;P=UI=U2/R=I2R;Q==UIt=U2t/R=I2Rt1.动能:E=v2/2{E:动能,:物体质量,v:物体瞬时速度}重力势能:EP=gh{EP:重力势能,g:重力加速度,h:竖直高度}3.电势能:EA=qφA{EA:带电体在A点的电势能,q:电量,φA:A点的电势}动能定理:合=vt2/2-vo2/2或合=ΔE{合:外力对物体做的总功,ΔE:动能变化ΔE=}机械能守恒定律:ΔE=0或E1+EP1=E2+EP2也可以是v12/2+gh1=v22/2+gh2重力做功与重力势能的变化G=-ΔEP注:功率大小表示做功快慢,做功多少表示能量转化多少;o0≤α<90o做正功;90o<α≤180o做负功;α=90o不做功方向垂直时该力不做功);重力做正功,则重力势能减少重力做功和电场力做功均与路径无关;机械能守恒成立条件:除重力外其它力不做功,只是动能和势能之间的转化;能的其它单位换算:1h=3.6×106j,1eV=1.60×10-19j;*弹簧弹性势能E=x2/2,与劲度系数和形变量有关。

大学物理 功和能汇总

大学物理 功和能汇总
0 1
2 动能定理: A 1 2 mv 0
2A v 4 m s m
[思考] 在 x =0 至 x =1m 过程中, F 的冲量?
10
§4.3 质点系的动能定理
Theorem of Kinetic Energy for a system of Particle
对第 i 质点 求和
O 张力不做功,重力做功: 用动能变化定理解:

l
m
T

A mg dl mg dl cos
mgl cos d mgl sin 0 1 2 mgl sin mv 2


ˆn e

v
mg
ˆt e
比直接解牛顿方程简单,但仍作积分运算。
13
§4.4 *柯尼希定理
i
14
一对力 的功
内力总是成对出现 dr1 两质点间的内力 f ij 和 f ji ,
B1
B2
dr2
f 12
称为一对力 f ij f ji
m1
r21
f 21
m2
A1
A2
一对力做的功之和
dA = f12 dr1 + f21 dr2
f 21 dr2 dr1 f 21 dr21
mi ac dri
m i ac
z
y
mi
= ac mi dri
ri
ac
C 质心 O
12
= ac d mi ri = 0 A i
B
x
=
0
【例】柔软细绳长为l,小球质量为m,求摆下至 角时小球的速度和绳的张力。

关于功和能的高二物理公式

关于功和能的高二物理公式

关于功和能的高二物理公式 高中各科目的学习对同学们提高综合成绩非常重要,大家一定要认真掌握,小编为大家整理了关于功和能的高二物理公式,希望同学们学业有成!1.功:W=Fscos(定义式){W:功(J),F:恒力(N),s:位移(m),:F、s间的夹角}2.重力做功:Wab=mghab {m:物体的质量,g=9.8m/s210m/s2,hab:a与b高度差(hab=ha-hb)}3.电场力做功:Wab=qUab {q:电量(C),Uab:a与b之间电势差(V)即Uab=b}4.电功:W=UIt(普适式) {U:电压(V),I:电流(A),t:通电时间(s)}5.功率:P=W/t(定义式) {P:功率[瓦(W)],W:t时间内所做的功(J),t:做功所用时间(s)}6.汽车牵引力的功率:P=Fv;P平=Fv平 {P:瞬时功率,P平:平均功率}7.汽车以恒定功率启动、以恒定加速度启动、汽车最大行驶速度(vmax=P额/f)8.电功率:P=UI(普适式) {U:电路电压(V),I:电路电流(A)}9.焦耳定律:Q=I2Rt {Q:电热(J),I:电流强度(A),R:电阻值(),t:通电时间(s)}10.纯电阻电路中I=U/R;P=UI=U2/R=I2R;Q=W=UIt=U2t/R=I2Rt11.动能:Ek=mv2/2 {Ek:动能(J),m:物体质量(kg),v:物体瞬时速度(m/s)}12.重力势能:EP=mgh {EP :重力势能(J),g:重力加速度,h:竖直高度(m)(从零势能面起)}13.电势能:EA=qA {EA:带电体在A点的电势能(J),q:电量(C),A:A点的电势(V)(从零势能面起)}14.动能定理(对物体做正功,物体的动能增加):W合=mvt2/2-mvo2/2或W合=EK{W合:外力对物体做的总功,EK:动能变化EK=(mvt2/2-mvo2/2)}15.机械能守恒定律:E=0或EK1+EP1=EK2+EP2也可以是mv12/2+mgh1=mv22/2+mgh216.重力做功与重力势能的变化(重力做功等于物体重力势能增量的负值)WG=-EP注:(1)功率大小表示做功快慢,做功多少表示能量转化多少;(2)O090O 做正功;90O180O做负功;=90o不做功(力的方向与位移(速度)方向垂直时该力不做功);(3)重力(弹力、电场力、分子力)做正功,那么重力(弹性、电、分子)势能减少(4)重力做功和电场力做功均与路径无关(见2、3两式);(5)机械能守恒成立条件:除重力(弹力)外其它力不做功,只是动能和势能之间的转化;(6)能的其它单位换算:1kWh(度)=3.6106J,1eV=1.6010-19J;*(7)弹簧弹性势能E=kx2/2,与劲度系数和形变量有关。

