1. General 

2. Compound curve 

3. Reverse curve 
1. General
A multicenter curve consists of two or more backtoback curves that are tangential. The simplest consists of two curves either in the same direction (compound) or opposite directions (reverse), Figure D1.
a. Compound curve  b. Reverse curve 
Figure D1 Multicenter curves 
Multicenter curves provide greater design flexibility. For example, Figure D2 shows a typical cloverleaf freeway interchange.
Figure D2 Cloverleaf interchange 
To travel southeast, southwestbound traffic changes direction approximately 280° using the southwestern loop. This is accomplished using a flat curve for initial deceleration, followed by sharper curves for most of the direction change, and finally shallower acceleration curves. Figure D3 shows the southwestern loop with overlaid circular arcs.
Figure D3 Multiple curves 
Using a multicenter curve makes the interchange more space efficient; consider how much area would be needed for a single radius curve in this situation.
A reverse curve also provides design flexibility, particularly in tight areas.
For example, in Public Land Survey (PLS) states, northsouth Township lines were offset along Standard Parallels to account for meridian convergence, Figure D4a. Roads commonly followed Section and Township lines. At an offset Township line, a sharp left turn shortly after a sharp right turn was perfectly acceptable at horse drawn wagon speed, Figure D4b. As vehicle speeds increased, flatter curves were necessary but had to fit between the Township line segments. This could be done using a reverse curve, Figure D4c.
a. Convergence offset  b. Low speed curves  c. High speed curves 
Figure D4 Offset Township lines 
A reverse curve can also be used to work an alignment around an obstruction. Figure D5 shows what were it not for the presence of a lake would be a simple curve situation .
Figure D5 Obstruction 
Neither a long nor short radius single curve will miss the lake. However, a curve to the right could be fit to an extension of the incoming tangent followed by a curve to the left to meet the original outgoing tangent, Figure D6.
Figure D6 Working around obstruction 
If multicenter curves are so flexible, why don't we see more of them?
Primarily because of the curvature change at each curvetocurve transition.
On a simple curve, once the driver sets the steering wheel angle, it is maintained through the entire curve. A multicenter curve requires a steering wheel angle change at the beginning of each curve. Except for a reverse curve, it may not be visually apparent where one curve ends and the next begins. This makes it easy to over or undershoot successive curves.
Traveling around a circular arc introduces centrifugal force which pushes the vehicle (and its occupants) to the outside of the curve. The sharper the curve or the higher the speed, the greater the force. One way to offset this centrifugal effect is to use superelvation  pavement crossslope inclination. As a vehicle traverses differing radii curves, different superelevation rates are needed. Superelevation change should be introduced gradually or passengers may feel like they are being tossed to the side. This is more pronounced with a large radii difference from one curve to the next. On a reverse curve the condition can be worse since the crossslope direction must be changed.
Figure D7 shows a threecenter curve system with 5 section view labels.
Figure D7 Threecenter curve 
Table D1 depicts the steering wheel angle and superelevation at each section view going through the curve system.
Table D1 

Section  Steering Wheel  Superelevation 
AA  
BB  
CC  
DD  
EE 
Note that the greatest wheel angle and superelvetion occur on the third curve and must be removed entirely when the exit tangent is reached. That abrupt change could cause safety and comfort issues.
A reverse curve provides an additional chanllenge, Figure D8 and Table D2.
Figure D8 Reverse Curve 
Table D2 

