Honors Physics I - 2 Force and Motion

Relative Motion

Galilean transformation :

  • xPA=xPB+xABx_{PA}=x_{PB}+x_{AB}

Projectile motion

x=v0cos⁡θ ty=y0+v0sin⁡θ t−12gt2=0R=v02gsin⁡2θ0x=v_0\cos\theta\, t\\ y=y_0+v_0\sin\theta\,t-\frac 1 2gt^2=0\\ R=\frac {v_0^2}g\sin2\theta_0

‪Projectile Motion‬

image-20260908092542699

Uniform Circular motion

a=v2Ra=\frac {v^2}R


*Basic Calculus

Derivative

df(x)dx=lim⁡Δx→0f(x+Δx)−f(x)Δx\frac{df(x)}{dx}=\lim_{\Delta x \to 0}\frac{f(x+\Delta x)-f(x)}{\Delta x}

Some examples :

ddxln⁡x=1x\frac{d}{dx}\ln x=\frac 1 x

Proof :

image-20260908101247428

Note that :

e=lim⁡n→+∞(1+1n)ne = \lim_{n\to +\infty}(1+\frac 1 n)^n

  • ddx(uv)=udvdx+vdudx\dfrac{d}{dx}(uv)=u\dfrac{dv}{dx}+v\dfrac{du}{dx}

For θ∈(0,π2)\theta \in (0,\frac{\pi}2) :

sin⁡θ<θ<tan⁡θ\sin \theta<\theta<\tan \theta

Therefore : ddxsin⁡x=cos⁡x\frac d {dx}\sin x=\cos x (Try!)

  • Chain Rules

image-20260908101218550

Integration

Use the partition. Fundamental Theorem of Calculus :

∫0xf(t)dt=lim⁡N→+∞∑i=1Nf(ti)Δt\int_0^xf(t)dt=\lim_{N\to +\infty}\sum_{i=1}^Nf(t_i)\Delta t

image-20260908101209848

Force and Emotion

  • Newton’s first law : If no force acts on a body, the body’s velocity cannot change; that is , the body cannot accelerate (Works in inertial reference frame)

  • Newton’s second law : The net force on a body is equal to the product of the body’s mass and its acceleration.

    Unit : N (Newton) =kg×m/s2=\text{kg}\times\text{m/s}^2

    Internal force is the force between two objects in the system.

    Remember to put the total force and direction (or the vector or even draw or figure) for you answer

Special Force

  • Gravitational force
  • Normal force
  • Friction and tension (a cord pulled taut)

  • Newton’s third law : When two bodies interact, the forces on the bodies from each other are always equal in magnitude and opposite in direction

Friction

Resistivity : 电阻 (superconductor)

  • static frictional force
  • kinetic frictional force

Why the maximum static frictional force is a bit larger than the kinetic frictional force :

When the body is static, it is more likely to track at the lower potential

μs\mu_s is the coefficient static friction.

The Drag Force and Terminal Speed

An empirical law of fluid, the drag force is

D=12CρAv2D=\frac 1 2C\rho Av^2

Where :

  • vv is the relative velocity
  • ρ\rho is the air density (mass/volume)
  • CC is the experimentally determined drag coefficient
  • AA is the effective cross-sectional area of the body (the area taken perpendicular to the relative velocity)

In reality, CC is not constant for all values of vv.


For a falling object :

D−Fg=masD-F_g=ma_s

In this case : vt=2FgCρAv_t=\sqrt{\dfrac{2F_g}{C\rho A}}, which is called the terminal speed

Uniform Circular Motion

a=v2R    (centripetal acceleration)F=mv2Ra=\frac{v^2}R\;\;\text{(centripetal acceleration)}\\ F=\frac{mv^2}R