《物理双语教学课件》Chapter 4 Work and Energy 功和能

《物理双语教学课件》Chapter 4 Work and Energy 功和能

Chapter 4 Work and EnergyThe concept of energy is one of the most important in the world of science. In everyday usage, the term energy has to do with the cost of fuel for transportation and heating, electricity for lights and appliances, and the foods we consume. However, these ideas do not really define energy. They tell us only that fuels are needed to do a job and that those fuels provide us with something we call energy.Energy is present in the Universe in a variety of forms, including mechanical energy, chemical energy, electromagnetic energy, heat energy, and nuclear energy. Although energy can be transformed from one form to another, the total amount of energy in the Universe remains the same. If an isolated system loses energy in some form, then by the principle of conservation of energy, the system must gain an equal amount of energy in other form. The transformation of energy from one form into another is an essential part of the study of physics, chemistry, biology, geology, and astronomy.In this chapter we are concerned only with mechanical energy. We introduce the concept of kinetic energy, which is defined as the energy associated with motion, and the concept of potential energy, the energy associated with position. We shall see that the ideas of work and energy can be used in place ofNewton’s law to solve certain problems.4.1 Work and Power1. Work W done by a constant force is defined as the product of the component of the force along the direction of displacement and the magnitude of the displacement.ϕcos FS S F W =⋅=Where the force makes an angle of ϕ with displacement .SThe SI unit of work is the joule (J), named for James Prescott Joule, an English scientist of the 1800s. It is derived directly from the units for mass and velocity:1joule=1J=1(kg) (m/s 2) (m)=1 kg m 2/s 22. Work done by a variable force(1). The increment of work dW done on the particle by F during the displacement d r isr d F dW ⋅=, where Force F is function of its position.(2). The work W done by F while the particle moves from an initial position a to a final position b is then⎰⎰⋅==b a b a r d F dW W(3). We use the components ofF and r d to express the forceand displacement, then we havedzF dy F dx F k dz j dy i dx k F j F i F r d F W z y b a x z y b a x b a ++=++⋅++=⋅=⎰⎰⎰)()( 3. Work done by multiple forces : If there are several forces act on a particle, we can replace F in above equation with the net force ∑F , where +++=∑321F F F F , where j F are theindividual forces. Then+++=⋅+++=⋅=⎰⎰321321)(W W W r d F F F r d F W b aba 4. Power(1). The rate at which work is done by a force is said to be the power due to the force . If an amount of work W is done in a time intervalt ∆ by a force, then the average power due to the force is t WP ∆=.(2). The instantaneous power P is the instantaneous rate of doing work, which can be written asv F dtr d F dt dW P ⋅=⋅==. (3). The SI unit of power is the joule per second . This unit is used so often that it has a special name, the watt (W), after James Watt, who greatly improved the rate at which steam engines could do work.4.2 Kinetic Energy and Work-Kinetic Energy TheoremEnergy is a scalar quantity that is associated with a state of oneor more object. The term state here has its common meaning: it is the condition of an object.1. Kinetic energy K is associated with the state of motion of an object. The faster the object moves, the greater is its kinetic energy. For an object of mass m and whose speed v is well below the speed of light , we define kinetic energy as 221mv K = The SI unit of kinetic energy is the same as work —joule.A convenient unit of energy for dealing with atoms or with subatomic particles is the electron-volt (eV).1 electron-volt = 1 eV =1.60 x 10 –19 J.2. Work-kinetic energy theorem : If a force changes the speed of an object, it also changes the kinetic energy of the object. If the kinetic energy is the only type of energy of the object being changed by the force, then the change in kinetic energy is equal to the work W done by the force:W K K K i f =-=∆ Here i K is the initial kinetic energy (=2021mv ) and f K is the kinetic energy (221mv ) after the work is done.3. We can prove work-kinetic energy theorem as follow:002022222221212121)(21k f v v b a z y x z z y y x x b a b a b a K K mv mv v m mvdv W dv v v v d dv v dv v dv v v d v v d v m dt v dtv d m s d f W -=-====++=++=⋅⋅=⋅⋅=⋅=⎰⎰⎰⎰(Numerator and denominator of a fraction)4.3 Work done by weight and by a spring force1. Work done by weight :[]a b a b b a b a m gh m gh h h m g dh m g dW W m gdhm gdl m gdl l d g m dW --=--=-==-=--==⋅=⎰⎰)()cos(cos απαWe can find that the work done by weight on a particle between two points does not depend on the path taken by the particle . Or no matter what path we choose to move the particle, the work done by its weight is the same . In other word if we move a particle around a closed path, the work done by weight on the particle is zero .2. Work done on aparticle-like object by aparticular type of variableforce, namely, springforce —the force exertedby a spring.