Physics 1

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17 Terms

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What is the first step in understanding physical processes?

Physical processes are observed and measured both quantitatively and qualitatively.

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What does the observation step of a physical process necessarily include?

The conception and definition of appropriate quantities by which measurements may be made.

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In what form is a hypothesis usually offered in physics?

In the form of a general principle or a mathematical statement of relationships between physical quantities.

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What is the primary use of physical principles or relationships?

They can be used to predict the results of other similar physical processes.

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What is considered the working language of physics?

Mathematics.

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What specific mathematical fields are noted as necessary for mastering physics?

Analytic geometry, calculus, trigonometry, and vector analysis.

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Instantanenous Acceleration

Formula: ax=dvxdt=d2xdt2a_x = \frac{dv_x}{dt} = \frac{d^2x}{dt^2}

(ax [m/s2],vx [m/s],t [s]a_x\text{ [m/s}^2\text{]}, v_x\text{ [m/s]}, t\text{ [s]} )



General 1D motion with differentiable vx(t)v_x(t)


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Velocity-Time Relation

vx=v0x+axtv_x = v_{0x} + a_x t



(v0x,vx [m/s],ax [m/s2],t [s]v_{0x}, v_x\text{ [m/s]}, a_x\text{ [m/s}^2\text{]}, t\text{ [s]})


Constant 1D acceleration (ax=consta_x = const)

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Position-Time-Relation

x=x0+v0xt+12axt2x = x_0 + v_{0x}t + \frac{1}{2}a_x t^2


(x0,x [m],v0x [m/s],ax [m/s2],t [s]x_0, x\text{ [m]}, v_{0x}\text{ [m/s]}, a_x\text{ [m/s}^2\text{]}, t\text{ [s]})


Constant 1D acceleration (ax=consta_x = \text{const})

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Timeless Kinematic Relation

vf2=vi2+2aΔxv_{f}^2=v_{i}^2+2a\Delta x


(v0x,vx [m/s],ax [m/s2],Δx [m]v_{0x}, v_x\text{ [m/s]}, a_x\text{ [m/s}^2\text{]}, \Delta x\text{ [m]} )



Constant 1D acceleration (tt unknown)

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Average velocity displacment

Δx=12(v0x+vx)t\Delta x = \frac{1}{2}(v_{0x} + v_x)t


(Δx [m],v0x,vx [m/s],t [s]\Delta x\text{ [m]}, v_{0x}, v_x\text{ [m/s]}, t\text{ [s]})



Constant 1D acceleration (axa_x unknown)

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Free-Fall Kinematics (+y+yup)

y=y0+v0yt−12gt2y = y_0 + v_{0y}t - \frac{1}{2}gt^2


(y [m],v0y [m/s],g=9.80 m/s2y\text{ [m]}, v_{0y}\text{ [m/s]}, g = 9.80\text{ m/s}^2)


Negligible air resistance near Earth surface


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General Calculus Integration

vx(t)=v0x+∫0tax(t′)dt′v_x(t) = v_{0x} + \int_0^t a_x(t') dt'



(ax(t) [m/s2],vx(t) [m/s]a_x(t)\text{ [m/s}^2\text{]}, v_x(t)\text{ [m/s]})


Time-dependent acceleration ax(t)a_x(t)



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Average Velocity

vˉ=ΔxΔt=xf−xitf−ti\bar{v} = \frac{\Delta x}{\Delta t} = \frac{x_f - x_i}{t_f - t_i}



vˉ (average velocity)Δx (displacement)Δt (time interval)xf (final position)xi (initial position)tf (final time)ti (initial time)\bar{v} \text{ (average velocity)} \\ \Delta x \text{ (displacement)} \\ \Delta t \text{ (time interval)} \\ x_f \text{ (final position)} \\ x_i \text{ (initial position)} \\ t_f \text{ (final time)} \\ t_i \text{ (initial time)}






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Displacement

Δx=xf−xi\Delta x=x_f-x_i


To find the change in position. Valid for any motion.

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Average Velocity

vavg=ΔxΔtv_{\text{avg}}=\frac{\Delta x}{\Delta t}



When displacement and elapsed time are known. Valid for any motion over a nonzero interval.

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