vanhees71 said:
It is simply impossible to teach physics without calculus. It's even impossible to talk about physics adequately without calculus. It's thus simply a flawed concept to think that one can teach physics in a "calculus free" way.
As someone who has taught introductory algebra-based physics (Mechanics, E&M and "Modern" Physics) several times at the university level, I disagree. Admittedly, I had initial doubts whether it could be done properly without calculus. However after doing it, my doubts evaporated and now I have become an apologist for algebra-based physics.
My clientele consisted of undergraduate students at a U.S. university who were pursuing degrees in the health and biosciences: medicine, biology, biochemistry, physical therapy, sports medicine, radiation technology, etc. Their curricula required them to take two semesters of introductory physics taught in a physics department and had no room for calculus. I set my apprehensions aside because It was clear to me from the start that if I did not teach algebra-based physics to these students, I would not be doing my job. Furthermore, if I taught algebra-based physics badly, I would be doing my job badly. Therefore, I had to teach introductory physics without calculus and do it well.
Take any calculus-based introductory physics textbook and carefully examine how much calculus is in it and whether it is really necessary. Yes, the mathematical description is more compact and elegant with calculus. Yes, it is necessary for students to see calculus introduced at the beginning of their study of physics, but only if they are headed towards a career related to physics and/or engineering. Most of the examples and problems in calculus-based introductory textbooks are artificial physical situations in which polynomials with constant coefficients are given as hypothetical models for a dependent variable and one is asked to find related variables using integration or differentiation. There is little physical understanding gained by the calculus formulation in such problems.
After the second semester, my students were not going to see any more formal physics instruction. However, they were going to see the application of physical models in their professional courses. The primary goal I defined for them was understanding the physical world in terms of predictive mathematical models that they could manipulate within their mathematical abilities. So I worked around the calculus barrier. Necessity is the mother of invention and here are some examples of what I did.
Considering kinematics, my students had to understand motion and acceleration, so that they could understand ##F_{net}=ma##, so that they could understand rotational dynamics and equilibrium, so that they could understand the parameters that come into play when they put patients in traction. No calculus needed for that.
I defined acceleration as "the speed of the speed", that is acceleration is a measure of how fast the speed is changing much like speed is a measure of how fast position is changing. This gave students an intuitive understanding of acceleration as a rate of change by relying on their existing perception of speed as a rate of change. I did not integrate ##~~\dfrac{d^2x}{dt^2}=a~~## to get ##v(t)## and ##x(t)## for motion under constant acceleration. Instead, I used the idea that the change in velocity (##v-v_0##) is the "area under the ##a## vs. ##t## curve" and that the change in position (##x-x_0##) is the "area under the ##v## vs. ##t## curve".
There were few instances in which I taught by writing expressions down rather than deriving them. A notable failure was my attempt at deriving the inverse ##r## potential from the inverse ##r^2## force in a way that would not glaze over the eyes of my audience. However, I was able to bring the essence of Maxwell's equations to the algebra-based class. This is what I did with Gauss's law, which is a no-no in its differential form and still a no-no in its integral form. I carried the integral form one more step over to the average form: $$\begin{align} & \int_S\mathbf{E}\cdot \mathbf{\hat n}~dA=\frac{q_{enc.}}{\epsilon_0} \nonumber \\
& \langle E_n\rangle_S=\frac{\int_S\mathbf{E}\cdot \mathbf{\hat n}~dA}{\int_S dA}= \frac{q_{enc.}}{\epsilon_0 S}. \nonumber \\
\end{align}$$In the expression ##~\langle E_n\rangle_S~## is the normal component of the electric field averaged over a closed surface ##S##. It is proportional to the charge enclosed by the surface and inversely proportional to the surface area ##S##. It can be written down as an experimental result without justification just like the differential and integral forms. It can be used to find the electric field on a surface in cases of high symmetry when the normal component of electric field anywhere on the surface is the same. In that case, the average electric field is the same as the average an idea for which students understand intuitively: when the entire class receives 100% on a test, the average test grade is 100%. One can then list the three cases of high symmetry and the expression for ##S## that accompanies them: ##S=4\pi r^2~## (sphere); ##S=2\pi rL~## (cylinder); ##S=2A~## (pillbox).
The remaining Maxwell's equations can be cast in similar forms. Ampere's law for example (without the displacement current) would be $$\langle B_t\rangle_C=\frac{\mu_0 I_{enc.}}{C}$$for the tangential component of the magnetic field averaged over a closed contour ##C##. This post is already longer than originally planned so I will leave the formulation of the remaining two Maxwell's equations in average form as an exercise to the reader. Yes, the equations in this form cannot be used to derive the wave equation and whole lot of other stuff, but the underpinnings of classical E&M can be conveyed to the audience in an easy to understand form.
Finally, I will mention in passing the derivation of Snell's law using Fermat's principle presented without calculus in an
earlier post.
In summary, I hope that I have convinced the reader that meaningful physics can be taught without calculus snd reach people who do not plan to pursue careers that require understanding of how physicists have modeled the physical world. Where there is a will there is a way.