Section  Steering Wheel  Superelevation 
AA  
BB  
CC  
DD 
At the point of reverse curvature, the steering angle must be changed to the other side. The superelevation also changes direction so the vehicle is "rolled" from one side to the other. Coupled with superelevation, the centrifugal force changes direction. Allinall quite a bit of stuff going on, especially when the vehicle is cruising along at a good rate.
So while multicenter curves provide greater design flexibility, they do have drawbacks. particularly in high speed situations. Except for special cases such as interchanges, their use should be limited to lower speeds with reasonable radii differences.
2. Compound curve
a. Nomenclature
Starting with two tangent lines intersecting at a PI, a compound curve is fit between them, Figure D9.
Figure D9 Compound curve 
Figure D10 shows major parts of the compound curve.
Figure D10 Compound curve parts 
The PCC (Point of Curve to Curve) is the EC of the first curve and BC of the second. A tangent line at the PCC intersects the incoming tangent at the PI_{1} and the outgoing tangent at PI_{2}.
T_{i} is the distance from the BC_{1} to the PI; T_{o} the distance from the PI to the EC_{2}.
There are seven parts to a compound curve: T_{i}, T_{o}, R_{1}, R_{2}, Δ_{1}, Δ_{2}, and Δ. Because the tangents deflect Δ at the PI and the compound curve transitions from the incoming to the outgoing tangent:
Δ = Δ_{1}+ Δ_{2}  Equation D1 
That means there are six independent parts. For a unique solution four parts must be fixed, including at least one angle and at least two distances.
Because they share a point (PCC) and tangent line, once all six parts are determined, the compound curve can be computed as two simple curves, Figure D11. Individual curve attributes can be computed using the single curve equations in Chapter C.
Figure D11 Two simple curves 
Depending on which parts are initially fixed, there are different ways to compute the remaining parts.
One way is solving the vertex triangle, Figure D12, created by the three PIs.
Figure D12 Vertex triangle 
Another method is to use a closed loop traverse through points O_{1}BC_{1}PIEC_{2}O_{2}, Figure D13.
Figure D13 Traverse method 
The direction of one line is assumed to be in a cardinal direction and the others written in terms of 90° angles and Δs. Distances are Rs and Ts. Latitudes and departures are computed, summed, are set eqaul to zero to force closure. This results in two equations in two unknowns which can then be simultaneously solved.
b. Examples
(1) Example 1
A PI is located at station 38+00.00 with a left deflection of 72°00'00"L. The compound curve begins at sta 33+50.00. The first curve has a 700.00 ft radius and 30°00'00" central angle.
Determine the radius and central angle of the second curve and the length of both curves.
Sketch:
We'll try a vertex triangle solution. Isolate the triangle and label the tangents:
Since we have the radius and central angle of the first curve, we can compute its tangent:
Compute Δ_{2} using Equation D1
Determine the distance from the PI_{1} to the PI which is a side of the triangle.
The distance between PI_{1} and PI_{2} is the sum of the curve tangents. Using the Law of Sines and the known T_{1}, we can compute T_{2}.
Using T_{2} and Δ_{2}, R_{2} can be determined.
Finally, compute each curve's length.
(2) Example 2
A PI is located at 55+69.23 with a deflection angle between tangents of 85°00'00"R. The compound curve must begin 463.64 ft before the PI and end 405.60 ft after. Central angles of the two curves are 30°00'00" and 55°00'00" respectivley.
Determine the radius of each curve,
Sketch:
Becasue we only have angles of the vertex triangle with no distances (and insufficient given data to compute any), the curve system can't be solved that way. Instead, we will use the traverse method.
To start, the curve system is rotated to make the initial radial line run North. Then using right angles and Δs, bearings of the other lines can be determined.
Updated sketch with bearings:
Compute Latitudes and Departures:
Line  Bearing  Length  Latitude  Departure 
O_{1}BC_{1}  North  R_{1}  R_{1}  0.00 
BC_{1}PI  East  463.64  0.00  463.64 
PIEC_{2}  S 5°00'00"E  405.60  405.60 x cos(5°00'00")  +405.60 x sin(5°00'00") 
EC_{2}O_{2}  S 85°00'00"W  R_{2}  R_{2} x cos(85°00'00")  R_{2} x sin(85°00'00") 
O_{2}O_{1}  S 30°00'00"W  R_{1}R_{2}  (R_{1}R_{2}) x cos(30°00'00")  (R_{1}R_{2}) x sin(30°00'00") 
Sum and reduce the Latitudes:
Sum and reduce the Departures:
We have two equatiosn with unkowns R_{1} and R_{2}. Solve them simultaneously. We'll use substitution.
Solve the Latitide summation for R_{1}
Substiute the equation for R_{1} in the Departures summation and solve R_{2}:
Solve R_{1}:
With R_{1} and R_{2} computed, we have two geometric attributes for each curve. Using Chapter C equations, their remaining attributes can be determined.
c. Stationing
As with a single curve, there are two paths to the EC from the BC. One goes up and down the original tangents, the other along the curves. Whether a station equation is used at the EC depends on how the entire alignment is stationed. Refer to the discussion in Chapter C Section 2.
Equations to compute the curves' endpoints are:
Equation D2  
Equation D3  
Equation D4  
Equation D5 
The stationing for Example (2) is:
e. Radial stakeout
Each curve's table is computed as described in Chapter C.
Following are radial chord tables for each curve in Example (2) (computations aren't shown).
Curve 1  
Sta  Defl ang  Chord  
EC  54+10.64  15º00'00"  301.58 
54+00  14º28'36"  291.29  
53+00  9º33'34"  193.51  
52+00  4º38'32"  94.31  
BC  51+05.59  0º00'00"  0.00 
Curve 2  
Sta  Defl ang  Chord  
EC  58+12.43  27º30'00"  386.54 
58+00  26º38'57"  375.47  
57+00  19º48'17"  283.63  
56+00  12º57'37"  187.77  
55+00  6º06'57"  89.109  
BC  54+10.64  0º00'00"  0.00 
Stakeout procedure
Measure T_{i} and T_{o} from the PI along the tangents to set the BC_{1} and EC_{2}.
Stake Curve 1
Setup instrument on BC_{1}.
Sight PI with 0º00'00" on the horizontal circle.
Stake curve points using the curve table.
Stake Curve 2
Setup on PCC
Sight BC_{1} with (Δ_{1}/2) = 15º00'00"=345°00'00" on the horizontal circle, Figure D14a.
Inverse the scope to sight away from the BC_{1}, Figure D14b.
Rotating right to a horizontal angle of 0º00'00" orients intrument tangent to the curves at the PCC, Figure D14c.
Stake curve points using the curve table.
Last point should match the previously set EC_{2}.
a. Sight BC_{1} with (Δ_{1}/2) reading 
b. Inverse telescope 
c. Rotate to 00°00'00" 
Figure D14 Orienting at PCC 
3. Reverse curve
a. General
A reverse curve consists of two consecutive tangent corves with radius points on opposite sides of the center line. Figure 15 shows basic nomenclature and parts.
Figure D15 Nomenclature 
The PRC is the Point of Reverse Curvature, and is the EC of the first curve and BC of the second.
The distance from PI_{1} to PI_{2} is T_{1} + T_{2}. Because of this relationship, as soon as one curve's geometry is fixed, so is the other's. This makes a reverse curve generally easier to compute than a compound curve.
Once the geometry of both curves are fixed, they can be computed as individual simple curves.
b. Stationing
Stationing can be a little confusing since there can be a station equation at both the PRC and EC of the second curve. Usually, if a stationing is maintained along the tangents, then a station equation only appears at the end of the reverse curve.
To compute stationing:
Equation D6  
Equation D7  
Equation D8  
Equation D9 
b. Example
For a reverse curve, the first PI is at 33+50.15 with a 75°20'00"L deflection angle and second PI is at 40+16.70 with a 83°50'00"R deflection angle.
The first curve has a 375.00' radius. Determine the radius of the second curve.
Sketch:
Tadaa!