Static Balancing of a Payload

by Bill Claybaugh, Reaction Research Society


Dislocations in the Center-of-Gravity (Cg) of a rocket with respect to the vehicle centerline can lead to “coning” in flight.  This coning is visually characterized by a corkscrew exhaust trail when it occurs during thrusting. Whenever it occurs—and it is likely in all rockets that are not axisymmetrically balanced—it increases drag and lowers performance.  In cases of “extreme” unbalance (which can occur for axial offsets of Cg of as little as a few tens of thousandths of an inch for small diameter rockets) the vehicle can be torn apart in flight by the aerodynamic forces created by the Cg imbalance.

For rockets that are carefully designed to be axisymmetric, the only important issue to address in assuring balance of the rocket is to make certain that the fins all have the same weight within a small margin (removing mass from the heavier fins is best done at the fin Cg).  If all other components are axisymmetric—including the propellant grain—then the only part of the vehicle that will require formal balancing is the payload:

I Longitudinal Balancing

The image below shows the set up for longitudinal balancing of a payload:

Dual-weight scales with precisely placed mounring locations

Two identical scales are slightly modified to support the payload so that the longitudinal axis is parallel with the base of the scales and level.

After carefully measuring the distance between the centers of the two scales (6.760” in this example) the weight of the payload supported by each scale is noted in two orthogonal planes.  Using a moment balance calculation, the center of gravity is determined in each plane:

Averaging three measurements in plane 1, the scales showed 6.953 lbsm on the left side and 4.523 lbsm on the right scale.  Creating an arbitrary starting datum for calculation that is 0.7125” to the right of the right scale center point (that is, at the bottom of the payload base plate) allows the following center of mass balance:

Cg = (4.487 lbsm * 0.7125 in.) + (6.967 lbsm * 7.4725 in.) / (4.487 lbsm + 6.967lbsm)

​​​​= 4.824” from the datum.

Rotating the payload by 90 degrees and weighing again allows calculating the Center of Gravity in that plane, in this case, that value was:

​​​Gg = 4.881” from the datum.

Thus, the Cg appears—on average—to be offset by 0.057” between the two planes.

Balancing: Subtractive and Additive

Balance can be achieved either by subtracting weight from the top of and in the plane that shows the longer Cg distance (Plane 2, in this case) or by adding weight to the top of the plane that has the shorter Cg.  Conversely, weight could be added at some bottom location of Plane 2 or deducted from a bottom location on Plane 1. Note that any of these actions have effects on the rotational balance, which we will address in a future article.

Subtractive Balancing

We can estimate the amount of weight that needs to be deducted from the firstplane by deciding that the weight will be removed at 9.375” from the datum (a location at the top of the conical aluminum section, just below the fiberglass structure that supports the flight computer / transmitter in the image).

The mass required to move the Cg by 0.057” is then:

Mass Lost (or Gained) / New Total Mass = Change in Cg / Distance to New Mass

Adjustment Mass / (11.451 – Adjustment Mass) = .057 / (9.375” – 4.881”)

Adjustment Mass = 0.142 lbsm

This mass must be removed at equidistant locations from the rotational axis, that is, we will require two 0.071 lbsm axisymmetric holes in opposite sides of the payload at the required location.

We can estimate the drill depth assuming the use of a mill cutter.  The required cutting depth is then the cross-sectional area of the mill times the drill depth times the density of aluminum:

​​Mass to be removed = 0.098 lbsm. / cu. in. * (pi * r^2) * h

For a 0.5” mill cutter that depth is:

​​​0.071 = 0.098 * 3.1416 * (0.5 / 2)^2 * h 

​​​​​h = 3.69”

Obviously, this is impractical as the depth of aluminum at the subject location is only 0.125”.

Additive Balancing

The relatively large cutting operation required for subtractive balancing is due to the low density of aluminum.  Alternatively, we can estimate the additional mass required in the shorter of the two planes (Plane 1). Because we can use, for example, tungsten for the weight adjustment, it is possible to move the shorter Cgforward with much smaller but higher density balance weights.

