User talk:Starwave - Revision history

Starwave: corrected links to pages and did minor updates

2012-09-30T13:51:29Z

corrected links to pages and did minor updates

← Older revision		Revision as of 13:51, 30 September 2012
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	== Heat switch physics in 1.106+ ==		== Heat switch physics in 1.106+ ==
	Heat switches distribute the heat of themselves, the reactor and the nearby components, until they all have the same heat compared to their respective max heat.		[[Heat Switch\|Heat switches]] distribute the heat of themselves, the reactor and the nearby components, until they all have the same heat compared to their respective max heat.

	Used Variables:		Used Variables:
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	== Heat vent physics in 1.106+ ==		== Heat vent physics in 1.106+ ==
	Heat vents are basically heat switches that additionally cool themselves down. They will however not ~~give their heat away by~~ themselves~~, you~~ have to ~~take~~ it ~~away~~ using other elements. There are 5 types of heat vents that are similar to the heat switches except for the overclocked one as it is new:		[[Heat Vent\|Heat vents]] are basically heat switches that additionally cool themselves down. They will however not take it from components themselves. You have to give it to them using other elements. There are 5 types of heat vents that are similar to the heat switches except for the overclocked one as it is new:
	Used Variables:		Used Variables:
	*Tm: max heat		*Tm: max heat

Starwave: added heat vent category and did some minor corrections

2012-09-21T19:23:57Z

added heat vent category and did some minor corrections

← Older revision		Revision as of 19:23, 21 September 2012
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	== Heat switch physics in 1.106+ ==		== Heat switch physics in 1.106+ ==

	Heat switches distribute the heat of themselves, the reactor and the nearby components, until they all have the same heat compared to their respective max heat.		Heat switches distribute the heat of themselves, the reactor and the nearby components, until they all have the same heat compared to their respective max heat.

Line 48:		Line 47:
	**Tr = 8		**Tr = 8

	*The component heat exchanger.		*The component heat exchanger, it only transfers heat between the reactor and itself.
	**Tm = 5000		**Tm = 5000
	**Ts = 36		**Ts = 36
	**Tr = 0		**Tr = 0

	*The reactor heat exchanger.		*The reactor heat exchanger, it only transfers heat between nearby components and itself.
	**Tm = 5000		**Tm = 5000
	**Ts = 0		**Ts = 0
Line 59:		Line 58:

	== Heat vent physics in 1.106+ ==		== Heat vent physics in 1.106+ ==
	~~Coming soon~~...		Heat vents are basically heat switches that additionally cool themselves down. They will however not give their heat away by themselves, you have to take it away using other elements. There are 5 types of heat vents that are similar to the heat switches except for the overclocked one as it is new:
			Used Variables:
			*Tm: max heat
			*Tr: reactor heat transfer rate
			*Tc: the self cooling rate

			The types of switches are as follows:
			*The (basic) heat vent that only vents heat it has stored.
			**Tm = 1000
			**Tr = 0
			**Tc = 6

			*The advanced heat vent which is again a better version of the basic one.
			**Tm = 1000
			**Tr = 0
			**Tc = 12

			*The overclocked heat vent which is the fastest but also gets destroyed pretty fast if it always finds heat.
			**Tm = 1000
			**Tr = 36
			**Tc = 20

			*The reactor heat vent takes the heat only out of the reactor again.
			**Tm = 1000
			**Tr = 5
			**Tc = 5

			*The component heat vent takes the heat only out of components again.
			**Special case: it removes 4 heat from every nearby component each tick and can not store heat.

