Difference between revisions of "Tutorial:Whats with all the math?"

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{{underlinked|July 2014}}
 
{{underlinked|July 2014}}
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{{delete|Page has not been edited since 2016 and is obsoleted by [[Terminology]]}}
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=KSP math explained for the rest of us=
 
=KSP math explained for the rest of us=
I started playing KSP a few months ago. I tried to understand what everybody was talking about when they mentioned TWR, ISP, Δv, apoapsis, eccentricity, and a whole bunch of other terms from math and physics. The learning curve is high, but this tutorial will try to explain what all these different numbers mean and why they are important for people who do not have a mathematical background.
+
I started playing KSP a few months ago. I tried to understand what everybody was talking about when they mentioned [[Thrust-to-weight ratio|TWR]], [[Specific impulse|ISP]], Δv, [[Orbit#Apoapsis|apoapsis]], [[Orbit#Eccentricity|eccentricity]], and a whole bunch of other terms from math and physics. The learning curve is high, but this tutorial will try to explain what all these different numbers mean and why they are important for people who do not have a mathematical background.
 
==A few words about physics==
 
==A few words about physics==
Many parts of orbital mechanics can be counter-intuitive for people. Most of us have not been to space, so our intuition about how things should work is based  on how we experience them. Historically, this was actually a major sticking point in [[Wikipedia:physics|physics]] because we had to think in ways that were different from our intuition to really understand how planets moved. Here we will explain a few basic physics concepts, although interested readers are encouraged to research the work of [[Wikipedia:Isaac Newton|Isaac Newton]] and the development of these ideas. It should be noted that these explanations are not entirely rigorous, and simply meant to give people an intuitive understanding of how things work.
+
Many parts of orbital mechanics can be counter-intuitive for people. Most of us have not been to space, so our intuition about how things should work is based  on how we experience them. Historically, this was actually a major sticking point in [[Wikipedia:physics|physics]] because we had to think in ways that were different from our intuition to really understand how planets moved. Here we will explain a few basic physics concepts, although interested readers are encouraged to research the work of [[Wikipedia:Isaac Newton|Isaac Newton]] and the development of these ideas. It should be noted that these explanations are not entirely rigorous and are simply meant to give people an intuitive understanding of how things work.
 
===Velocity, Speed, Friction, and Acceleration===
 
===Velocity, Speed, Friction, and Acceleration===
 
Say you are driving down the street at 70 miles per hour (about 113 kilometers per hour). If you were to turn put your car's engine in neutral, your car would slow to a stop. Our intuition says that if we want to keep moving the same speed, we need to keep pushing the gas pedal, or we will slow down. The reason we think this is that all our experiences involve [[Wikipedia:friction|friction]]. In the car example, there is air friction on the surface of the car and friction from the wheels on the ground. Friction can be thought of as pushing us backwards, while the gas pedal pushes us forwards. If we stop the engine, friction continues to push us backwards, which is why we stop.  
 
Say you are driving down the street at 70 miles per hour (about 113 kilometers per hour). If you were to turn put your car's engine in neutral, your car would slow to a stop. Our intuition says that if we want to keep moving the same speed, we need to keep pushing the gas pedal, or we will slow down. The reason we think this is that all our experiences involve [[Wikipedia:friction|friction]]. In the car example, there is air friction on the surface of the car and friction from the wheels on the ground. Friction can be thought of as pushing us backwards, while the gas pedal pushes us forwards. If we stop the engine, friction continues to push us backwards, which is why we stop.  
 
In space, there is no friction. Therefore, there is nothing pushing us backwards. Imagine you are in space, and there are no planets or stars or anything but you. If you are moving, you will keep moving in a straight line forever. This comes from one of [[Wikipedia:Newton's laws of motion|Newton's laws of motion]], that an object in motion stays in motion and an object at rest stays at rest unless acted upon by a [[Wikipedia:force|force]]. On earth, friction is a force that pushes us backwards, and the gas pedal applies a force that pushes us forwards. A force is basically just a 'push.'
 