Adding mass at a greater distance from the Cg will lower the mass required to achieve the needed shift.  If we consider adding mass at a location 13.375” from the datum location (on the cross bar near the top of the fiberglass structure that supports the flight computer / transmitter) we can calculate:

Adjustment Mass / (11.454 + Adjustment Mass) = .057 / (13.375” – 4.824”)

Adjustment Mass = 0.0763 lbsm

Noting that one-half of this is 0.03815 lbsm or 17.3 grams, we can observe that a standard tungsten weight used in “pinewood derby” cars of 0.25” diameter and 0.5” length weighs about 14 grams. Thus, drilling two axisymmetric holes at the required location and gluing the tungsten counterweights in place will produce a Gg offset close to the 0.057” adjustment required (see the comments below on the resolution of this system for locating the Cg).  Note that the two balance weights, in final form, need to weigh the same within a small margin or they will introduce a mass imbalance in rotation. We should also note that we are not here accounting for the mass removed to make the holes for the counterweights.

Verification

The final step is to remeasure the Cg in both planes and verify that they are within the resolution of the measurement system.  If not, another, smaller, adjustment in mass in the longer plane or an adjustment of the balance weight in the shorter plane may be required.

A Note on Accuracy

The relativity low cost scales used in this example resolve weight to 0.10 grams. However, multiple measurement in the same plane (achieved by gently pressing on the payload to reset the scales) shows that the scales are in fact accurate to about +/- 10 grams, about 0.3% of the total weight of the subject payload.

This means that the true resolution of this system with regard to differences in Cg between planes is about 0.015”, thus, once the Cg between the planes is within 0.15”, further adjustment is unlikely to increase accuracy using these relatively low-cost scales.


MTA work event, 2023-03-03

Dimitri Timohovich, RRS.ORG


Last weekend saw a big dent put into the bathroom project. On Friday, 3/3/23, I was able to install the 2 remaining pass-throughs, one for the water to enter the container and one to serve as part of the shower drainage.

Clean cut window and a look from the inside
Supply header pass-through in place.

I was able to also attach the main drainage line to the outside drainage line and set up to connect the shower drainage to the main line.

Saturday, 3/4/23, started out with nice weather and I was able to connect the water line from the pass through and run it to the pump area.  More PEX lines were run and a manifold was made for a bypass incase of pump failure.  Final attachments will need to be made.

Dave showed up just in time for the wind to pick up.  Meanwhile, I started to tie in the electrical and build a small control box with a main switch and voltmeter.  Unfortunately, Dave couldn’t stay long and after lunch I went back to more electrical work.  Meanwhile, the weather kept getting worse.  

Sunday, 3/5/23, was cold, very windy, and with scattered showers, so I packed up early and headed back to town.

Next event is coming soon. Progress and next steps to be discussed at the March 10th monthly meeting.

New plumbing feedthroughs
Voltmeter installed for checking battery health.

We are getting close to having the restroom become operational. We hope the weather continues to be favorable.


MTA work and launch event, 2023-02-19

by Dimitri Timohovich, RRS.ORG


The RRS met at the Mojave Test Area from Sunday, February 19, through Tuesday, February 21st, primarily to continue working on the restroom. We also got a launch or two off on Sunday thanks to Keith Yoerg.

Returning rocket to the MTA courtesy of favorable winds

Here is a basic recap of what was done and what needs to be finished to get the bathroom up to working order.

On Sunday, 2/19/2023, Keith and I installed 5 of the 6 unistrut segments on top of the Dosa building. The last piece was accidentally left behind and will be installed on the next trip out. Dave Nordling assisted with installing the lighting in both bathrooms which were tested. 4-hour mechanical timer switches were used to avoid wasting power.

Dave Nordling also cleared brush in the western part of the MTA property that day.

Mechanical timer switches used in both restrooms.
Dual LED panels from recreational vehicles provide excellent low-power lighting.
Good quality light from just two panels.

On Monday, 2/20/2023, I welded and installed the four-inch sewage drain passthrough and attached the sewage drain line to the passthrough. I started welding the other two passthroughs.

On Tuesday, 2/21/2023, I continued welding passthroughs until the wind came up and had to stop. From there, I continued installing the water intake line on top of the container and continued hooking up Pex pipes inside the container.

What’s next will be finishing the 4-inch drain line and starting the 2-inch drain line in the ground. The 2-inch passthrough must be welded in to the container wall. Attachment of the intake water line to it’s passthrough will follow, then attaching the water line from passthrough to water pump. We must also finish attaching the water lines from the pump to all fixtures.

We will temporarily attach the water pump to battery power and test the lines. This will get the bathroom to interim working status which is a major goal of the project. The date of the next work event is not known at this time but will be coming very soon.