	== Conclusion ==		== Conclusion ==

Starwave: added heat switch category

2012-09-21T18:38:55Z

added heat switch category

← Older revision		Revision as of 18:38, 21 September 2012
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	== Uranium physics in 1.106+ ==		== Uranium physics in 1.106+ ==
	Used variables:		Used variables:
	*n: Nearby uranium cells		*n: Nearby uranium cells (by "nearby" I mean one slot horizontally or vertically)
	*p: Amount of pulses this reactor tick		*p: Amount of pulses this reactor tick
	*h: Heat produced this reactor tick		*h: Heat produced this reactor tick
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	== Coolant physics in 1.106+ ==		== Coolant physics in 1.106+ ==
	~~There are 2 types~~ of ~~coolant capacitors~~:		As uranium reactions produce heat and coolant is what you need to not let your reactor melt. In order to do so you can use one of these:
	*The coolant cell. There are 3 types of it which can store up to 10K, 30K or 60K heat and you can get that heat out again. Be careful tough, as it will break when being heated beyond the max heat value.		*The coolant cell. There are 3 types of coolant cells which can store up to 10K, 30K or 60K heat and you can get that heat out again. Be careful tough, as it will break when being heated beyond the max heat value.
	*The condensator. There are 2 types of the condensator, the RSH (20K) and the LZH (100K). They are pretty much coolant cells but can store more heat, will not break when reaching their heat cap but you can still get the heat out again.		*The condensator. There are 2 types of the condensator, the RSH (20K) and the LZH (100K). They are pretty much coolant cells but can store more heat, will not break when reaching their heat cap but you can still get the heat out again.
	Additionally you can "repair" them using redstone (and lapis for the LZH). Redstone fills up a RSH by 10K a LZH by 5K and lapis fills a LZH by 40K.		Additionally you can "repair" them using redstone (and lapis for the LZH). Redstone fills up a RSH by 10K a LZH by 5K and lapis fills a LZH by 40K.
			If you want to heat the reactor instead, you can use a heating cell. They stack to 64 and heat every adjacent component by stack size until it reaches stack size 1000.

	== Heat switch physics in 1.106+ ==		== Heat switch physics in 1.106+ ==
	~~Coming soon~~...
			Heat switches distribute the heat of themselves, the reactor and the nearby components, until they all have the same heat compared to their respective max heat.

			Used Variables:
			*Tm: max heat
			*Ts: side heat transfer rate
			*Tr: reactor heat transfer rate

			There are 4 types of heat switches or heat exchangers:
			*The (normal) heat exchanger.
			**Tm = 2500
			**Ts = 12
			**Tr = 4

			*The advanced heat exchanger, which is just the upgraded version of the normal one.
			**Tm = 10000
			**Ts = 24
			**Tr = 8

			*The component heat exchanger.
			**Tm = 5000
			**Ts = 36
			**Tr = 0

			*The reactor heat exchanger.
			**Tm = 5000
			**Ts = 0
			**Tr = 72

	== Heat vent physics in 1.106+ ==		== Heat vent physics in 1.106+ ==
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	***4 / 60 / 25		***4 / 60 / 25

	** Dual uranium cell: (n / h / e)		**Dual uranium cell: (n / h / e)
	***0 / 24 / 20		***0 / 24 / 20
	***1 / 48 / 30		***1 / 48 / 30
Line 53:		Line 81:
	***4 / 168 / 60		***4 / 168 / 60

	** Quad uranium cell: (n / h / e)		**Quad uranium cell: (n / h / e)
	***0 / 96 / 60		***0 / 96 / 60
	***1 / 160 / 80		***1 / 160 / 80
Line 62:		Line 90:

	If you need help with reactor calculation, don't understand parts of this formula or find a mistake, please contact me.		If you need help with reactor calculation, don't understand parts of this formula or find a mistake, please contact me.
			Note: Yes I have actually found everything out myself except for some basic things that Alblaka wrote [http://forum.industrial-craft.net/index.php?page=Thread&threadID=7659.com here] (for the copyright stuff).

Starwave: added Coolant physics category

2012-09-21T18:02:30Z

added Coolant physics category

← Older revision		Revision as of 18:02, 21 September 2012
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	== Coolant physics in 1.106+ ==		== Coolant physics in 1.106+ ==
	~~Coming soon~~...		There are 2 types of coolant capacitors:
			*The coolant cell. There are 3 types of it which can store up to 10K, 30K or 60K heat and you can get that heat out again. Be careful tough, as it will break when being heated beyond the max heat value.
			*The condensator. There are 2 types of the condensator, the RSH (20K) and the LZH (100K). They are pretty much coolant cells but can store more heat, will not break when reaching their heat cap but you can still get the heat out again.
			Additionally you can "repair" them using redstone (and lapis for the LZH). Redstone fills up a RSH by 10K a LZH by 5K and lapis fills a LZH by 40K.