In space, there is no friction. Therefore, there is nothing pushing us backwards. Imagine you are in space, and there are no planets or stars or anything but you. If you are moving, you will keep moving in a straight line forever. This comes from one of [[Wikipedia:Newton's laws of motion|Newton's laws of motion]], that an object in motion stays in motion and an object at rest stays at rest unless acted upon by a [[Wikipedia:force|force]]. On earth, friction is a force that pushes us backwards, and the gas pedal applies a force that pushes us forwards. A force is basically just a 'push.'
 
When we say velocity, we mean the speed you are moving in, and the direction you are moving in. Therefore, if your speed stays the same but you are turning, then your velocity is changing. Think about making a 90-degree turn in a car, you have to push the gas pedal down during the turn. Acceleration is nothing more than a change in velocity. Therefore in physics, when we say that something is accelerating,  either it's speed is changing, the direction it is moving is changing, or both.
 
When we say velocity, we mean the speed you are moving in, and the direction you are moving in. Therefore, if your speed stays the same but you are turning, then your velocity is changing. Think about making a 90-degree turn in a car, you have to push the gas pedal down during the turn. Acceleration is nothing more than a change in velocity. Therefore in physics, when we say that something is accelerating,  either it's speed is changing, the direction it is moving is changing, or both.
Note for the interested readers: There is an important mathematical relationship between position, velocity, and acceleration. In fact, the exploration of this relationship by [[Wikipedia:Isaac Newton|Isaac Newton]] and [[Wikipedia:Gottfried Leibniz|Gottfried Leibniz]] lead to the invention of what we math people now call [[Wikipedia:Calculus|Calculus]].
+
====Side-note for interested and advanced readers====
 +
There is an important mathematical relationship between position, velocity, and acceleration. In fact, the exploration of this relationship by [[Wikipedia:Isaac Newton|Isaac Newton]] and [[Wikipedia:Gottfried Leibniz|Gottfried Leibniz]] lead to the invention of what we math people now call [[Wikipedia:Calculus|Calculus]].
  
 
==Orbital Mechanics==
 
==Orbital Mechanics==
 
{{See also|Orbit}}
 
{{See also|Orbit}}
+
 
 
Since we are trying to play Kerbal Space Program, we will spend a significant amount of time dealing with orbit. To help us think about being in orbit, we will first describe a 'thought experiment', although I would encourage anybody to go outside and give this a try. Imagine you tie a baseball to one end of a string. Now imagine you hold the other end of the string and spin around in a circle very quickly. The ball will 'orbit' around you. When your spacecraft orbits a planet or moon in KSP, the gravity pulls you in like the string keeps the ball near you.  
 
Since we are trying to play Kerbal Space Program, we will spend a significant amount of time dealing with orbit. To help us think about being in orbit, we will first describe a 'thought experiment', although I would encourage anybody to go outside and give this a try. Imagine you tie a baseball to one end of a string. Now imagine you hold the other end of the string and spin around in a circle very quickly. The ball will 'orbit' around you. When your spacecraft orbits a planet or moon in KSP, the gravity pulls you in like the string keeps the ball near you.  
 
If you are in a circular orbit, your speed will not change (note that since you are always turning, you are actually always accelerating). The planet is pulling you straight down, but you are already moving fast enough away from the planet that you move in a circle. You are actually in free-fall, but you are moving so fast that you miss the planet every time. Readers are encouraged to convince themselves of this, it is easier to see in a highly eccentric orbit than in a circular orbit, more on that later.
 
If you are in a circular orbit, your speed will not change (note that since you are always turning, you are actually always accelerating). The planet is pulling you straight down, but you are already moving fast enough away from the planet that you move in a circle. You are actually in free-fall, but you are moving so fast that you miss the planet every time. Readers are encouraged to convince themselves of this, it is easier to see in a highly eccentric orbit than in a circular orbit, more on that later.
 
In KSP, as long as you are in a well behaved orbit (not on an escape trajectory, not going to crash into the surface, completely above the atmosphere), your orbit will never change. You will keep moving in the same path forever. In the real world, it's not quite that simple, but that is outside the scope of this explanation.
 