⎥⎦⎤⎢⎣⎡--=-=-==-=⋅=-=⎰⎰222212121'a b x x x x b a kx kx x k kxdx dW W kxdxs d F dW law s Hook kx F b a b a 3. Conservative force and Non-conservative force : If the workdone by the force is independent of the path the particle moves,the force is a conservative force ; otherwise a non-conservative force . Weight and spring-force are conservative forces; friction is a non-conservative force.4.4 Potential energyPotential energy U is energy that can be associated with the configuration (or arrangement) of a system of objects that exert a force on one another. If the configuration of the system changes, then the potential energy of the system also changes.1. We know that work done by a conservative force has nothing to do with the path the particle taken. So we can introduce a quantity which is the function of the state of the system to indicate this kind of nature for a conservative force. We call it potential .2. Gravitational Potential Energy(1). The work done by weight can be expressed as: []U mgh mgh W a b ∆-=--==, where U ∆ is the change in the gravitational potential energy. Since the work done by weight has definite magnitude from an initial position to a final position, so only a changeU ∆ in gravitational potential energy is physically important .(2). However, to simplify a calculation or a discussion, we cansay that a certain gravitational potential U is associated with any given configuration of the system, with the particle at a given height h. To do so, we rewrite the above equation as:)(i i h h mg U U -=-Then we take i U to be the gravitational potential energy of thesystem when it is in a reference configuration, with the particle at a reference pointi h . Usually, we set 0=i U and 0=i h , then we have mgh U =. So the gravitational potential energy associated with a particle-Earth system depends on the height h of the particle relative to the reference position of h i =0, not the horizontal position.3. Elastic Potential Energy(1). Similar to a particle-Earth system, the work done by the spring force can be rewritten as U kx kx W a b ∆-=⎥⎦⎤⎢⎣⎡--=)21()21(22.(2). To associated a potential energy U with any given configuration of the system, with the block at position x, we set the reference point for the block as x i =0, which is always at the equilibrium position of the block. And we set the corresponding elastic potential energy of the system as U i =0. Thus we have 221)(kx x U =. Attention: (1). Potential energy belongs to the whole system.(2). The magnitude of potential energy depends onthe choice of the reference point.4.5 Work-Energy Theorem and Conservation of Mechanical Energy1. Work-kinetic energy theorem for one particle: We have W K K K i f =-=∆2. Work-Energy Theorem: Suppose we have particles of N in the system we discussed and we use work-kinetic energy theorem for each particle, then we have total amount of N equations like those:jijf j if if K K W K K W K K W -=-=-=222111We can divide the forces exerted on every particle into external forces and internal forces. And the internal forces can also be classified as conservative internal forces and non-conservative forces. Summing the two side of above equations, we will have: i fN j ji jf N j j K K K K W -=-=∑∑==11)(Or to be exactly,K W W W noncon in con in ext ∆=++--We also know that the work done by the conservative internalforce can be written as the minus difference of potential energy. So we get the Work-Energy Theorem :E U K W K W W con in noncon in ext ∆=∆+∆=-∆=+--The work done by external forces and non-conservative internal forces in a given system is exactly equal to the difference of its Mechanical Energy .3. Conservation of Mechanical Energy : When only conservative forces act within a system, the kinetic energy and potential energy can change. However, their sum, the mechanical energy E of the system, does not change . 0=∆+∆=∆U K E4.6 Reading a Potential energy curveConsider a particle that is part of a system in which a conservative force acts. Suppose that the particle is constrained to move along an x axis while the conservative force does work on it.1. Finding the Force Analytically : For one-dimensional motion, the work W done by a conservative force that acts on a particle as the particle moves, and the potential energy have the relation as followdx x F dW x U )()(-=-=∆So can get the force from the potential energytion ensionalmo one dx x dU x F dim )()(--=We can, for example, check this result by putting221)(kx x U =, which is the elastic potentialenergy function for a springforce. Above equation yieldskx x F -=)( as expected.2. The Potential EnergyCurve : The following figureis a plot of a potential energyfunction U(x) for a system inwhich a particle is inone-dimensional motionwhile a conservative forceF(x) does work on it. We caneasily find F(x) by taking theslope of the U(x) curve atvarious points. Fig. (b) is a plot of F(x) found in this way.3. Tuning Point : Since there is only conservative force acting on the particle, the system will remain conservation of its mechanical energy. So we have)()(x U E x K -=. Since kinetic energy)(x K is not less than zero. As the particle moves from 2xto 1x (Fig. a), when the particle reaches 1x , its kineticenergy is zero, meanwhile the force on the particle is positive. It means the particle does not remain atx but instead begins to1move back to the right. Hencex is a tuning point, a place1where K=0 and the particle changes direction of its motion.4.Equilibrium Points:Neutral equilibriumUnstable equilibriumStable equilibrium。