	== Heat switch physics in 1.106+ ==		== Heat switch physics in 1.106+ ==

Starwave: made the page prettier

2012-09-21T16:56:25Z

made the page prettier

← Older revision		Revision as of 16:56, 21 September 2012
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	== Conclusion ==		== Conclusion ==
	*Uranium cells:		*Uranium cells:
	*h = 2 c * (1 + floor(c / 2) + n) * (2 + floor(c / 2) + n)		**Basic Formulas:
	*e = 5 c * (1 + floor(c / 2) + n)		**h = 2 c * (1 + floor(c / 2) + n) * (2 + floor(c / 2) + n)
			**e = 5 c * (1 + floor(c / 2) + n)

	** Single uranium cell: (n / h / e)		**Single uranium cell: (n / h / e)
	***0 / 4 / 5		***0 / 4 / 5
	***1 / 12 / 10		***1 / 12 / 10

Starwave at 16:55, 21 September 2012

2012-09-21T16:55:07Z

← Older revision		Revision as of 16:55, 21 September 2012
Line 35:		Line 35:
	*e = 5 c * (1 + floor(c / 2) + n)		*e = 5 c * (1 + floor(c / 2) + n)

	**Single uranium cell: (n / h / e)		** Single uranium cell: (n / h / e)
	***0 / 4 / 5		***0 / 4 / 5
	***1 / 12 / 10		***1 / 12 / 10
Line 42:		Line 42:
	***4 / 60 / 25		***4 / 60 / 25

	**Dual uranium cell: (n / h / e)		** Dual uranium cell: (n / h / e)
	***0 / 24 / 20		***0 / 24 / 20
	***1 / 48 / 30		***1 / 48 / 30
Line 49:		Line 49:
	***4 / 168 / 60		***4 / 168 / 60

	**Quad uranium cell: (n / h / e)		** Quad uranium cell: (n / h / e)
	***0 / 96 / 60		***0 / 96 / 60
	***1 / 160 / 80		***1 / 160 / 80

Starwave: Created page with "== Uranium physics in 1.106+ == Used variables: n: Nearby uranium cells p: Amount of pulses this reactor tick h: Heat produced this reactor tick e: Energy produced this re..."

2012-09-21T16:54:06Z

Created page with "== Uranium physics in 1.106+ == Used variables: *n: Nearby uranium cells *p: Amount of pulses this reactor tick *h: Heat produced this reactor tick *e: Energy produced this re..."

New page

== Uranium physics in 1.106+ ==
Used variables:
*n: Nearby uranium cells
*p: Amount of pulses this reactor tick
*h: Heat produced this reactor tick
*e: Energy produced this reactor tick
*c: Amount of cells in this item

A uranium cell will always pulse once plus the amount of cells that are directly adjacent (and contain uranium):
*p = 1 + n

Addition: To compensate dual and quad cells you should use:
*p = 1 + floor(c / 2) + n

A uranium cell will always create heat and energy based on how often it ticks per reactor tick:
*h = 2 * p * (p + 1)
*e = 5 * p

Addition: To compensate dual and quad cells you should use:
*h = 2 * c * p * (p + 1)
*e = 5 * c * p

== Coolant physics in 1.106+ ==
Coming soon...

== Heat switch physics in 1.106+ ==
Coming soon...

== Heat vent physics in 1.106+ ==
Coming soon...

== Conclusion ==
*Uranium cells:
**h = 2 * c * (1 + floor(c / 2) + n) * (2 + floor(c / 2) + n)
**e = 5 * c * (1 + floor(c / 2) + n)

**Single uranium cell: (n / h / e)
***0 / 4 / 5
***1 / 12 / 10
***2 / 24 / 15
***3 / 40 / 20
***4 / 60 / 25

**Dual uranium cell: (n / h / e)
***0 / 24 / 20
***1 / 48 / 30
***2 / 80 / 40
***3 / 120 / 50
***4 / 168 / 60

**Quad uranium cell: (n / h / e)
***0 / 96 / 60
***1 / 160 / 80
***2 / 240 / 100
***3 / 336 / 120
***4 / 448 / 140

If you need help with reactor calculation, don't understand parts of this formula or find a mistake, please contact me.