In KSP, as long as you are in a well behaved orbit (not on an escape trajectory, not going to crash into the surface, completely above the atmosphere), your orbit will never change. You will keep moving in the same path forever. In the real world, it's not quite that simple, but that is outside the scope of this explanation.
 +
 
===Orbital Velocity===
 
===Orbital Velocity===
 
[[File:Simple orbit diagram.svg|thumb|upright=3.0]]
 
[[File:Simple orbit diagram.svg|thumb|upright=3.0]]
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===Eccentricity===
 
===Eccentricity===
[[Eccentricity]] is a number to describe the 'shape' of our orbit. The closer our eccentricity is to 0, the more circular our orbit is. Elliptical orbits have eccentricity somewhere between 0 and 1. In the image to the right, the smaller, circular orbit would have an eccentricity of 0, and the larger orbit would have eccentricity around 1/2 (very rough number). Eccentricity of 1 or greater is what we call a parabolic or hyperbolic orbit. All that means is that you will not stay in orbit, you will escape the planet's sphere of influence and never come back without accelerating back towards it somehow.
+
[[Orbit#Eccentricity|Eccentricity]] is a number to describe the 'shape' of our orbit. The closer our eccentricity is to 0, the more circular our orbit is. Elliptical orbits have eccentricity somewhere between 0 and 1. In the image to the right, the smaller, circular orbit would have an eccentricity of 0, and the larger orbit would have eccentricity around 1/2 (very rough number). Eccentricity of 1 or greater is what we call a parabolic or hyperbolic orbit. All that means is that you will not stay in orbit, you will escape the planet's sphere of influence and never come back without accelerating back towards it somehow.
 
+
====Side-note for interested and advanced readers====
 +
The circle, ellipse, parabola, and hyperbola are all [[Wikipedia:Conic section|conics]]. A troubling problem then becomes modeling [[Wikipedia:Precession#Perihelion precession| perihelion precessions]] whose orbits don't end and start at the same place.
 
===Maneuvers===
 
===Maneuvers===
 
{{See also|Basic maneuvers}}
 
{{See also|Basic maneuvers}}
 +
 
Say we are at point A in the figure to the right, and we point the nose of our rocket in the direction of the arrow ([[prograde]], the direction we are moving) and burn our engines for a while. In reality, this burn takes a certain amount of time, and our position changes during that time. However, that is some much more complicated math, so we are going to pretend that the burn starts and ends instantly. Basically, we pretend that we '''accelerate''' by a certain amount at point A. Since we are still at point A, when we complete one orbital period, we will be back at point A. However, the opposite side of our orbit will move away from us, making our orbit more eccentric in this case. The important take-away here is that we '''accelerate''' at point A to change our '''velocity'''. This changes the shape of our orbit. Say our original velocity was 10,000 m/s (10 kilometers per second), and our new speed is 10,200 m/s. Our velocity changed by 200 m/s, and this is our Δv!  
 
Say we are at point A in the figure to the right, and we point the nose of our rocket in the direction of the arrow ([[prograde]], the direction we are moving) and burn our engines for a while. In reality, this burn takes a certain amount of time, and our position changes during that time. However, that is some much more complicated math, so we are going to pretend that the burn starts and ends instantly. Basically, we pretend that we '''accelerate''' by a certain amount at point A. Since we are still at point A, when we complete one orbital period, we will be back at point A. However, the opposite side of our orbit will move away from us, making our orbit more eccentric in this case. The important take-away here is that we '''accelerate''' at point A to change our '''velocity'''. This changes the shape of our orbit. Say our original velocity was 10,000 m/s (10 kilometers per second), and our new speed is 10,200 m/s. Our velocity changed by 200 m/s, and this is our Δv!  
  