高二物理下学期机械能(English-vertion)--牛津英语

高二物理下学期机械能(English-vertion)--牛津英语
4. A 2kg mass is pulled up by a string that passes over a smooth light pulley as shown opposite .if the hand moves through a 0.5m in the shown direction. What’s the gain in PE of the block ?
2. formula : PE= mgh 3. unit : joule (J) 4. note :
△PE=mg△h=mgh1- mgh2 (△PE is independent of the path ,just depends on the h1 -h2
㈢.
㈣.
1. A 5kg object is initially traveling alone a frictionless surface at a velocity of 2m.s-1, it is pushed by a 3n force in the direction of motion for a distance of 4m. What’s the KE of the project after the push ?
3. In a construction site ,a block with a mass of 50kg is raised slowly upward by a crane though a vertical distance of 3 m. (a). What is the work done by the crane ? (b). what is the gain in PE of the block ?
2. A 2Kg mass moves across a rough surface with a frictional force of 2N at 4 m.s-1 ,

初中物理说课稿全英文版

初中物理说课稿全英文版

初中物理说课稿全英文版1. IntroductionIn this lesson, we will be discussing an English version of the lesson plan for teaching middle school physics. The aim of this lesson is to introduce basic physics concepts to middle school students and promote their understanding of the subject. The lesson will be delivered in an engaging and interactive manner to ensure students' active participation and effective learning.2. Lesson ObjectivesThe objectives of this lesson are as follows:- To introduce the concept of force and its characteristics.- To explain the relationship between force, mass, and acceleration.- To demonstrate the application of Newton's laws of motion in real-life situations.- To enhance students' critical thinking and problem-solving skills through hands-on activities and experiments.3. Teaching StrategiesTo achieve the objectives of this lesson, the following teaching strategies will be employed:- Use of multimedia presentations, diagrams, and visual aids to enhance understanding.- Engage students in group discussions and encourage them to ask questions to promote active learning.- Conduct hands-on experiments to allow students to experience and observe the principles of physics firsthand.- Provide real-life examples and case studies to help students understand the practical applications of physics concepts.4. Lesson ContentThe lesson will be divided into the following sections:4.1 Introduction to Force- Definition of force and its units of measurement.- Discussion on different types of forces, such as friction, gravity, and magnetism.- Examples of forces in everyday life.4.2 Newton's Laws of Motion- Explanation of Newton's three laws of motion.