I was just wondering why exactly the force is the negative gradient of the potential, which is shown by the relation $${\bf F}=−{\bf∇}V$$I know that this equation only holds for conservative forces, where the potential only depends on the position of an object. The only problem I have is why there is a minus sign/ what the minus sign means in a physical context.


3 Answers 3


Well, despite the fact that the other answers are interesting, I'd prefer going directly to the "origin" of this thing, rather than its useful physical meaning.

The key idea is that

The minus sign is just a convention.

Forces do exist, and we define the potential based on them, not vice-versa.

By the way, I am commiting the mistake I hate: we are talking about potentials. But actually, the relation is

$$ \vec{F}=-\vec{\nabla}E_p$$

Where $E_p$ is the potential energy. You'll say: "that's what I wrote", yes, but we are lazy and we say "potential", but we write potential energy. I curse the person who decided to use $V$ for potential energy, when it was being used for "potential", as in Volts of electric potential. Volts $\neq$ joules, you know.

Well, sorry, back to the topic. The thing is that, the only thing we know is:

  • A Conservative force is such that the work done by it does not depend on the path.
  • But that implies that we can write work as "one function", evaluated at the final point, minus the same function evaluated at the initial point:

$$W_{cons}=\int_{\vec{x_0}}^{\vec{x_F}} \vec{F}\cdot d\vec{x}=B(\vec{x_F})-B(\vec{x_0})$$

That's the only thing we know.

And then, we decide to define a new function, called "potential energy", such that


And we do that because

$$W_{Total}=\Delta E_k$$

$$W_{total}=W_{cons}+W_{not \ cons}$$


$$\Delta E_k = W_{not\ cons}+ \Delta B$$

$$\Delta E_k - \Delta B= W_{not\ cons}$$

And that's it. We could just work with that formula. But, we prefer having a possitive quantity, so we write

$$\Delta E_k + \Delta E_p= W_{not\ cons}$$

And so, we can think of potential energy in the same way as kinetic energy, in the sense of, "the more energy, the more work".

That is the actual reason for the minus sign. But, as I said, it's just a convention. We could just work with the opposite funcion, which I called $B$.

Hope I helped.

  • $\begingroup$ Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D $\endgroup$ Nov 3, 2018 at 13:21

The gradient is a vector pointing to the direction where the change of $V$ is maximum. If a force $F$ is pointing in the direction of $-\nabla V$, it will push you in the direction where $V$ decreases the fastest. Think of a little marble placed on the edge of a bowl - it will roll down, but in which way? It can go down in a helix or just roll down to the center, and it chooses the second - why is that? Because that is the direction of fastest decrease in height (and thus gravitational potential energy). That is the physical meaning of the minus sign. If it was a plus, the ball would roll up the potential.


One of the simplest ways to look at this is in 1 dimension:


Imagine a ball in a hilly landscape. Plotting a graph of gravitational potential energy vs $x$ might look something like

enter image description here

If the ball is at position $A$, then the gradient of the potential energy with $x$ is negative, and the resulting force will be in the positive $x$-direction.

If the ball is at position $B$, then the gradient of potential energy with $x$ is positive, so the force is in the negative $x$ direction.

This overall point here is that things like to try and lower their (potential) energy if they can. This means that if in a certain direction the potential energy is going to increase, the ball is going to want to move $away$ from this, and in a direction where the ball is decreasing potential energy, until equilibrium is reached at a stationary point.


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