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==Why is Δv so important?==
 
==Why is Δv so important?==
At this point, we have a rough idea of what Δv is, and Δv is probably the most important thing to understand. Note that above, when we talked about how fast our rocket was moving, or how it's orbit changed, we said nothing about the mass of the rocket. We don't know if we are talking about a tiny satellite, a spaceplane, or a huge rocket, but we know that how our orbit changes is only dependent on how our velocity changes! This is why we talk about Δv so much, because no matter what rocket you build, it takes the same amount of Δv to go from point A to point B in space. Furthermore, we know it takes about 4600 Δv to get into orbit around Kerbin, so if we know the Δv our ascent stage generates, we know if it will get us to space!
+
Note that above, when we talked about how fast our rocket was moving, or how it's orbit changed, we said nothing about the mass of the rocket. We don't know if we are talking about a tiny satellite, a spaceplane, or a huge rocket, but we know that how our orbit changes is only dependent on how our velocity changes! This is why we talk about Δv so much, because no matter what rocket you build, it takes the same amount of Δv to go from point A to point B in space. Furthermore, we know it takes about 4600 Δv to get into orbit around Kerbin, so if we know the Δv our ascent stage generates, we know if it will get us to space! This is why Δv is probably the most important thing to understand.
  
 
==Determining Δv==
 
==Determining Δv==
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===Thrust and Thrust-to-Weight Ratio(TWR)===
 
===Thrust and Thrust-to-Weight Ratio(TWR)===
 
{{See also|Thrust-to-weight ratio}}
 
{{See also|Thrust-to-weight ratio}}
Thrust is the amount of force (how much 'push') your engine is generating. Remember the example of the car going down the road where the engine pushes the car forward and friction pushes the car backwards? The same thing happens with rockets. Thrust is basically how hard the rocket is being pushed up from the surface of [[Kerbin]].
+
 
 +
Thrust is the amount of force (how much 'push') your engine is generating. Recall the car metaphor where the car is going down the road, the engine pushes the car forward, and friction pushes the car backwards. Thrust is basically how hard the rocket is being pushed up from the surface of [[Kerbin]].  
  
 
We all know that heavy things are harder to pick up than lighter things. If you don't believe me, go lift a piece of paper off the ground over your head, and then do the same with a piece of furniture, like a couch. The couch is much harder to pick up. The same thing is true in rocket science, heavier rockets are harder to pick up (lift off) than lighter rockets! This is why TWR is so important, the rocket's engines are pushing the rocket up, and gravity is pushing the rocket back down. If you have ever arm-wrestled, you know that the person who pushes harder is going to win. The rocket's weight is how hard gravity is pushing down. Therefore, the rocket's thrust must push harder than gravity, or you are not going to space. A TWR less than one means that gravity is going to win. A TWR over one means the rocket is going to win, and a TWR of exactly one means the rocket will hover in place. However, once you are in a stable obit, you no longer need a TWR over one to change your velocity.
 
We all know that heavy things are harder to pick up than lighter things. If you don't believe me, go lift a piece of paper off the ground over your head, and then do the same with a piece of furniture, like a couch. The couch is much harder to pick up. The same thing is true in rocket science, heavier rockets are harder to pick up (lift off) than lighter rockets! This is why TWR is so important, the rocket's engines are pushing the rocket up, and gravity is pushing the rocket back down. If you have ever arm-wrestled, you know that the person who pushes harder is going to win. The rocket's weight is how hard gravity is pushing down. Therefore, the rocket's thrust must push harder than gravity, or you are not going to space. A TWR less than one means that gravity is going to win. A TWR over one means the rocket is going to win, and a TWR of exactly one means the rocket will hover in place. However, once you are in a stable obit, you no longer need a TWR over one to change your velocity.
Line 50: Line 57:
 
===So, what engine should my rocket use, and what is engine ISP?===
 
===So, what engine should my rocket use, and what is engine ISP?===
 
{{See also|Specific impulse}}
 
{{See also|Specific impulse}}
Let's start with engine ISP. Basically, it tells you how fuel-efficient your engine is. An engine with a higher ISP will give you more Δv for the same amount of fuel as an engine with lower ISP. However, it is important to keep in mind the thrust different engines generate and strike a balance between ISP, which determines Δv, and thrust, which effects TWR. Put in different terms, the choice is between how much your spacecraft accelerates and how fast your spacecraft accelerates.
+
Let's start with engine ISP. Basically, it tells you how fuel-efficient your engine is. An engine with a higher ISP will give you more Δv for the same amount of fuel as an engine with lower ISP. However, it is important to keep in mind the thrust different engines generate and strike a balance between ISP, which determines Δv, and thrust, which affects TWR. Put in different terms, the choice is between how much your spacecraft accelerates and how fast your spacecraft accelerates.
  