- Illustration of the relationship between force, mass, and acceleration.- Application of the laws of motion in different scenarios.4.3 Hands-on Activities and Experiments- Conducting experiments to demonstrate the effects of different forces.- Engaging students in hands-on activities to understand the concepts of force, mass, and acceleration.- Analyzing the results of the experiments and discussing their implications.5. ConclusionIn conclusion, this lesson aims to provide middle school students with a solid foundation in physics by introducing them to the basic concepts and principles of the subject. Through interactive teaching strategies and hands-on activities, students will be able to develop a deeper understanding of force, motion, and the laws governing them. Bythe end of the lesson, students should be able to apply their knowledge to real-life situations and appreciate the role of physics in our daily lives.。

高中物理第二册功和能

高中物理第二册功和能

p
k
2
功能
(gōngnéng)
关系
功是能量转化的量度——W=△E
动能定理:
W合
1mv2 1mv2 2t 20
机械能 守恒定律
mgh 1m2v mgh 1m2
1
第三页,共二十二页。
21
2 2
2
功:W=FScos

功 和能 能
功率(gōnPglǜ): WFvcos
t
动能 : E (dòngnénkg)
3.20×103kw, 已 知 该 发 电 站 水 库 面 积 为
S=2.50×106m2 , 电 站 的 总 效 率 为 10% , 则 每 次 涨 、
落潮的平均潮差是___m。则该电站每天平均满 负荷发电的时间为___h。
第十九页,共二十二页。
❖分析(fēnxī):年总发电量除以365再除以4,得每
1mv2 1mv2 2t 20
机械能
守恒定律
mgh 1m2v mgh 1m2
1
第六页,共二十二页。
21
2 2
2
功:W=FScos

功 和能 能
功率(gōP nglǜ): WFvcos
t
动能 : E (dòngnénkg)
1 mv2 2
势能:重力势能 E mgh p
机械能:EEEmgh 1m2v
第一页,共二十二页。
请您欣赏(xīnshǎng
功:W=FScos

功 和能 能
功率(gōnPglǜ): WFvcos
t
动能 : E (dòngnénkg)
1 mv2 2
势能:重力势能 E mgh p
机械能:EEEmgh 1m2v

「高中三年级物理必修二要点」功和能转化公式

「高中三年级物理必修二要点」功和能转化公式

「高中三年级物理必修二要点」功和能转化公式高考考试角逐异常激烈,千军万马争过独木桥,秋季到了,而你正以凌厉的节奏迈进这段特别的岁月中。

这是一段青涩而又平淡的日子,每一个人都隐身于高考考试,而平淡之中的张力却只有真的的勇士才可以破译。

为了帮你一臂之力,高中频道为你精心筹备了《高中三年级物理必修二要点:功和能转化公式》帮你金榜题名!1.功:W=Fscosplayα{W:功,F:恒力,s:位移,α:F、s间的夹角}2.重力做功:Wab=mghab{m:物体的水平,g=9.8m/s2≈10m/s2,hab:a与b高度差}3.电场力做功:Wab=qUab{q:电量,Uab:a与b之间电势差即Uab=φa-φb}4.电功:W=UIt{U:电压,I:电流,t:通电时间}5.功率:P=W/t{P:功率[瓦],W:t时间内所做的功,t:做功所用时间}6.汽车牵引力的功率:P=Fv;P平=Fv平{P:瞬时功率,P平:平均功率}7.汽车以恒定功率启动、以恒定加速度启动、汽车*大行驶速度8.电功率:P=UI{U:电路电压,I:电路电流}9.焦耳定律:Q=I2Rt{Q:电热,I:电流强度,R:电阻值,t:通电时间}10.纯电阻电路中I=U/R;P=UI=U2/R=I2R;Q=W=UIt=U2t/R=I2Rt11.动能:Ek=mv2/2{Ek:动能,m:物体水平,v:物体瞬时速度}12.重力势能:EP=mgh{EP:重力势能,g:重力加速度,h:竖直高度}13.电势能:EA=qφA{EA:带电体在A点的电势能,q:电量,φA:A 点的电势}14.动能定理:W合=mvt2/2-mvo2/2或W合=ΔEK{W合:外力对物体做的总功,ΔEK:动能变化ΔEK=}15.机械能守恒定律:ΔE=0或EK1+EP1=EK2+EP2也可以是mv12/2+mgh1=mv22/2+mgh216.重力做功与重力势能的变化WG=-ΔEP注:功率大小表示做功快慢,做功多少表示能量转化多少;O0≤α重力做正功,则重力势能降低重力做功和电场力做功均与路径无关;机械能守恒成立条件:除重力外其它力不做功,只是动能和势能之间的转化;能的其它单位换算:1kWh=3.6×106J,1eV=1.60×10-19J;*弹簧弹性势能E=kx2/2,与劲度系数和形变量有关。

