WOLFRAM|DEMONSTRATIONS PROJECT

Properties of Kerr Spacetime

​
a
0.5
specific radii
​
static limit
r
0
θ =
π
2
​
=
2.
event horizon
r
+
=
1.86603
inner horizon
r
-
=
0.133975
marginally stable orbits
​
rotation
=
4.233
counter-rotation
=
7.55458
photon orbits
​
direct
=
2.3473
retrograde
=
3.53209
​
Kerr spacetime describes a rotating black hole. The line element in Boyer–Lindquist coordinates
(t,r,θ,ϕ)
is given by
d
2
s
=-1-
2Mr
Σ
d
2
t
-
4Mar
2
sin
θ
Σ
dtdϕ+
Σ
Δ
d
2
r
+Σd
2
θ
+
2
r
+
2
a
+
2M
2
a
r
2
sin
θ
Σ
2
sin
θd
2
ϕ
with
Δ=
2
r
-2Mr+
2
a
and
Σ=
2
r
+
2
a
2
cos
θ
.
M
is the mass of the black hole and
a
is the angular momentum.
The roots of the function
Δ
define the event horizon
r
+
and the inner horizon
r
-
, where
r
±
=M±
2
M
-
2
a
. The region between the event horizon and the static limit
r
0
=M+
2
M
-
2
a
2
cos
θ
is called the ergosphere.
The two marginally stable timelike circular geodesics are defined by the radii
r
ms
=M3+
Z
2
∓
(3-
Z
1
)(3+
Z
1
+2
Z
2
)

, where
Z
1
=1+
1/3
1-
2
a
2
M
1/3
1+
a
M
+
1/3
1-
a
M
and
Z
2
=
3
2
a
2
M
+
2
Z
1
. An object on the smaller radius rotates with the Kerr black hole, whereas an object on the larger radius rotates in the opposite direction.
The direct (-) and retrograde (+) photon orbits are defined via
r
po±
=2M1+cos
2
3
arccos
∓a
M
.
Here, the mass of the black hole is taken as
M=1
.