 
====Example====
 
====Example====
The [[LV-909 Liquid Fuel Engine]] engine has ISP of 300 in atmosphere or 390 in space. The [[Rockomax "Mainsail" Liquid Engine]] has ISP of 320 in atmosphere or 360 in space. This doesn't seem like much of a difference. However, the mainsail can generate a thrust of 1500, while the LV-909 can only generate a thrust of 50. Therefore, the LV-909 will accelerate your rocket more slowly. Sometimes, you need to generate a lot of thrust very quickly (like when you are trying to go from the ground to orbit), so an engine with lower ISP but higher thrust may be better.
+
The [[LV-909 Liquid Fuel Engine]] engine has ISP of 85 s at 1 atmosphere (atm) and 345 s in the vacuum of space. The [[Rockomax "Mainsail" Liquid Engine]] has ISP of 285 s at 1 atm and 310 s in space. This doesn't seem like much of a difference. However, the mainsail can generate a thrust of 1379.03 kN at 1 atm and 1500.00 kN in vacuum, while the LV-909 can only generate a thrust of 14.78 kN at 1 atm and 60.00 kN in space. Therefore, the LV-909 will accelerate your rocket more slowly. Sometimes, you need to generate a lot of thrust very quickly (like when you are trying to go from the ground to orbit), so an engine with lower ISP but higher thrust may be better.
  
 
==What about SRBs?==
 
==What about SRBs?==

Latest revision as of 02:16, 7 August 2020

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KSP math explained for the rest of us

I started playing KSP a few months ago. I tried to understand what everybody was talking about when they mentioned TWR, ISP, Δv, apoapsis, eccentricity, and a whole bunch of other terms from math and physics. The learning curve is high, but this tutorial will try to explain what all these different numbers mean and why they are important for people who do not have a mathematical background.

A few words about physics

Many parts of orbital mechanics can be counter-intuitive for people. Most of us have not been to space, so our intuition about how things should work is based on how we experience them. Historically, this was actually a major sticking point in physics because we had to think in ways that were different from our intuition to really understand how planets moved. Here we will explain a few basic physics concepts, although interested readers are encouraged to research the work of Isaac Newton and the development of these ideas. It should be noted that these explanations are not entirely rigorous and are simply meant to give people an intuitive understanding of how things work.

Velocity, Speed, Friction, and Acceleration

Say you are driving down the street at 70 miles per hour (about 113 kilometers per hour). If you were to turn put your car's engine in neutral, your car would slow to a stop. Our intuition says that if we want to keep moving the same speed, we need to keep pushing the gas pedal, or we will slow down. The reason we think this is that all our experiences involve friction. In the car example, there is air friction on the surface of the car and friction from the wheels on the ground. Friction can be thought of as pushing us backwards, while the gas pedal pushes us forwards. If we stop the engine, friction continues to push us backwards, which is why we stop. In space, there is no friction. Therefore, there is nothing pushing us backwards. Imagine you are in space, and there are no planets or stars or anything but you. If you are moving, you will keep moving in a straight line forever. This comes from one of Newton's laws of motion, that an object in motion stays in motion and an object at rest stays at rest unless acted upon by a force. On earth, friction is a force that pushes us backwards, and the gas pedal applies a force that pushes us forwards. A force is basically just a 'push.' When we say velocity, we mean the speed you are moving in, and the direction you are moving in. Therefore, if your speed stays the same but you are turning, then your velocity is changing. Think about making a 90-degree turn in a car, you have to push the gas pedal down during the turn. Acceleration is nothing more than a change in velocity. Therefore in physics, when we say that something is accelerating, either it's speed is changing, the direction it is moving is changing, or both.

Side-note for interested and advanced readers

There is an important mathematical relationship between position, velocity, and acceleration. In fact, the exploration of this relationship by Isaac Newton and Gottfried Leibniz lead to the invention of what we math people now call Calculus.