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Calculate the work by the force when the particle moves from x1=2(m) to x2=3(m) in the following cases: 1. The trajectory is a parabola
Example
x 4y
2
2. The trajectory is a straight line 4 y x 6
Work is a scalar, no direction. π positive work; 0 d W 0 ,
π 2 π 2 π 2 dW 0 , d W 0,
Constant Force (including its direction)
A
rA
o
s
(2) Work done by a varying force: When a particle moves from A to B along a curve path, the total work ds done by the force equals the integral of F from A to B: A
7-1 Work and Power (P147-)
1. Work
研究力和运动的空间过程关系。
The work done by a force F in displacing a s body s as the scalar product of F and s.
W F r cos F r
1
2
O
3 X
A1
( Fx dx Fy dy ) 2 ydx 4dy
x1 y1 2 94 1
x2
y2
( x / 2)dx 4dy 10 . 8 J
2
Work depends on path.
A2
x2 , y 2 x1 , y1 3
( Fx dx Fy dy) 2 ydx 4dy
L1 m1
f12 Force on m1 by m2
o
L2
dA f12 dr12 f 21 dr21
dA f12 dr12 f 21 dr21
We have used this conclusion before Work by pair of normal forces
W1 W2 W3 Fra bibliotekThe work done by several forces = algebraic sum of the work done by the individual force. (4) Special expression in scalar product: F Fx i Fy j Fz k , and dr dxi dy j dzk .
Y x2 4 y
4y x 6
2.25
1
2
O
3
X
5
Solution:
Fx dx Fy dy Fz dz 4 y x 6
b a
A
B
A
F dr
2.25
Y x2 4 y
F 2 yi 4 j ( N )
x2 , y 2 x1 , y1 3
zero work; negative work.
Explanations:
s rB rA —displacement from A to B
(1) If the force is constant in the whole path, B A W F dr F (rB rA ) F s
f12 ,
f12
r1
f21
f 21
m2 r2
d r12 Displacement of m1 w.r.t to m2
f12 dr1 f12 dr2 f12 (dr1 dr2 ) f12 dr12
f12 f 21
x1 y1 94 1
x2
y2
( x 6) / 2dx 4dy 21 .25 J
2
Work of a pair of forces Interaction force between m1 and m2
dA dA1 dA2 f12 dr1 f 21 dr2
W dW
A B B A
rB
B
F
B
F
F dS
Work is dependant on the reference frame.
(3) Work done by several forces:
If F F1 F2 F3 F4 W F d r F1 d r F2 dr F3 dr
W
B A xi
B F dr ( Fx dx F y dy Fz dz )
A

xf
F x dx
yf yi
F y dy Fz dz
zi
zf
(5) Geometrical representation of work: F The work done by a force equals the area under the F versus x curve —— 变力曲线与 x1 dx 位移轴在两点x1, x2 之间所包围的面积.
F F x F
x
x2
x
x
W>0
W<0
W=0
(6) Unit of work: Dimension is: MLT –2 L= M L2 T –2
In SI system, 1 N· m = 1J (joule) = 1kg· m2/s2
The force on the particle is F 2 yi 4 j ( N )
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