Custom Angle Bend
Routing a Waveguide Run at Any Angle
Standard waveguide catalogs stock bends at 45° and 90° because those angles cover most rectangular chassis layouts. Real systems rarely cooperate. An antenna feed may need to clear a gimbal bracket, a test fixture may route around a cryostat port, or a phased-array manifold may demand a 60° or 30° jog to keep every path length equal. A custom angle bend solves this by machining or electroforming the exact turn the geometry requires, in either the E-plane or the H-plane, so a designer is not forced to cascade two stock bends and absorb the extra length, loss, and reflection.
The engineering challenge is that any corner is an impedance discontinuity. The dominant TE10 mode wants to travel in a straight line; forcing it around a corner scatters energy into reflections and, if the corner is sharp, into higher-order modes that may propagate near the upper band edge. Two compensation strategies dominate. A radiused bend sweeps the centerline through the angle with a radius R of roughly 1.5 to 3 times the broad-wall dimension a; the gentle curve keeps the match excellent but lengthens the part. A mitered bend keeps the corner short by cutting a flat (single miter) or a pair of flats (double miter) whose depth is tuned so the reactance of the cut reflects a wave that cancels the reflection from the abrupt corner.
For the standard 90° case, miter dimensions follow well-known closed-form approximations, but custom angles fall outside those tables. Production parts are therefore optimized in a full-wave field solver, sweeping miter depth or radius until simulated VSWR meets the spec across the full band before a single chip is cut. This is why a custom bend is a design exercise, not a stock pull.
Match Compensation Geometry
Larc = R × θ (radians) = R × θdeg × π / 180
Single-miter cut depth (rule of thumb):
dmiter ≈ a × tan(θ / 2) × k, k ≈ 0.55 to 0.65
Guide wavelength (sets electrical length of the bend):
λg = λ0 / √(1 − (λ0 / 2a)2)
Where R = centerline radius, θ = turn angle, a = broad-wall width, λ0 = free-space wavelength, λg = guide wavelength, k = empirical miter factor refined in simulation. Example: WR-90 (a = 22.86 mm) 60° E-plane bend, R = 2a ≈ 45.7 mm → Larc ≈ 47.9 mm.
Bend Type and Performance Comparison
| Bend Style | Compensation | Footprint | VSWR (in-band) | Bandwidth | Best Use |
|---|---|---|---|---|---|
| Radiused E-plane | Curved centerline, R = 2 to 3a | Largest | 1.03 to 1.05:1 | Full waveguide band | Low-loss feeds, broadband |
| Radiused H-plane | Curved centerline, R = 2 to 3a | Large | 1.03 to 1.06:1 | Full waveguide band | Manifold routing |
| Single miter | One step-cut corner | Compact | 1.10 to 1.20:1 | 10 to 15% | Tight-space layouts |
| Double miter | Two tuned flats | Compact | 1.03 to 1.10:1 | 15 to 20% | Best size-to-match |
| Cascaded stock 45° | Two catalog bends | Long | 1.10 to 1.25:1 | Per part | When no custom budget |
Frequently Asked Questions
How do you keep VSWR low in a non-90-degree waveguide bend?
A radiused bend curves the centerline through the angle with R typically 1.5 to 3 times the broad wall a; a well-radiused 60° E-plane bend in WR-90 holds VSWR below 1.05:1 across 8.2 to 12.4 GHz. A mitered bend is shorter but introduces a discontinuity, so the cut depth is tuned to cancel the reflection; a double miter reaches 1.03:1 to 1.10:1 over 15 to 20% bandwidth. Custom angles are optimized in a full-wave solver because closed-form miter formulas only cover 90°.
What is the difference between an E-plane and an H-plane custom angle bend?
An E-plane bend turns in the plane of the electric field, so the bend axis is parallel to the broad wall and the narrow walls flare around the corner. An H-plane bend turns in the plane of the magnetic field, with the axis parallel to the narrow wall and the broad walls following the corner. The two perturb the TE10 field differently, so the matched-corner geometry, miter depth, and minimum radius are solved separately for each plane and are not interchangeable. The plane must be stated on every drawing because the same numeric angle yields a different physical part.
What turn angles and tolerances are achievable on a custom waveguide bend?
Almost any angle from a few degrees up to about 120° can be made as a single part; beyond that it is built as two cascaded bends. Precision millimeter-wave bends hold ±0.5° angular tolerance and ±0.25 mm flange-to-flange. Electroformed copper reaches roughly 0.4 µm Ra interior finish, keeping loss near theoretical at WR-15 and WR-10. CNC split-block aluminum is lower cost at about ±1°, suitable through Ka-band before roughness loss matters.