Orbital Mechanics

→ See also: Orbit

Since we are trying to play Kerbal Space Program, we will spend a significant amount of time dealing with orbit. To help us think about being in orbit, we will first describe a 'thought experiment', although I would encourage anybody to go outside and give this a try. Imagine you tie a baseball to one end of a string. Now imagine you hold the other end of the string and spin around in a circle very quickly. The ball will 'orbit' around you. When your spacecraft orbits a planet or moon in KSP, the gravity pulls you in like the string keeps the ball near you. If you are in a circular orbit, your speed will not change (note that since you are always turning, you are actually always accelerating). The planet is pulling you straight down, but you are already moving fast enough away from the planet that you move in a circle. You are actually in free-fall, but you are moving so fast that you miss the planet every time. Readers are encouraged to convince themselves of this, it is easier to see in a highly eccentric orbit than in a circular orbit, more on that later. In KSP, as long as you are in a well behaved orbit (not on an escape trajectory, not going to crash into the surface, completely above the atmosphere), your orbit will never change. You will keep moving in the same path forever. In the real world, it's not quite that simple, but that is outside the scope of this explanation.

Orbital Velocity

Simple orbit diagram.svg

Given a fixed, stable orbit, your velocity (the speed you are moving and direction you are moving in) depends only on your position in that orbit. Understanding this is incredibly important, so here is some explanation. In the image to the right, look at any point on the bigger shape (the ellipse). If you don't burn your engines, your speed when you are at that point will be the same as when you return to that point after one orbital period (the amount of time your orbit takes to complete one full revolution).

Eccentricity

Eccentricity is a number to describe the 'shape' of our orbit. The closer our eccentricity is to 0, the more circular our orbit is. Elliptical orbits have eccentricity somewhere between 0 and 1. In the image to the right, the smaller, circular orbit would have an eccentricity of 0, and the larger orbit would have eccentricity around 1/2 (very rough number). Eccentricity of 1 or greater is what we call a parabolic or hyperbolic orbit. All that means is that you will not stay in orbit, you will escape the planet's sphere of influence and never come back without accelerating back towards it somehow.

Side-note for interested and advanced readers

The circle, ellipse, parabola, and hyperbola are all conics. A troubling problem then becomes modeling perihelion precessions whose orbits don't end and start at the same place.

Maneuvers

→ See also: Basic maneuvers

Say we are at point A in the figure to the right, and we point the nose of our rocket in the direction of the arrow (prograde, the direction we are moving) and burn our engines for a while. In reality, this burn takes a certain amount of time, and our position changes during that time. However, that is some much more complicated math, so we are going to pretend that the burn starts and ends instantly. Basically, we pretend that we accelerate by a certain amount at point A. Since we are still at point A, when we complete one orbital period, we will be back at point A. However, the opposite side of our orbit will move away from us, making our orbit more eccentric in this case. The important take-away here is that we accelerate at point A to change our velocity. This changes the shape of our orbit. Say our original velocity was 10,000 m/s (10 kilometers per second), and our new speed is 10,200 m/s. Our velocity changed by 200 m/s, and this is our Δv!

What does all this mean?

Okay, by now if you are still reading, you are probably starting to think "How does all this stuff help me go to space!?" Well, we are going to start talking about that right now!

Why is Δv so important?

Note that above, when we talked about how fast our rocket was moving, or how it's orbit changed, we said nothing about the mass of the rocket. We don't know if we are talking about a tiny satellite, a spaceplane, or a huge rocket, but we know that how our orbit changes is only dependent on how our velocity changes! This is why we talk about Δv so much, because no matter what rocket you build, it takes the same amount of Δv to go from point A to point B in space. Furthermore, we know it takes about 4600 Δv to get into orbit around Kerbin, so if we know the Δv our ascent stage generates, we know if it will get us to space! This is why Δv is probably the most important thing to understand.

Determining Δv

Since this is an article for people without mathematical backgrounds, we are not going to look at the formula for calculating Δv. There are great tutorials explaining the equations for all of this, and readers are encouraged to consult them for a more rigorous understanding. However, most people see big, complicated equations and they stop reading, whether it comes from some post-traumatic stress left over from school, or being generally uninterested in mathematics, and that is okay. Here, we are going to simply look at what Δv depends on, that is, what effect does building a rocket in one way or another impact Δv?

