How many black holes can fit on the head of a pin?

Black holes are regions of space from which nothing can escape. If you consider a spherical object of mass M and radius R and set the escape velocity from the object to be c c , the speed of light, you can determine a relationship between R and M, R = 2 G M / c 2 R=2 GM/c^2 , where G G is Newton's gravitational constant. This radius is called the Schwarzschild radius, denoted by R s R_s . If mass M is concentrated into a region with a radius smaller than R s R_s then you have a black hole, and if not, there is no black hole.

From the above relation you can determine the minimum mass of a black hole, as roughly speaking the Schwarzschild radius must be larger or equal to the Compton wavelength - the minimum size of the region in which an object at rest can be localized.

Find the minimum mass of a black hole in μ g \mu g .

Finally, a bonus thing to think about. What does this result mean for the masses of the particles that we see in nature?

Details and assumptions

  • The value of the gravitational constant is G = 6.67 × 1 0 11 m 3 /kg s 2 G=6.67 \times 10^{-11} \text{ m}^3\text{/kg s}^2 .
  • The speed of light is c = 3 × 1 0 8 m/s c=3 \times 10^8\text{ m/s} .
  • Planck's constant is h = 6.63 × 1 0 34 kgm 2 /s h=6.63 \times 10^{-34} \text{ kgm}^2\text{/s} .
  • 1 μ g = 1 0 6 g = 1 0 9 kg 1 ~\mu g = 10^{-6} \text{ g} = 10^{-9} \text{ kg}


The answer is 38.6.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

3 solutions

Saurabh Dubey
May 20, 2014

The Compton wavelength of any particle is given by, L= h m c \frac{h}{mc} where L =Compton wavelength, h =Planck's constant, m =Rest mass of the particle, and c =speed of light. Given in the question, R= 2 G m c 2 \frac {2Gm}{c^2} As stated in the problem, R \geq L For minimum mass,the radius should be minimum (as R is directly proportional to mass) i.e. R = L . Therefore, 2 G m c 2 = h m c \frac{2Gm}{c^2}=\frac{h}{mc} . Solving the above equality, we get, m= h c 2 G \sqrt {\frac {hc}{2G}} . Substituting the values of h,c and G, we find that m= 3.86 × 1 0 8 3.86 \times10^-8 kg , or 38.6 μ g \mu g .

Compton wavelength = h / (M * c) So, 2GM / c^2 >= h / (M * c) Thus, M^2 >= hc / 2G

Solving M >= 38.6 * 10^ (-9)

David Mattingly Staff
May 13, 2014

The smallest black hole must have r s = λ c r_s=\lambda_c , where λ c \lambda_c is the Compton wavelength h / m c h/mc so:

2 G m c r c 2 = h m c r c m c r = h c 2 G = 3.86 × 1 0 8 ( k g ) = 38.6 ( μ g ) \frac{2Gm_{cr}}{c^2}=\frac{h}{m_{cr}c} \Rightarrow m_{cr}=\sqrt{\frac{hc}{2G}} = 3.86 \times 10^{-8} (kg)=38.6(\mu g)

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...