There are mods that will tell you what your stage's Δv is, and I personally use one of them, but since this article is about vanilla KSP we will leave them out of this discussion. There are also mods that will do your entire take-off, gravity turn, and all your orbital maneuvers for you. While these can be fun, I personally do not believe in using them outside of sandbox mode for experimental purposes, since the point of playing the game is learning for me.

Thrust and Thrust-to-Weight Ratio(TWR)

→ See also: Thrust-to-weight ratio

Thrust is the amount of force (how much 'push') your engine is generating. Recall the car metaphor where the car is going down the road, the engine pushes the car forward, and friction pushes the car backwards. Thrust is basically how hard the rocket is being pushed up from the surface of Kerbin.

We all know that heavy things are harder to pick up than lighter things. If you don't believe me, go lift a piece of paper off the ground over your head, and then do the same with a piece of furniture, like a couch. The couch is much harder to pick up. The same thing is true in rocket science, heavier rockets are harder to pick up (lift off) than lighter rockets! This is why TWR is so important, the rocket's engines are pushing the rocket up, and gravity is pushing the rocket back down. If you have ever arm-wrestled, you know that the person who pushes harder is going to win. The rocket's weight is how hard gravity is pushing down. Therefore, the rocket's thrust must push harder than gravity, or you are not going to space. A TWR less than one means that gravity is going to win. A TWR over one means the rocket is going to win, and a TWR of exactly one means the rocket will hover in place. However, once you are in a stable obit, you no longer need a TWR over one to change your velocity.

Side-note for interested and advanced readers

TWR changes during the flight of a rocket. As you burn more fuel, you lose mass, and your TWR increases since your weight decreases. TWR also depends on what planet/moon you are on since each celestial body has different gravity. Therefore, the same rocket with the same amount of fuel as a lower TWR on Eve than it does on Kerbin.

So, what engine should my rocket use, and what is engine ISP?

→ See also: Specific impulse

Let's start with engine ISP. Basically, it tells you how fuel-efficient your engine is. An engine with a higher ISP will give you more Δv for the same amount of fuel as an engine with lower ISP. However, it is important to keep in mind the thrust different engines generate and strike a balance between ISP, which determines Δv, and thrust, which affects TWR. Put in different terms, the choice is between how much your spacecraft accelerates and how fast your spacecraft accelerates.

Example

The LV-909 Liquid Fuel Engine engine has ISP of 85 s at 1 atmosphere (atm) and 345 s in the vacuum of space. The Rockomax "Mainsail" Liquid Engine has ISP of 285 s at 1 atm and 310 s in space. This doesn't seem like much of a difference. However, the mainsail can generate a thrust of 1379.03 kN at 1 atm and 1500.00 kN in vacuum, while the LV-909 can only generate a thrust of 14.78 kN at 1 atm and 60.00 kN in space. Therefore, the LV-909 will accelerate your rocket more slowly. Sometimes, you need to generate a lot of thrust very quickly (like when you are trying to go from the ground to orbit), so an engine with lower ISP but higher thrust may be better.

What about SRBs?

→ See also: SRB

My first ship to successfully orbit Minmus had around 50 SRB's on it. I do not recommend this approach. First off, as of .24, we have to pay for parts, so efficiency is important. Second, it was very difficult to get enough struts on the ship to get it to stay in one piece. Third, it was very difficult to steer, so my gravity turn was very inefficient. I only mention this because a common part of the learning curve for new players is to add more SRB's and more struts when we have trouble reaching orbit.

SRB's add a good amount of thrust, but also add weight. Therefore, the more you add, the less of a benefit you are getting. Also, since they only have one setting, which is to burn until empty, they are best used for ascent stages only, since we need more control when we are in space. Therefore, my recommendation is that if you are having trouble getting into orbit, putting a few SRB's on the side of your rocket as a first stage may help. As you unlock more parts in career mode, and get a better feel for getting into orbit, you may or may not continue to use them.

Final Notes

Hopefully this tutorial has given you a decent primer on what all the math really means. I highly recommend experimenting with different rocket designs, reading more rigorous mathematical explanations, and continuing to learn, since this is just a baseline to get you started.